- 21 Sections
- 1012 Lessons
- 32 Weeks
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- Course Related InformationImportant Information Related To The Courses, Live Classes, Zoom Links etc.3
- Notes + Written Material For Contents of The SyllabusNotes for Chapters + Written Resources Regarding The Content157
- 3.1Motion In A Circle: Kinematics Of Uniform Circular Motion: Define The Radian And Express Angular Displacement In Radians
- 3.2Motion In A Circle: Kinematics Of Uniform Circular Motion: Understand And Use The Concept Of Angular Speed
- 3.3Motion In A Circle: Kinematics Of Uniform Circular Motion: Recall And Use Ω = 2π/t And V = Rω
- 3.4Motion In A Circle: Centripetal Acceleration: Understand That A Force Of Constant Magnitude That Is Always Perpendicular To The Direction Of Motion Causes Centripetal Acceleration
- 3.5Motion In A Circle: Centripetal Acceleration: Understand That Centripetal Acceleration Causes Circular Motion With A Constant Angular Speed
- 3.6Motion In A Circle: Centripetal Acceleration: Recall And Use A = Rω2 And A = V2 /r
- 3.7Motion In A Circle: Centripetal Acceleration: Recall And Use F = Mrω2 And F = Mv2 /r
- 3.8Gravitational Fields: Gravitational Field: Understand That A Gravitational Field Is An Example Of A Field Of Force And Define Gravitational Field As Force Per Unit Mass
- 3.9Gravitational Fields: Gravitational Field: Represent A Gravitational Field By Means Of Field Lines
- 3.10Gravitational Fields: Gravitational Force Between Point Masses: Understand That, For A Point Outside A Uniform Sphere, The Mass Of The Sphere May Be Considered To Be A Point Mass At Its Centre
- 3.11Gravitational Fields: Gravitational Force Between Point Masses: Recall And Use Newton’s Law Of Gravitation F = Gm1m2 /r 2 For The Force Between Two Point Masses
- 3.12Gravitational Fields: Gravitational Force Between Point Masses: Analyse Circular Orbits In Gravitational Fields By Relating The Gravitational Force To The Centripetal Acceleration It Causes
- 3.13Gravitational Fields: Gravitational Force Between Point Masses: Understand That A Satellite In A Geostationary Orbit Remains At The Same Point Above The Earth’s Surface, With An Orbital Period Of 24 Hours, Orbiting From West To East, Directly Above The Equator
- 3.14Gravitational Fields: Gravitational Field Of A Point Mass: Derive, From Newton’s Law Of Gravitation And The Definition Of Gravitational Field, The Equation G = Gm/r 2 For The Gravitational Field Strength Due To A Point Mass
- 3.15Gravitational Fields: Gravitational Field Of A Point Mass: Recall And Use G = Gm/r 2
- 3.16Gravitational Fields: Gravitational Field Of A Point Mass: Understand Why G Is Approximately Constant For Small Changes In Height Near The Earth’s Surface
- 3.17Gravitational Fields: Gravitational Potential: Define Gravitational Potential At A Point As The Work Done Per Unit Mass In Bringing A Small Test Mass From Infinity To The Point
- 3.18Gravitational Fields: Gravitational Potential: Use Φ = –gm/r For The Gravitational Potential In The Field Due To A Point Mass
- 3.19Gravitational Fields: Gravitational Potential: Understand How The Concept Of Gravitational Potential Leads To The Gravitational Potential Energy Of Two Point Masses And Use Ep = –gmm/r
- 3.20Temperature: Thermal Equilibrium: Understand That (Thermal) Energy Is Transferred From A Region Of Higher Temperature To A Region Of Lower Temperature
- 3.21Temperature: Thermal Equilibrium: Understand That Regions Of Equal Temperature Are In Thermal Equilibrium
- 3.22Temperature: Temperature Scales: Understand That A Physical Property That Varies With Temperature May Be Used For The Measurement Of Temperature And State Examples Of Such Properties, Including The Density Of A Liquid, Volume Of A Gas At Constant Pressure, Resistance Of A Metal, E.m.f. Of A Thermocouple
- 3.23Temperature: Temperature Scales: Understand That The Scale Of Thermodynamic Temperature Does Not Depend On The Property Of Any Particular Substance
- 3.24Temperature: Temperature Scales: Convert Temperatures Between Kelvin And Degrees Celsius And Recall That T/k = Θ/ °c + 273.15
- 3.25Temperature: Temperature Scales: Understand That The Lowest Possible Temperature Is Zero Kelvin On The Thermodynamic Temperature Scale And That This Is Known As Absolute Zero
- 3.26Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Heat Capacity
- 3.27Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Latent Heat And Distinguish Between Specific Latent Heat Of Fusion And Specific Latent Heat Of Vaporisation
- 3.28Ideal Gases: The Mole: Understand That Amount Of Substance Is An Si Base Quantity With The Base Unit Mol
- 3.29Ideal Gases: The Mole: Use Molar Quantities Where One Mole Of Any Substance Is The Amount Containing A Number Of Particles Of That Substance Equal To The Avogadro Constant Na
- 3.30Ideal Gases: Equation Of State: Understand That A Gas Obeying Pv ∝ T, Where T Is The Thermodynamic Temperature, Is Known As An Ideal Gas
- 3.31Ideal Gases: Equation Of State: Recall And Use The Equation Of State For An Ideal Gas Expressed As Pv = Nrt, Where N = Amount Of Substance (Number Of Moles) And As Pv = Nkt, Where N = Number Of Molecules
- 3.32Ideal Gases: Equation Of State: Recall That The Boltzmann Constant K Is Given By K = R/na
- 3.33Ideal Gases: Kinetic Theory Of Gases: State The Basic Assumptions Of The Kinetic Theory Of Gases
- 3.34Ideal Gases: Kinetic Theory Of Gases: Explain How Molecular Movement Causes The Pressure Exerted By A Gas And Derive And Use The Relationship Pv = 3 1 Nm, Where Is The Mean-square Speed (A Simple Model Considering One-dimensional Collisions And Then Extending To Three Dimensions Using 3 1 = Is Sufficient)
- 3.35Ideal Gases: Kinetic Theory Of Gases: Understand That The Root-mean-square Speed Cr.m.s. Is Given By C 2
- 3.36Ideal Gases: Kinetic Theory Of Gases: Compare Pv = 3 1 Nm With Pv = Nkt To Deduce That The Average Translational Kinetic Energy Of A Molecule Is 2 3 Kt, And Recall And Use This Expression
- 3.37Thermodynamics: Internal Energy: Understand That Internal Energy Is Determined By The State Of The System And That It Can Be Expressed As The Sum Of A Random Distribution Of Kinetic And Potential Energies Associated With The Molecules Of A System
- 3.38Thermodynamics: Internal Energy: Relate A Rise In Temperature Of An Object To An Increase In Its Internal Energy
- 3.39Thermodynamics: The First Law Of Thermodynamics: Recall And Use W = P∆v For The Work Done When The Volume Of A Gas Changes At Constant Pressure And Understand The Difference Between The Work Done By The Gas And The Work Done On The Gas
- 3.40Thermodynamics: The First Law Of Thermodynamics: Recall And Use The First Law Of Thermodynamics ∆u = Q + W Expressed In Terms Of The Increase In Internal Energy, The Heating Of The System (Energy Transferred To The System By Heating) And The Work Done On The System
- 3.41Oscillations: Simple Harmonic Oscillations: Understand And Use The Terms Displacement, Amplitude, Period, Frequency, Angular Frequency And Phase Difference In The Context Of Oscillations, And Express The Period In Terms Of Both Frequency And Angular Frequency
- 3.42Oscillations: Simple Harmonic Oscillations: Understand That Simple Harmonic Motion Occurs When Acceleration Is Proportional To Displacement From A Fixed Point And In The Opposite Direction
- 3.43Oscillations: Simple Harmonic Oscillations: Use A = –ω2 X And Recall And Use, As A Solution To This Equation, X = X0 Sin Ωt
- 3.44Oscillations: Simple Harmonic Oscillations: Use The Equations V = V0 Cos Ωt And V = ±ω ( ) X X 0 2 2 −
- 3.45Oscillations: Simple Harmonic Oscillations: Analyse And Interpret Graphical Representations Of The Variations Of Displacement, Velocity And Acceleration For Simple Harmonic Motion
- 3.46Oscillations: Energy In Simple Harmonic Motion: Describe The Interchange Between Kinetic And Potential Energy During Simple Harmonic Motion
- 3.47Oscillations: Energy In Simple Harmonic Motion: Recall And Use E = 2 1 Mω2 X0 2 For The Total Energy Of A System Undergoing Simple Harmonic Motion
- 3.48Oscillations: Damped And Forced Oscillations, Resonance: Understand That A Resistive Force Acting On An Oscillating System Causes Damping
- 3.49Oscillations: Damped And Forced Oscillations, Resonance: Understand And Use The Terms Light, Critical And Heavy Damping And Sketch Displacement–time Graphs Illustrating These Types Of Damping
- 3.50Oscillations: Damped And Forced Oscillations, Resonance: Understand That Resonance Involves A Maximum Amplitude Of Oscillations And That This Occurs When An Oscillating System Is Forced To Oscillate At Its Natural Frequency
- 3.51Electric Fields: Electric Fields And Field Lines: Understand That An Electric Field Is An Example Of A Field Of Force And Define Electric Field As Force Per Unit Positive Charge
- 3.52Electric Fields: Electric Fields And Field Lines: Recall And Use F = Qe For The Force On A Charge In An Electric Field
- 3.53Electric Fields: Electric Fields And Field Lines: Represent An Electric Field By Means Of Field Lines
- 3.54Electric Fields: Uniform Electric Fields: Recall And Use E = ∆v/∆d To Calculate The Field Strength Of The Uniform Field Between Charged Parallel Plates
- 3.55Electric Fields: Uniform Electric Fields: Describe The Effect Of A Uniform Electric Field On The Motion Of Charged Particles
- 3.56Electric Fields: Electric Force Between Point Charges: Understand That, For A Point Outside A Spherical Conductor, The Charge On The Sphere May Be Considered To Be A Point Charge At Its Centre
- 3.57Electric Fields: Electric Force Between Point Charges: Recall And Use Coulomb’s Law F = Q1q2 /(4πε0r 2 ) For The Force Between Two Point Charges In Free Space
- 3.58Electric Fields: Electric Field Of A Point Charge: Recall And Use E = Q/(4πε0r 2 ) For The Electric Field Strength Due To A Point Charge In Free Space
- 3.59Electric Fields: Electric Potential: Define Electric Potential At A Point As The Work Done Per Unit Positive Charge In Bringing A Small Test Charge From Infinity To The Point
- 3.60Electric Fields: Electric Potential: Recall And Use The Fact That The Electric Field At A Point Is Equal To The Negative Of Potential Gradient At That Point
- 3.61Electric Fields: Electric Potential: Use V = Q/(4πε0r) For The Electric Potential In The Field Due To A Point Charge
- 3.62Electric Fields: Electric Potential: Understand How The Concept Of Electric Potential Leads To The Electric Potential Energy Of Two Point Charges And Use Ep = Qq/(4πε0r)
- 3.63Capacitance: Capacitors And Capacitance: Define Capacitance, As Applied To Both Isolated Spherical Conductors And To Parallel Plate Capacitors
- 3.64Capacitance: Capacitors And Capacitance: Recall And Use C = Q/v
- 3.65Capacitance: Capacitors And Capacitance: v
- 3.66Capacitance: Capacitors And Capacitance: Use The Capacitance Formulae For Capacitors In Series And In Parallel
- 3.67Capacitance: Energy Stored In A Capacitor: Determine The Electric Potential Energy Stored In A Capacitor From The Area Under The Potential–charge Graph
- 3.68Capacitance: Energy Stored In A Capacitor: Recall And Use W = 2 1 Qv = 2 1 Cv2
- 3.69Capacitance: Discharging A Capacitor: Analyse Graphs Of The Variation With Time Of Potential Difference, Charge And Current For A Capacitor Discharging Through A Resistor
- 3.70Capacitance: Discharging A Capacitor:Recall And Use Τ = Rc For The Time Constant For A Capacitor Discharging Through A Resistor
- 3.71Capacitance: Discharging A Capacitor: Use Equations Of The Form X = X0 E–(T/rc) Where X Could Represent Current, Charge Or Potential Difference For A Capacitor Discharging Through A Resistor
- 3.72Magnetic Fields: Concept Of A Magnetic Field: Understand That A Magnetic Field Is An Example Of A Field Of Force Produced Either By Moving Charges Or By Permanent Magnets
- 3.73Magnetic Fields: Concept Of A Magnetic Field: Represent A Magnetic Field By Field Lines
- 3.74Magnetic Fields: Force On A Current-carrying Conductor: Understand That A Force Might Act On A Current-carrying Conductor Placed In A Magnetic Field
- 3.75Magnetic Fields: Force On A Current-carrying Conductor: Recall And Use The Equation F = Bil Sin Θ, With Directions As Interpreted By Fleming’s Left-hand Rule
- 3.76Magnetic Fields: Force On A Current-carrying Conductor: Define Magnetic Flux Density As The Force Acting Per Unit Current Per Unit Length On A Wire Placed At Rightangles To The Magnetic Field
- 3.77Magnetic Fields: Force On A Moving Charge: Determine The Direction Of The Force On A Charge Moving In A Magnetic Field
- 3.78Magnetic Fields: Force On A Moving Charge: Recall And Use F = Bqv Sin Θ
- 3.79Magnetic Fields: Force On A Moving Charge: Understand The Origin Of The Hall Voltage And Derive And Use The Expression Vh = Bi /(Ntq), Where T = Thickness
- 3.80Magnetic Fields: Force On A Moving Charge: Understand The Use Of A Hall Probe To Measure Magnetic Flux Density
- 3.81Magnetic Fields: Force On A Moving Charge: Describe The Motion Of A Charged Particle Moving In A Uniform Magnetic Field Perpendicular To The Direction Of Motion Of The Particle
- 3.82Magnetic Fields: Force On A Moving Charge: Explain How Electric And Magnetic Fields Can Be Used In Velocity Selection
- 3.83Magnetic Fields: Magnetic Fields Due To Currents: Sketch Magnetic Field Patterns Due To The Currents In A Long Straight Wire, A Flat Circular Coil And A Long Solenoid
- 3.84Magnetic Fields: Magnetic Fields Due To Currents: Understand That The Magnetic Field Due To The Current In A Solenoid Is Increased By A Ferrous Core
- 3.85Magnetic Fields: Magnetic Fields Due To Currents: Explain The Origin Of The Forces Between Current-carrying Conductors And Determine The Direction Of The Forces
- 3.86Magnetic Fields: Electromagnetic Induction: Define Magnetic Flux As The Product Of The Magnetic Flux Density And The Cross-sectional Area Perpendicular To The Direction Of The Magnetic Flux Density
- 3.87Magnetic Fields: Electromagnetic Induction: Recall And Use Φ = Ba
- 3.88Magnetic Fields: Electromagnetic Induction: Understand And Use The Concept Of Magnetic Flux Linkage
- 3.89Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That A Changing Magnetic Flux Can Induce An E.m.f. In A Circuit
- 3.90Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That The Induced E.m.f. Is In Such A Direction As To Oppose The Change Producing It
- 3.91Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: The Factors Affecting The Magnitude Of The Induced E.m.f.
- 3.92Magnetic Fields: Electromagnetic Induction: Recall And Use Faraday’s And Lenz’s Laws Of Electromagnetic Induction
- 3.93Alternating Currents: Characteristics Of Alternating Currents: Understand And Use The Terms Period, Frequency And Peak Value As Applied To An Alternating Current Or Voltage
- 3.94Alternating Currents: Characteristics Of Alternating Currents: Use Equations Of The Form X = X0 Sin Ωt Representing A Sinusoidally Alternating Current Or Voltage
- 3.95Alternating Currents: Characteristics Of Alternating Currents: Recall And Use The Fact That The Mean Power In A Resistive Load Is Half The Maximum Power For A Sinusoidal Alternating Current
- 3.96Alternating Currents: Characteristics Of Alternating Currents: Distinguish Between Root-mean-square (R.m.s.) And Peak Values And Recall And Use I R.m.s. = I0 / 2 And Vr.m.s. = V0 / 2 For A Sinusoidal Alternating Current
- 3.97Alternating Currents: Rectification And Smoothing: Distinguish Graphically Between Half-wave And Full-wave Rectification
- 3.98Alternating Currents: Rectification And Smoothing: Explain The Use Of A Single Diode For The Half-wave Rectification Of An Alternating Current
- 3.99Alternating Currents: Rectification And Smoothing: Explain The Use Of Four Diodes (Bridge Rectifier) For The Full-wave Rectification Of An Alternating Current
- 3.100Alternating Currents: Rectification And Smoothing: Analyse The Effect Of A Single Capacitor In Smoothing, Including The Effect Of The Values Of Capacitance And The Load Resistance
- 3.101Quantum Physics: Energy And Momentum Of A Photon: Understand That Electromagnetic Radiation Has A Particulate Nature
- 3.102Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Is A Quantum Of Electromagnetic Energy
- 3.103Quantum Physics: Energy And Momentum Of A Photon: Recall And Use E = Hf
- 3.104Quantum Physics: Energy And Momentum Of A Photon: Use The Electronvolt (Ev) As A Unit Of Energy
- 3.105Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Has Momentum And That The Momentum Is Given By P = E/c
- 3.106Quantum Physics: Photoelectric Effect: Understand That Photoelectrons May Be Emitted From A Metal Surface When It Is Illuminated By Electromagnetic Radiation
- 3.107Quantum Physics: Photoelectric Effect: Understand And Use The Terms Threshold Frequency And Threshold Wavelength
- 3.108Quantum Physics: Photoelectric Effect: Explain Photoelectric Emission In Terms Of Photon Energy And Work Function Energy
- 3.109Quantum Physics: Photoelectric Effect: Recall And Use Hf = Φ + 2 1 Mvmax 2
- 3.110Quantum Physics: Photoelectric Effect: Explain Why The Maximum Kinetic Energy Of Photoelectrons Is Independent Of Intensity, Whereas The Photoelectric Current Is Proportional To Intensity
- 3.111Quantum Physics: Wave-particle Duality: Understand That The Photoelectric Effect Provides Evidence For A Particulate Nature Of Electromagnetic Radiation While Phenomena Such As Interference And Diffraction Provide Evidence For A Wave Nature
- 3.112Quantum Physics: Wave-particle Duality: Describe And Interpret Qualitatively The Evidence Provided By Electron Diffraction For The Wave Nature Of Particles
- 3.113Quantum Physics: Wave-particle Duality: Understand The De Broglie Wavelength As The Wavelength Associated With A Moving Particle
- 3.114Quantum Physics: Wave-particle Duality: Recall And Use Λ = H/p
- 3.115Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand That There Are Discrete Electron Energy Levels In Isolated Atoms (E.g. Atomic Hydrogen)
- 3.116Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand The Appearance And Formation Of Emission And Absorption Line Spectra
- 3.117Quantum Physics: Energy Levels In Atoms And Line Spectra: Recall And Use Hf = E1 – E2
- 3.118Nuclear Physics: Mass Defect And Nuclear Binding Energy: Understand The Equivalence Between Energy And Mass As Represented By E = Mc2 And Recall And Use This Equation
- 3.119Nuclear Physics: Mass Defect And Nuclear Binding Energy: Represent Simple Nuclear Reactions By Nuclear Equations Of The Form 7n He O H 14 2 4 8 17 1 1 + + “
- 3.120Nuclear Physics: Mass Defect And Nuclear Binding Energy: Define And Use The Terms Mass Defect And Binding Energy
- 3.121Nuclear Physics: Mass Defect And Nuclear Binding Energy: Sketch The Variation Of Binding Energy Per Nucleon With Nucleon Number
- 3.122Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain What Is Meant By Nuclear Fusion And Nuclear Fission
- 3.123Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain The Relevance Of Binding Energy Per Nucleon To Nuclear Reactions, Including Nuclear Fusion And Nuclear Fission
- 3.124Nuclear Physics: Mass Defect And Nuclear Binding Energy: Calculate The Energy Released In Nuclear Reactions Using E = C2 ∆m
- 3.125Nuclear Physics: Radioactive Decay: Understand That Fluctuations In Count Rate Provide Evidence For The Random Nature Of Radioactive Decay
- 3.126Nuclear Physics: Radioactive Decay: Understand That Radioactive Decay Is Both Spontaneous And Random
- 3.127Nuclear Physics: Radioactive Decay: Define Activity And Decay Constant, And Recall And Use A = Λn
- 3.128Nuclear Physics: Radioactive Decay: Define Half-life
- 3.129Nuclear Physics: Radioactive Decay: Use Λ = 0.693/t 2 1
- 3.130Nuclear Physics: Radioactive Decay: Understand The Exponential Nature Of Radioactive Decay, And Sketch And Use The Relationship X = X0e–λt , Where X Could Represent Activity, Number Of Undecayed Nuclei Or Received Count Rate
- 3.131Medical Physics: Production And Use Of Ultrasound: Understand That A Piezo-electric Crystal Changes Shape When A P.d. Is Applied Across It And That The Crystal Generates An E.m.f. When Its Shape Changes
- 3.132Medical Physics: Production And Use Understand How Ultrasound Waves Are Generated And Detected By A Piezoelectric TransducerOf Ultrasound:
- 3.133Medical Physics: Production And Use Of Ultrasound: Understand How The Reflection Of Pulses Of Ultrasound At Boundaries Between Tissues Can Be Used To Obtain Diagnostic Information About Internal Structures
- 3.134Medical Physics: Production And Use Of Ultrasound: Define The Specific Acoustic Impedance Of A Medium As Z = Ρc, Where C Is The Speed Of Sound In The Medium
- 3.135Medical Physics: Production And Use Of Ultrasound: Use Ir / I0 = (Z1 – Z2) 2 /(Z1 + Z2) 2 For The Intensity Reflection Coefficient Of A Boundary Between Two Media
- 3.136Medical Physics: Production And Use Of Ultrasound: Recall And Use I = I0e–μx For The Attenuation Of Ultrasound In Matter
- 3.137Medical Physics: Production And Use Of X-rays: Explain That X-rays Are Produced By Electron Bombardment Of A Metal Target And Calculate The Minimum Wavelength Of X-rays Produced From The Accelerating P.d.
- 3.138Medical Physics: Production And Use Of X-rays: Understand The Use Of X-rays In Imaging Internal Body Structures, Including An Understanding Of The Term Contrast In X-ray Imaging
- 3.139Medical Physics: Production And Use Of X-rays: Recall And Use I = I0e–μx For The Attenuation Of X-rays In Matter
- 3.140Medical Physics: Production And Use Of X-rays: Understand That Computed Tomography (Ct) Scanning Produces A 3d Image Of An Internal Structure By First Combining Multiple X-ray Images Taken In The Same Section From Different Angles To Obtain A 2d Image Of The Section, Then Repeating This Process Along An Axis And Combining 2d Images Of Multiple Sections
- 3.141Medical Physics: Pet Scanning: Understand That A Tracer Is A Substance Containing Radioactive Nuclei That Can Be Introduced Into The Body And Is Then Absorbed By The Tissue Being Studied
- 3.142Medical Physics: Pet Scanning: Recall That A Tracer That Decays By Β+ Decay Is Used In Positron Emission Tomography (Pet Scanning)
- 3.143Medical Physics: Pet Scanning: Understand That Annihilation Occurs When A Particle Interacts With Its Antiparticle And That Mass–energy And Momentum Are Conserved In The Process
- 3.144Medical Physics: Pet Scanning: Explain That, In Pet Scanning, Positrons Emitted By The Decay Of The Tracer Annihilate When They Interact With Electrons In The Tissue, Producing A Pair Of Gamma-ray Photons Travelling In Opposite Directions
- 3.145Medical Physics: Pet Scanning: Calculate The Energy Of The Gamma-ray Photons Emitted During The Annihilation Of An Electron-positron Pair
- 3.146Medical Physics: Pet Scanning: Understand That The Gamma-ray Photons From An Annihilation Event Travel Outside The Body And Can Be Detected, And An Image Of The Tracer Concentration In The Tissue Can Be Created By Processing The Arrival Times Of The Gamma-ray Photons
- 3.147Astronomy And Cosmology: Standard Candles: Understand The Term Luminosity As The Total Power Of Radiation Emitted By A Star
- 3.148Astronomy And Cosmology: Standard Candles: Recall And Use The Inverse Square Law For Radiant Flux Intensity F In Terms Of The Luminosity L Of The Source F = L/(4πd2 )
- 3.149Astronomy And Cosmology: Standard Candles: Understand That An Object Of Known Luminosity Is Called A Standard Candle
- 3.150Astronomy And Cosmology: Standard Candles: Understand The Use Of Standard Candles To Determine Distances To Galaxies
- 3.151Astronomy And Cosmology: Stellar Radii: Recall And Use Wien’s Displacement Law Λmax ∝ 1/t To Estimate The Peak Surface Temperature Of A Star
- 3.152Astronomy And Cosmology: Stellar Radii: Use The Stefan–boltzmann Law L = 4πσr 2 T4
- 3.153Astronomy And Cosmology: Stellar Radii: Use Wien’s Displacement Law And The Stefan–boltzmann Law To Estimate The Radius Of A Star
- 3.154Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Understand That The Lines In The Emission And Absorption Spectra From Distant Objects Show An Increase In Wavelength From Their Known Values
- 3.155Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Use ∆λ / Λ . ∆f/f . V /c For The Redshift Of Electromagnetic Radiation From A Source Moving Relative To An Observer
- 3.156Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Explain Why Redshift Leads To The Idea That The Universe Is Expanding
- 3.157Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Recall And Use Hubble’s Law V . H0d And Explain How This Leads To The Big Bang Theory (Candidates Will Only Be Required To Use Si Units)
- Video Lectures For The ContentVideo Lectures Covering Course Content In Detail14
- QuizzesShort Quizzes To Auto-Test Your Knowledge of The Syllabus29
- 5.1Motion In A Circle10 Minutes0 Questions
- 5.2Gravitational Fields10 Minutes0 Questions
- 5.3Temperature10 Minutes0 Questions
- 5.4Ideal Gases10 Minutes0 Questions
- 5.5Thermodynamics10 Minutes0 Questions
- 5.6Oscillations10 Minutes0 Questions
- 5.7Electric Fields10 Minutes0 Questions
- 5.8Capacitance10 Minutes0 Questions
- 5.9Magnetic Fields10 Minutes0 Questions
- 5.10Alternating Currents10 Minutes0 Questions
- 5.11Quantum Physics10 Minutes0 Questions
- 5.12Nuclear Physics10 Minutes0 Questions
- 5.13Medical Physics10 Minutes0 Questions
- 5.14Astronomy And Cosmology10 Minutes0 Questions
- 5.15Quizzes For Preparation: Motion In A Circle
- 5.16Quizzes For Preparation: Gravitational Fields
- 5.17Quizzes For Preparation: Temperature
- 5.18Quizzes For Preparation: Ideal Gases
- 5.19Quizzes For Preparation:
- 5.20Quizzes For Preparation: Thermodynamics
- 5.21Quizzes For Preparation: Oscillations
- 5.22Quizzes For Preparation: Capacitance
- 5.23Quizzes For Preparation: Electric Fields
- 5.24Quizzes For Preparation: Magnetic Fields
- 5.25Quizzes For Preparation: Alternating Current
- 5.26Quizzes For Preparation: Quantum Physics
- 5.27Quizzes For Preparation: Nuclear Physics
- 5.28Quizzes For Preparation: Medial Physical
- 5.29Quizzes For Preparation: Astronomy And Cosmology
- Quizzes For PreparationQuizzes With Detailed Explained Answers And Common Mistakes Discussed In Detail157
- 6.1Motion In A Circle: Kinematics Of Uniform Circular Motion: Define The Radian And Express Angular Displacement In Radians
- 6.2Motion In A Circle: Kinematics Of Uniform Circular Motion: Understand And Use The Concept Of Angular Speed
- 6.3Motion In A Circle: Kinematics Of Uniform Circular Motion: Recall And Use Ω = 2π/t And V = Rω
- 6.4Motion In A Circle: Centripetal Acceleration: Understand That A Force Of Constant Magnitude That Is Always Perpendicular To The Direction Of Motion Causes Centripetal Acceleration
- 6.5Motion In A Circle: Centripetal Acceleration: Understand That Centripetal Acceleration Causes Circular Motion With A Constant Angular Speed
- 6.6Motion In A Circle: Centripetal Acceleration: Recall And Use A = Rω2 And A = V2 /r
- 6.7Motion In A Circle: Centripetal Acceleration: Recall And Use F = Mrω2 And F = Mv2 /r
- 6.8Gravitational Fields: Gravitational Field: Understand That A Gravitational Field Is An Example Of A Field Of Force And Define Gravitational Field As Force Per Unit Mass
- 6.9Gravitational Fields: Gravitational Field: Represent A Gravitational Field By Means Of Field Lines
- 6.10Gravitational Fields: Gravitational Force Between Point Masses: Understand That, For A Point Outside A Uniform Sphere, The Mass Of The Sphere May Be Considered To Be A Point Mass At Its Centre
- 6.11Gravitational Fields: Gravitational Force Between Point Masses: Recall And Use Newton’s Law Of Gravitation F = Gm1m2 /r 2 For The Force Between Two Point Masses
- 6.12Gravitational Fields: Gravitational Force Between Point Masses: Analyse Circular Orbits In Gravitational Fields By Relating The Gravitational Force To The Centripetal Acceleration It Causes
- 6.13Gravitational Fields: Gravitational Force Between Point Masses: Understand That A Satellite In A Geostationary Orbit Remains At The Same Point Above The Earth’s Surface, With An Orbital Period Of 24 Hours, Orbiting From West To East, Directly Above The Equator
- 6.14Gravitational Fields: Gravitational Field Of A Point Mass: Derive, From Newton’s Law Of Gravitation And The Definition Of Gravitational Field, The Equation G = Gm/r 2 For The Gravitational Field Strength Due To A Point Mass
- 6.15Gravitational Fields: Gravitational Field Of A Point Mass: Recall And Use G = Gm/r 2
- 6.16Gravitational Fields: Gravitational Field Of A Point Mass: Understand Why G Is Approximately Constant For Small Changes In Height Near The Earth’s Surface
- 6.17Gravitational Fields: Gravitational Potential: Define Gravitational Potential At A Point As The Work Done Per Unit Mass In Bringing A Small Test Mass From Infinity To The Point
- 6.18Gravitational Fields: Gravitational Potential: Use Φ = –gm/r For The Gravitational Potential In The Field Due To A Point Mass
- 6.19Gravitational Fields: Gravitational Potential: Understand How The Concept Of Gravitational Potential Leads To The Gravitational Potential Energy Of Two Point Masses And Use Ep = –gmm/r
- 6.20Temperature: Thermal Equilibrium: Understand That (Thermal) Energy Is Transferred From A Region Of Higher Temperature To A Region Of Lower Temperature
- 6.21Temperature: Thermal Equilibrium: Understand That Regions Of Equal Temperature Are In Thermal Equilibrium
- 6.22Temperature: Temperature Scales: Understand That A Physical Property That Varies With Temperature May Be Used For The Measurement Of Temperature And State Examples Of Such Properties, Including The Density Of A Liquid, Volume Of A Gas At Constant Pressure, Resistance Of A Metal, E.m.f. Of A Thermocouple
- 6.23Temperature: Temperature Scales: Understand That The Scale Of Thermodynamic Temperature Does Not Depend On The Property Of Any Particular Substance
- 6.24Temperature: Temperature Scales: Convert Temperatures Between Kelvin And Degrees Celsius And Recall That T/k = Θ/ °c + 273.15
- 6.25Temperature: Temperature Scales: Understand That The Lowest Possible Temperature Is Zero Kelvin On The Thermodynamic Temperature Scale And That This Is Known As Absolute Zero
- 6.26Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Heat Capacity
- 6.27Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Latent Heat And Distinguish Between Specific Latent Heat Of Fusion And Specific Latent Heat Of Vaporisation
- 6.28Ideal Gases: The Mole: Understand That Amount Of Substance Is An Si Base Quantity With The Base Unit Mol
- 6.29Ideal Gases: The Mole: Use Molar Quantities Where One Mole Of Any Substance Is The Amount Containing A Number Of Particles Of That Substance Equal To The Avogadro Constant Na
- 6.30Ideal Gases: Equation Of State: Understand That A Gas Obeying Pv ∝ T, Where T Is The Thermodynamic Temperature, Is Known As An Ideal Gas
- 6.31Ideal Gases: Equation Of State: Recall And Use The Equation Of State For An Ideal Gas Expressed As Pv = Nrt, Where N = Amount Of Substance (Number Of Moles) And As Pv = Nkt, Where N = Number Of Molecules
- 6.32Ideal Gases: Equation Of State: Recall That The Boltzmann Constant K Is Given By K = R/na
- 6.33Ideal Gases: Kinetic Theory Of Gases: State The Basic Assumptions Of The Kinetic Theory Of Gases
- 6.34Ideal Gases: Kinetic Theory Of Gases: Explain How Molecular Movement Causes The Pressure Exerted By A Gas And Derive And Use The Relationship Pv = 3 1 Nm, Where Is The Mean-square Speed (A Simple Model Considering One-dimensional Collisions And Then Extending To Three Dimensions Using 3 1 = Is Sufficient)
- 6.35Ideal Gases: Kinetic Theory Of Gases: Understand That The Root-mean-square Speed Cr.m.s. Is Given By C 2
- 6.36Ideal Gases: Kinetic Theory Of Gases: Compare Pv = 3 1 Nm With Pv = Nkt To Deduce That The Average Translational Kinetic Energy Of A Molecule Is 2 3 Kt, And Recall And Use This Expression
- 6.37Thermodynamics: Internal Energy: Understand That Internal Energy Is Determined By The State Of The System And That It Can Be Expressed As The Sum Of A Random Distribution Of Kinetic And Potential Energies Associated With The Molecules Of A System
- 6.38Thermodynamics: Internal Energy: Relate A Rise In Temperature Of An Object To An Increase In Its Internal Energy
- 6.39Thermodynamics: The First Law Of Thermodynamics: Recall And Use W = P∆v For The Work Done When The Volume Of A Gas Changes At Constant Pressure And Understand The Difference Between The Work Done By The Gas And The Work Done On The Gas
- 6.40Thermodynamics: The First Law Of Thermodynamics: Recall And Use The First Law Of Thermodynamics ∆u = Q + W Expressed In Terms Of The Increase In Internal Energy, The Heating Of The System (Energy Transferred To The System By Heating) And The Work Done On The System
- 6.41Oscillations: Simple Harmonic Oscillations: Understand And Use The Terms Displacement, Amplitude, Period, Frequency, Angular Frequency And Phase Difference In The Context Of Oscillations, And Express The Period In Terms Of Both Frequency And Angular Frequency
- 6.42Oscillations: Simple Harmonic Oscillations: Understand That Simple Harmonic Motion Occurs When Acceleration Is Proportional To Displacement From A Fixed Point And In The Opposite Direction
- 6.43Oscillations: Simple Harmonic Oscillations: Use A = –ω2 X And Recall And Use, As A Solution To This Equation, X = X0 Sin Ωt
- 6.44Oscillations: Simple Harmonic Oscillations: Use The Equations V = V0 Cos Ωt And V = ±ω ( ) X X 0 2 2 −
- 6.45Oscillations: Simple Harmonic Oscillations: Analyse And Interpret Graphical Representations Of The Variations Of Displacement, Velocity And Acceleration For Simple Harmonic Motion
- 6.46Oscillations: Energy In Simple Harmonic Motion: Describe The Interchange Between Kinetic And Potential Energy During Simple Harmonic Motion
- 6.47Oscillations: Energy In Simple Harmonic Motion: Recall And Use E = 2 1 Mω2 X0 2 For The Total Energy Of A System Undergoing Simple Harmonic Motion
- 6.48Oscillations: Damped And Forced Oscillations, Resonance: Understand That A Resistive Force Acting On An Oscillating System Causes Damping
- 6.49Oscillations: Damped And Forced Oscillations, Resonance: Understand And Use The Terms Light, Critical And Heavy Damping And Sketch Displacement–time Graphs Illustrating These Types Of Damping
- 6.50Oscillations: Damped And Forced Oscillations, Resonance: Understand That Resonance Involves A Maximum Amplitude Of Oscillations And That This Occurs When An Oscillating System Is Forced To Oscillate At Its Natural Frequency
- 6.51Electric Fields: Electric Fields And Field Lines: Understand That An Electric Field Is An Example Of A Field Of Force And Define Electric Field As Force Per Unit Positive Charge
- 6.52Electric Fields: Electric Fields And Field Lines: Recall And Use F = Qe For The Force On A Charge In An Electric Field
- 6.53Electric Fields: Electric Fields And Field Lines: Represent An Electric Field By Means Of Field Lines
- 6.54Electric Fields: Uniform Electric Fields: Recall And Use E = ∆v/∆d To Calculate The Field Strength Of The Uniform Field Between Charged Parallel Plates
- 6.55Electric Fields: Uniform Electric Fields: Describe The Effect Of A Uniform Electric Field On The Motion Of Charged Particles
- 6.56Electric Fields: Electric Force Between Point Charges: Understand That, For A Point Outside A Spherical Conductor, The Charge On The Sphere May Be Considered To Be A Point Charge At Its Centre
- 6.57Electric Fields: Electric Force Between Point Charges: Recall And Use Coulomb’s Law F = Q1q2 /(4πε0r 2 ) For The Force Between Two Point Charges In Free Space
- 6.58Electric Fields: Electric Field Of A Point Charge: Recall And Use E = Q/(4πε0r 2 ) For The Electric Field Strength Due To A Point Charge In Free Space
- 6.59Electric Fields: Electric Potential: Define Electric Potential At A Point As The Work Done Per Unit Positive Charge In Bringing A Small Test Charge From Infinity To The Point
- 6.60Electric Fields: Electric Potential: Recall And Use The Fact That The Electric Field At A Point Is Equal To The Negative Of Potential Gradient At That Point
- 6.61Electric Fields: Electric Potential: Use V = Q/(4πε0r) For The Electric Potential In The Field Due To A Point Charge
- 6.62Electric Fields: Electric Potential: Understand How The Concept Of Electric Potential Leads To The Electric Potential Energy Of Two Point Charges And Use Ep = Qq/(4πε0r)
- 6.63Capacitance: Capacitors And Capacitance: Define Capacitance, As Applied To Both Isolated Spherical Conductors And To Parallel Plate Capacitors
- 6.64Capacitance: Capacitors And Capacitance: Recall And Use C = Q/v
- 6.65Capacitance: Capacitors And Capacitance: v
- 6.66Capacitance: Capacitors And Capacitance: Use The Capacitance Formulae For Capacitors In Series And In Parallel
- 6.67Capacitance: Energy Stored In A Capacitor: Determine The Electric Potential Energy Stored In A Capacitor From The Area Under The Potential–charge Graph
- 6.68Capacitance: Energy Stored In A Capacitor: Recall And Use W = 2 1 Qv = 2 1 Cv2
- 6.69Capacitance: Discharging A Capacitor: Analyse Graphs Of The Variation With Time Of Potential Difference, Charge And Current For A Capacitor Discharging Through A Resistor
- 6.70Capacitance: Discharging A Capacitor:Recall And Use Τ = Rc For The Time Constant For A Capacitor Discharging Through A Resistor
- 6.71Capacitance: Discharging A Capacitor: Use Equations Of The Form X = X0 E–(T/rc) Where X Could Represent Current, Charge Or Potential Difference For A Capacitor Discharging Through A Resistor
- 6.72Magnetic Fields: Concept Of A Magnetic Field: Understand That A Magnetic Field Is An Example Of A Field Of Force Produced Either By Moving Charges Or By Permanent Magnets
- 6.73Magnetic Fields: Concept Of A Magnetic Field: Represent A Magnetic Field By Field Lines
- 6.74Magnetic Fields: Force On A Current-carrying Conductor: Understand That A Force Might Act On A Current-carrying Conductor Placed In A Magnetic Field
- 6.75Magnetic Fields: Force On A Current-carrying Conductor: Recall And Use The Equation F = Bil Sin Θ, With Directions As Interpreted By Fleming’s Left-hand Rule
- 6.76Magnetic Fields: Force On A Current-carrying Conductor: Define Magnetic Flux Density As The Force Acting Per Unit Current Per Unit Length On A Wire Placed At Rightangles To The Magnetic Field
- 6.77Magnetic Fields: Force On A Moving Charge: Determine The Direction Of The Force On A Charge Moving In A Magnetic Field
- 6.78Magnetic Fields: Force On A Moving Charge: Recall And Use F = Bqv Sin Θ
- 6.79Magnetic Fields: Force On A Moving Charge: Understand The Origin Of The Hall Voltage And Derive And Use The Expression Vh = Bi /(Ntq), Where T = Thickness
- 6.80Magnetic Fields: Force On A Moving Charge: Understand The Use Of A Hall Probe To Measure Magnetic Flux Density
- 6.81Magnetic Fields: Force On A Moving Charge: Describe The Motion Of A Charged Particle Moving In A Uniform Magnetic Field Perpendicular To The Direction Of Motion Of The Particle
- 6.82Magnetic Fields: Force On A Moving Charge: Explain How Electric And Magnetic Fields Can Be Used In Velocity Selection
- 6.83Magnetic Fields: Magnetic Fields Due To Currents: Sketch Magnetic Field Patterns Due To The Currents In A Long Straight Wire, A Flat Circular Coil And A Long Solenoid
- 6.84Magnetic Fields: Magnetic Fields Due To Currents: Understand That The Magnetic Field Due To The Current In A Solenoid Is Increased By A Ferrous Core
- 6.85Magnetic Fields: Magnetic Fields Due To Currents: Explain The Origin Of The Forces Between Current-carrying Conductors And Determine The Direction Of The Forces
- 6.86Magnetic Fields: Electromagnetic Induction: Define Magnetic Flux As The Product Of The Magnetic Flux Density And The Cross-sectional Area Perpendicular To The Direction Of The Magnetic Flux Density
- 6.87Magnetic Fields: Electromagnetic Induction: Recall And Use Φ = Ba
- 6.88Magnetic Fields: Electromagnetic Induction: Understand And Use The Concept Of Magnetic Flux Linkage
- 6.89Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That A Changing Magnetic Flux Can Induce An E.m.f. In A Circuit
- 6.90Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That The Induced E.m.f. Is In Such A Direction As To Oppose The Change Producing It
- 6.91Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: The Factors Affecting The Magnitude Of The Induced E.m.f.
- 6.92Magnetic Fields: Electromagnetic Induction: Recall And Use Faraday’s And Lenz’s Laws Of Electromagnetic Induction
- 6.93Alternating Currents: Characteristics Of Alternating Currents: Understand And Use The Terms Period, Frequency And Peak Value As Applied To An Alternating Current Or Voltage
- 6.94Alternating Currents: Characteristics Of Alternating Currents: Use Equations Of The Form X = X0 Sin Ωt Representing A Sinusoidally Alternating Current Or Voltage
- 6.95Alternating Currents: Characteristics Of Alternating Currents: Recall And Use The Fact That The Mean Power In A Resistive Load Is Half The Maximum Power For A Sinusoidal Alternating Current
- 6.96Alternating Currents: Characteristics Of Alternating Currents: Distinguish Between Root-mean-square (R.m.s.) And Peak Values And Recall And Use I R.m.s. = I0 / 2 And Vr.m.s. = V0 / 2 For A Sinusoidal Alternating Current
- 6.97Alternating Currents: Rectification And Smoothing: Distinguish Graphically Between Half-wave And Full-wave Rectification
- 6.98Alternating Currents: Rectification And Smoothing: Explain The Use Of A Single Diode For The Half-wave Rectification Of An Alternating Current
- 6.99Alternating Currents: Rectification And Smoothing: Explain The Use Of Four Diodes (Bridge Rectifier) For The Full-wave Rectification Of An Alternating Current
- 6.100Alternating Currents: Rectification And Smoothing: Analyse The Effect Of A Single Capacitor In Smoothing, Including The Effect Of The Values Of Capacitance And The Load Resistance
- 6.101Quantum Physics: Energy And Momentum Of A Photon: Understand That Electromagnetic Radiation Has A Particulate Nature
- 6.102Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Is A Quantum Of Electromagnetic Energy
- 6.103Quantum Physics: Energy And Momentum Of A Photon: Recall And Use E = Hf
- 6.104Quantum Physics: Energy And Momentum Of A Photon: Use The Electronvolt (Ev) As A Unit Of Energy
- 6.105Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Has Momentum And That The Momentum Is Given By P = E/c
- 6.106Quantum Physics: Photoelectric Effect: Understand That Photoelectrons May Be Emitted From A Metal Surface When It Is Illuminated By Electromagnetic Radiation
- 6.107Quantum Physics: Photoelectric Effect: Understand And Use The Terms Threshold Frequency And Threshold Wavelength
- 6.108Quantum Physics: Photoelectric Effect: Explain Photoelectric Emission In Terms Of Photon Energy And Work Function Energy
- 6.109Quantum Physics: Photoelectric Effect: Recall And Use Hf = Φ + 2 1 Mvmax 2
- 6.110Quantum Physics: Photoelectric Effect: Explain Why The Maximum Kinetic Energy Of Photoelectrons Is Independent Of Intensity, Whereas The Photoelectric Current Is Proportional To Intensity
- 6.111Quantum Physics: Wave-particle Duality: Understand That The Photoelectric Effect Provides Evidence For A Particulate Nature Of Electromagnetic Radiation While Phenomena Such As Interference And Diffraction Provide Evidence For A Wave Nature
- 6.112Quantum Physics: Wave-particle Duality: Describe And Interpret Qualitatively The Evidence Provided By Electron Diffraction For The Wave Nature Of Particles
- 6.113Quantum Physics: Wave-particle Duality: Understand The De Broglie Wavelength As The Wavelength Associated With A Moving Particle
- 6.114Quantum Physics: Wave-particle Duality: Recall And Use Λ = H/p
- 6.115Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand That There Are Discrete Electron Energy Levels In Isolated Atoms (E.g. Atomic Hydrogen)
- 6.116Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand The Appearance And Formation Of Emission And Absorption Line Spectra
- 6.117Quantum Physics: Energy Levels In Atoms And Line Spectra: Recall And Use Hf = E1 – E2
- 6.118Nuclear Physics: Mass Defect And Nuclear Binding Energy: Understand The Equivalence Between Energy And Mass As Represented By E = Mc2 And Recall And Use This Equation
- 6.119Nuclear Physics: Mass Defect And Nuclear Binding Energy: Represent Simple Nuclear Reactions By Nuclear Equations Of The Form 7n He O H 14 2 4 8 17 1 1 + + “
- 6.120Nuclear Physics: Mass Defect And Nuclear Binding Energy: Define And Use The Terms Mass Defect And Binding Energy
- 6.121Nuclear Physics: Mass Defect And Nuclear Binding Energy: Sketch The Variation Of Binding Energy Per Nucleon With Nucleon Number
- 6.122Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain What Is Meant By Nuclear Fusion And Nuclear Fission
- 6.123Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain The Relevance Of Binding Energy Per Nucleon To Nuclear Reactions, Including Nuclear Fusion And Nuclear Fission
- 6.124Nuclear Physics: Mass Defect And Nuclear Binding Energy: Calculate The Energy Released In Nuclear Reactions Using E = C2 ∆m
- 6.125Nuclear Physics: Radioactive Decay: Understand That Fluctuations In Count Rate Provide Evidence For The Random Nature Of Radioactive Decay
- 6.126Nuclear Physics: Radioactive Decay: Understand That Radioactive Decay Is Both Spontaneous And Random
- 6.127Nuclear Physics: Radioactive Decay: Define Activity And Decay Constant, And Recall And Use A = Λn
- 6.128Nuclear Physics: Radioactive Decay: Define Half-life
- 6.129Nuclear Physics: Radioactive Decay: Use Λ = 0.693/t 2 1
- 6.130Nuclear Physics: Radioactive Decay: Understand The Exponential Nature Of Radioactive Decay, And Sketch And Use The Relationship X = X0e–λt , Where X Could Represent Activity, Number Of Undecayed Nuclei Or Received Count Rate
- 6.131Medical Physics: Production And Use Of Ultrasound: Understand That A Piezo-electric Crystal Changes Shape When A P.d. Is Applied Across It And That The Crystal Generates An E.m.f. When Its Shape Changes
- 6.132Medical Physics: Production And Use Understand How Ultrasound Waves Are Generated And Detected By A Piezoelectric TransducerOf Ultrasound:
- 6.133Medical Physics: Production And Use Of Ultrasound: Understand How The Reflection Of Pulses Of Ultrasound At Boundaries Between Tissues Can Be Used To Obtain Diagnostic Information About Internal Structures
- 6.134Medical Physics: Production And Use Of Ultrasound: Define The Specific Acoustic Impedance Of A Medium As Z = Ρc, Where C Is The Speed Of Sound In The Medium
- 6.135Medical Physics: Production And Use Of Ultrasound: Use Ir / I0 = (Z1 – Z2) 2 /(Z1 + Z2) 2 For The Intensity Reflection Coefficient Of A Boundary Between Two Media
- 6.136Medical Physics: Production And Use Of Ultrasound: Recall And Use I = I0e–μx For The Attenuation Of Ultrasound In Matter
- 6.137Medical Physics: Production And Use Of X-rays: Explain That X-rays Are Produced By Electron Bombardment Of A Metal Target And Calculate The Minimum Wavelength Of X-rays Produced From The Accelerating P.d.
- 6.138Medical Physics: Production And Use Of X-rays: Understand The Use Of X-rays In Imaging Internal Body Structures, Including An Understanding Of The Term Contrast In X-ray Imaging
- 6.139Medical Physics: Production And Use Of X-rays: Recall And Use I = I0e–μx For The Attenuation Of X-rays In Matter
- 6.140Medical Physics: Production And Use Of X-rays: Understand That Computed Tomography (Ct) Scanning Produces A 3d Image Of An Internal Structure By First Combining Multiple X-ray Images Taken In The Same Section From Different Angles To Obtain A 2d Image Of The Section, Then Repeating This Process Along An Axis And Combining 2d Images Of Multiple Sections
- 6.141Medical Physics: Pet Scanning: Understand That A Tracer Is A Substance Containing Radioactive Nuclei That Can Be Introduced Into The Body And Is Then Absorbed By The Tissue Being Studied
- 6.142Medical Physics: Pet Scanning: Recall That A Tracer That Decays By Β+ Decay Is Used In Positron Emission Tomography (Pet Scanning)
- 6.143Medical Physics: Pet Scanning: Understand That Annihilation Occurs When A Particle Interacts With Its Antiparticle And That Mass–energy And Momentum Are Conserved In The Process
- 6.144Medical Physics: Pet Scanning: Explain That, In Pet Scanning, Positrons Emitted By The Decay Of The Tracer Annihilate When They Interact With Electrons In The Tissue, Producing A Pair Of Gamma-ray Photons Travelling In Opposite Directions
- 6.145Medical Physics: Pet Scanning: Calculate The Energy Of The Gamma-ray Photons Emitted During The Annihilation Of An Electron-positron Pair
- 6.146Medical Physics: Pet Scanning: Understand That The Gamma-ray Photons From An Annihilation Event Travel Outside The Body And Can Be Detected, And An Image Of The Tracer Concentration In The Tissue Can Be Created By Processing The Arrival Times Of The Gamma-ray Photons
- 6.147Astronomy And Cosmology: Standard Candles: Understand The Term Luminosity As The Total Power Of Radiation Emitted By A Star
- 6.148Astronomy And Cosmology: Standard Candles: Recall And Use The Inverse Square Law For Radiant Flux Intensity F In Terms Of The Luminosity L Of The Source F = L/(4πd2 )
- 6.149Astronomy And Cosmology: Standard Candles: Understand That An Object Of Known Luminosity Is Called A Standard Candle
- 6.150Astronomy And Cosmology: Standard Candles: Understand The Use Of Standard Candles To Determine Distances To Galaxies
- 6.151Astronomy And Cosmology: Stellar Radii: Recall And Use Wien’s Displacement Law Λmax ∝ 1/t To Estimate The Peak Surface Temperature Of A Star
- 6.152Astronomy And Cosmology: Stellar Radii: Use The Stefan–boltzmann Law L = 4πσr 2 T4
- 6.153Astronomy And Cosmology: Stellar Radii: Use Wien’s Displacement Law And The Stefan–boltzmann Law To Estimate The Radius Of A Star
- 6.154Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Understand That The Lines In The Emission And Absorption Spectra From Distant Objects Show An Increase In Wavelength From Their Known Values
- 6.155Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Use ∆λ / Λ . ∆f/f . V /c For The Redshift Of Electromagnetic Radiation From A Source Moving Relative To An Observer
- 6.156Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Explain Why Redshift Leads To The Idea That The Universe Is Expanding
- 6.157Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Recall And Use Hubble’s Law V . H0d And Explain How This Leads To The Big Bang Theory (Candidates Will Only Be Required To Use Si Units)
- AssignmentsDetailed Assignments For Syllabus Preparation (Including Past Paper Questions)14
- 7.1Motion In A Circle3 Days
- 7.2Gravitational Fields3 Days
- 7.3Temperature3 Days
- 7.4Ideal Gases3 Days
- 7.5Thermodynamics3 Days
- 7.6Oscillations3 Days
- 7.7Electric Fields3 Days
- 7.8Capacitance3 Days
- 7.9Magnetic Fields3 Days
- 7.10Alternating Currents3 Days
- 7.11Quantum Physics3 Days
- 7.12Nuclear Physics3 Days
- 7.13Medical Physics3 Days
- 7.14Astronomy And Cosmology3 Days
- Paper Pattern/ Paper Preparation/ Techniques To Attempt The Paper/ Common Mistakes To AvoidDetailed Information Including Written + Video Material Regarding Paper Attempt / Preparation/ Techniques/ Common Mistakes To Avoid50
- 8.1Paper Structure, Weighting & Examiner Intent: How Paper 4 And Paper 5 Combine To Decide A*–E Grades At A2 Level
- 8.2Paper Structure, Weighting & Examiner Intent: Examiner Intent Behind A2 Structured Questions Vs AS Structured Questions
- 8.3Paper Structure, Weighting & Examiner Intent: How Assessment Objectives AO1, AO2 And AO3 Are Balanced In A2 Papers
- 8.4Paper Structure, Weighting & Examiner Intent: Typical Mark Allocation Patterns In Paper 4 Across Long And Short Questions
- 8.5Paper Structure, Weighting & Examiner Intent: Why Paper 5 Is A Differentiator Paper For A And A* Candidates
- 8.6Paper Structure, Weighting & Examiner Intent: Understanding How Cambridge Scales Difficulty Across Questions Within Paper 4
- 8.7Paper Pattern/ Paper Preparation/ Techniques To Attempt The Paper/ Common Mistakes To Avoid:: How Carry-Forward AS Knowledge Is Assumed But Never Re-Explained In A2
- 8.8Command Words, Question Language & Traps: A2 Command Words: What Examiners Actually Expect For Each
- 8.9Command Words, Question Language & Traps: The Real Difference Between “State”, “Explain”, “Show”, “Determine” And “Evaluate”
- 8.10Command Words, Question Language & Traps: How “Hence” And “Hence Or Otherwise” Control Your Method And Marks
- 8.11Command Words, Question Language & Traps: Multi-Part Question Dependency: How One Wrong Step Affects Later Marks
- 8.12Command Words, Question Language & Traps: Recognising When Examiners Want Physics Reasoning Vs Mathematics
- 8.13Command Words, Question Language & Traps: Hidden Instructions Embedded In Question Wording
- 8.14Mathematical Execution & Calculation Control: Structuring Long A2 Calculations To Avoid Method Mark Loss
- 8.15Mathematical Execution & Calculation Control: When Substitution Must Be Shown And When It Can Be Skipped
- 8.16Mathematical Execution & Calculation Control: Common Power-Of-Ten And Unit Conversion Errors Seen By Examiners
- 8.17Mathematical Execution & Calculation Control: Significant Figures Rules As Actually Applied In Mark Schemes
- 8.18Mathematical Execution & Calculation Control: Handling Rearrangement Of Complex A2 Formulae Safely
- 8.19Mathematical Execution & Calculation Control: Avoiding Rounding Errors That Kill Final Accuracy Marks
- 8.20Mathematical Execution & Calculation Control: Recognising When An Answer Is Physically Impossible Before Writing It
- 8.21Graphs, Data Handling & Interpretation (A2 Level): Drawing Examiner-Perfect Graphs Under Exam Conditions
- 8.22Graphs, Data Handling & Interpretation (A2 Level): Axis Scaling Errors That Lose Marks Even When The Physics Is Right
- 8.23Graphs, Data Handling & Interpretation (A2 Level): Gradient, Intercept And Their Physical Meaning In A2 Contexts
- 8.24Graphs, Data Handling & Interpretation (A2 Level): Linearisation Techniques And Why Examiners Love Them
- 8.25Graphs, Data Handling & Interpretation (A2 Level): Identifying Trends, Proportionality And Non-Linear Behaviour
- 8.26Graphs, Data Handling & Interpretation (A2 Level): Extracting Correct Conclusions From Imperfect Experimental Data
- 8.27Graphs, Data Handling & Interpretation (A2 Level): Avoiding Over-Interpretation Of Data Tables
- 8.28Written Explanations & Physics Language: Writing High-Precision Explanations That Match Marking Points
- 8.29Written Explanations & Physics Language: How Excess Writing Actively Loses Marks At A2 Level
- 8.30Written Explanations & Physics Language: Correct Use Of Scientific Terminology Under Time Pressure
- 8.31Written Explanations & Physics Language: Structuring 3–5 Mark Explanations Efficiently
- 8.32Written Explanations & Physics Language: Avoiding Vague Statements That Examiners Ignore
- 8.33Written Explanations & Physics Language: Using Cause–Effect Chains Correctly In Explanations
- 8.34Paper 5 – Planning, Analysis & Evaluation (Full Mastery): The Exact Skills Cambridge Tests In Paper 5 (And What It Does Not Test)
- 8.35Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Writing Experimental Plans That Are Practical, Testable And Mark-Worthy
- 8.36Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Identifying Independent, Dependent And Control Variables Correctly
- 8.37Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Writing Methods That Are Detailed Without Being Unrealistic
- 8.38Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Distinguishing Between Random Errors, Systematic Errors And Limitations
- 8.39Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Writing Improvements That Are Specific, Practical And Marked
- 8.40Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Handling Uncertainty, Precision And Resolution Without Confusion
- 8.41Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Percentage Uncertainty Calculations And Propagation Rules
- 8.42Paper 5 – Planning, Analysis & Evaluation (Full Mastery): Recognising Correlation, Trend And Scatter In Experimental Results
- 8.43Examiner-Reported Common Mistakes (A2 Specific): Repeating AS-Level Explanations Instead Of Applying A2 Reasoning
- 8.44Examiner-Reported Common Mistakes (A2 Specific): Ignoring Given Information And Re-Deriving Unnecessary Physics
- 8.45Examiner-Reported Common Mistakes (A2 Specific): Losing Marks Through Poor Diagram Use And Labelling
- 8.46Examiner-Reported Common Mistakes (A2 Specific): Misreading Axes, Constants Or Given Conditions
- 8.47Examiner-Reported Common Mistakes (A2 Specific): Answering From Memory Instead Of From The Question
- 8.48Examiner-Reported Common Mistakes (A2 Specific): Writing Contradictory Statements In Explanations
- 8.49Exam-Day Strategy & Final Execution: How To Use The Formula Sheet Strategically Without Dependency
- 8.50Exam-Day Strategy & Final Execution: Question Order, Skipping Strategy And Final 15-Minute A2 Submission Technique
- Solved Past PapersDetailed Written Explanations And Solutions of Past Papers, Including Model Answers and Explanations For Past Paper Questions81
- 9.1May June 2020 Paper 41
- 9.2May June 2020 Paper 42
- 9.3May June 2020 Paper 43
- 9.4May June 2020 Paper 51
- 9.5May June 2020 Paper 52
- 9.6May June 2020 Paper 53
- 9.7Feb March 2020 Paper 42
- 9.8October November 2020 Paper 41
- 9.9October November 2020 Paper 42
- 9.10Feb March 2020 Paper 52
- 9.11October November 2020 Paper 43
- 9.12October November 2020 Paper 51
- 9.13October November 2020 Paper 52
- 9.14October November 2020 Paper 53
- 9.15May June 2021 Paper 41
- 9.16May June 2021 Paper 42
- 9.17May June 2021 Paper 43
- 9.18May June 2021 Paper 51
- 9.19May June 2021 Paper 52
- 9.20May June 2021 Paper 53
- 9.21Feb March 2021 Paper 42
- 9.22Feb March 2021 Paper 52
- 9.23October November 2021 Paper 41
- 9.24October November 2021 Paper 42
- 9.25October November 2021 Paper 43
- 9.26May June 2022 Paper 41
- 9.27May June 2022 Paper 42
- 9.28May June 2022 Paper 43
- 9.29May June 2022 Paper 51
- 9.30May June 2022 Paper 52
- 9.31May June 2022 Paper 53
- 9.32Feb March 2022 Paper 42
- 9.33Feb March 2022 Paper 52
- 9.34October November 2022 Paper 41
- 9.35October November 2022 Paper 42
- 9.36October November 2022 Paper 43
- 9.37October November 2022 Paper 51
- 9.38October November 2022 Paper 52
- 9.39October November 2022 Paper 53
- 9.40May June 2023 Paper 41
- 9.41May June 2023 Paper 42
- 9.42May June 2023 Paper 43
- 9.43May June 2023 Paper 51
- 9.44May June 2023 Paper 52
- 9.45May June 2023 Paper 53
- 9.46Feb March 2023 Paper 42
- 9.47Feb March 2023 Paper 52
- 9.48October November 2023 Paper 41
- 9.49October November 2023 Paper 42
- 9.50October November 2023 Paper 43
- 9.51October November 2023 Paper 51
- 9.52October November 2023 Paper 52
- 9.53October November 2023 Paper 53
- 9.54May June 2024 Paper 41
- 9.55May June 2024 Paper 42
- 9.56May June 2024 Paper 43
- 9.57May June 2024 Paper 51
- 9.58May June 2024 Paper 52
- 9.59May June 2024 Paper 53
- 9.60Feb March 2024 Paper 42
- 9.61Feb March 2024 Paper 52
- 9.62October November 2024 Paper 41
- 9.63October November 2024 Paper 42
- 9.64October November 2024 Paper 43
- 9.65October November 2024 Paper 51
- 9.66October November 2024 Paper 52
- 9.67October November 2024 Paper 53
- 9.68May June 2025 Paper 42
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- Past Paper SessionsVideo Content Regarding Past Paper Solutions81
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- Cheat Sheets156
- 11.1Motion In A Circle: Kinematics Of Uniform Circular Motion: Define The Radian And Express Angular Displacement In Radians
- 11.2Motion In A Circle: Kinematics Of Uniform Circular Motion: Understand And Use The Concept Of Angular Speed
- 11.3Motion In A Circle: Kinematics Of Uniform Circular Motion: Recall And Use Ω = 2π/t And V = Rω
- 11.4Motion In A Circle: Centripetal Acceleration: Understand That A Force Of Constant Magnitude That Is Always Perpendicular To The Direction Of Motion Causes Centripetal Acceleration
- 11.5Motion In A Circle: Centripetal Acceleration: Understand That Centripetal Acceleration Causes Circular Motion With A Constant Angular Speed
- 11.6Motion In A Circle: Centripetal Acceleration: Recall And Use A = Rω2 And A = V2 /r
- 11.7Motion In A Circle: Centripetal Acceleration: Recall And Use F = Mrω2 And F = Mv2 /r
- 11.8Gravitational Fields: Gravitational Field: Understand That A Gravitational Field Is An Example Of A Field Of Force And Define Gravitational Field As Force Per Unit Mass
- 11.9Gravitational Fields: Gravitational Field: Represent A Gravitational Field By Means Of Field Lines
- 11.10Gravitational Fields: Gravitational Force Between Point Masses: Understand That, For A Point Outside A Uniform Sphere, The Mass Of The Sphere May Be Considered To Be A Point Mass At Its Centre
- 11.11Gravitational Fields: Gravitational Force Between Point Masses: Recall And Use Newton’s Law Of Gravitation F = Gm1m2 /r 2 For The Force Between Two Point Masses
- 11.12Gravitational Fields: Gravitational Force Between Point Masses: Analyse Circular Orbits In Gravitational Fields By Relating The Gravitational Force To The Centripetal Acceleration It Causes
- 11.13Gravitational Fields: Gravitational Force Between Point Masses: Understand That A Satellite In A Geostationary Orbit Remains At The Same Point Above The Earth’s Surface, With An Orbital Period Of 24 Hours, Orbiting From West To East, Directly Above The Equator
- 11.14Gravitational Fields: Gravitational Field Of A Point Mass: Derive, From Newton’s Law Of Gravitation And The Definition Of Gravitational Field, The Equation G = Gm/r 2 For The Gravitational Field Strength Due To A Point Mass
- 11.15Gravitational Fields: Gravitational Field Of A Point Mass: Recall And Use G = Gm/r 2
- 11.16Gravitational Fields: Gravitational Field Of A Point Mass: Understand Why G Is Approximately Constant For Small Changes In Height Near The Earth’s Surface
- 11.17Gravitational Fields: Gravitational Potential: Define Gravitational Potential At A Point As The Work Done Per Unit Mass In Bringing A Small Test Mass From Infinity To The Point
- 11.18Gravitational Fields: Gravitational Potential: Use Φ = –gm/r For The Gravitational Potential In The Field Due To A Point Mass
- 11.19Gravitational Fields: Gravitational Potential: Understand How The Concept Of Gravitational Potential Leads To The Gravitational Potential Energy Of Two Point Masses And Use Ep = –gmm/r
- 11.20Temperature: Thermal Equilibrium: Understand That (Thermal) Energy Is Transferred From A Region Of Higher Temperature To A Region Of Lower Temperature
- 11.21Temperature: Thermal Equilibrium: Understand That Regions Of Equal Temperature Are In Thermal Equilibrium
- 11.22Temperature: Temperature Scales: Understand That A Physical Property That Varies With Temperature May Be Used For The Measurement Of Temperature And State Examples Of Such Properties, Including The Density Of A Liquid, Volume Of A Gas At Constant Pressure, Resistance Of A Metal, E.m.f. Of A Thermocouple
- 11.23Temperature: Temperature Scales: Understand That The Scale Of Thermodynamic Temperature Does Not Depend On The Property Of Any Particular Substance
- 11.24Temperature: Temperature Scales: Convert Temperatures Between Kelvin And Degrees Celsius And Recall That T/k = Θ/ °c + 273.15
- 11.25Temperature: Temperature Scales: Understand That The Lowest Possible Temperature Is Zero Kelvin On The Thermodynamic Temperature Scale And That This Is Known As Absolute Zero
- 11.26Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Heat Capacity
- 11.27Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Latent Heat And Distinguish Between Specific Latent Heat Of Fusion And Specific Latent Heat Of Vaporisation
- 11.28Ideal Gases: The Mole: Understand That Amount Of Substance Is An Si Base Quantity With The Base Unit Mol
- 11.29Ideal Gases: The Mole: Use Molar Quantities Where One Mole Of Any Substance Is The Amount Containing A Number Of Particles Of That Substance Equal To The Avogadro Constant Na
- 11.30Ideal Gases: Equation Of State: Understand That A Gas Obeying Pv ∝ T, Where T Is The Thermodynamic Temperature, Is Known As An Ideal Gas
- 11.31Ideal Gases: Equation Of State: Recall And Use The Equation Of State For An Ideal Gas Expressed As Pv = Nrt, Where N = Amount Of Substance (Number Of Moles) And As Pv = Nkt, Where N = Number Of Molecules
- 11.32Ideal Gases: Equation Of State: Recall That The Boltzmann Constant K Is Given By K = R/na
- 11.33Ideal Gases: Kinetic Theory Of Gases: State The Basic Assumptions Of The Kinetic Theory Of Gases
- 11.34Ideal Gases: Kinetic Theory Of Gases: Explain How Molecular Movement Causes The Pressure Exerted By A Gas And Derive And Use The Relationship Pv = 3 1 Nm, Where Is The Mean-square Speed (A Simple Model Considering One-dimensional Collisions And Then Extending To Three Dimensions Using 3 1 = Is Sufficient)
- 11.35Ideal Gases: Kinetic Theory Of Gases: Understand That The Root-mean-square Speed Cr.m.s. Is Given By C 2
- 11.36Ideal Gases: Kinetic Theory Of Gases: Compare Pv = 3 1 Nm With Pv = Nkt To Deduce That The Average Translational Kinetic Energy Of A Molecule Is 2 3 Kt, And Recall And Use This Expression
- 11.37Thermodynamics: Internal Energy: Understand That Internal Energy Is Determined By The State Of The System And That It Can Be Expressed As The Sum Of A Random Distribution Of Kinetic And Potential Energies Associated With The Molecules Of A System
- 11.38Thermodynamics: Internal Energy: Relate A Rise In Temperature Of An Object To An Increase In Its Internal Energy
- 11.39Thermodynamics: The First Law Of Thermodynamics: Recall And Use W = P∆v For The Work Done When The Volume Of A Gas Changes At Constant Pressure And Understand The Difference Between The Work Done By The Gas And The Work Done On The Gas
- 11.40Thermodynamics: The First Law Of Thermodynamics: Recall And Use The First Law Of Thermodynamics ∆u = Q + W Expressed In Terms Of The Increase In Internal Energy, The Heating Of The System (Energy Transferred To The System By Heating) And The Work Done On The System
- 11.41Oscillations: Simple Harmonic Oscillations: Understand And Use The Terms Displacement, Amplitude, Period, Frequency, Angular Frequency And Phase Difference In The Context Of Oscillations, And Express The Period In Terms Of Both Frequency And Angular Frequency
- 11.42Oscillations: Simple Harmonic Oscillations: Understand That Simple Harmonic Motion Occurs When Acceleration Is Proportional To Displacement From A Fixed Point And In The Opposite Direction
- 11.43Oscillations: Simple Harmonic Oscillations: Use A = –ω2 X And Recall And Use, As A Solution To This Equation, X = X0 Sin Ωt
- 11.44Oscillations: Simple Harmonic Oscillations: Use The Equations V = V0 Cos Ωt And V = ±ω ( ) X X 0 2 2 −
- 11.45Oscillations: Simple Harmonic Oscillations: Analyse And Interpret Graphical Representations Of The Variations Of Displacement, Velocity And Acceleration For Simple Harmonic Motion
- 11.46Oscillations: Energy In Simple Harmonic Motion: Describe The Interchange Between Kinetic And Potential Energy During Simple Harmonic Motion
- 11.47Oscillations: Energy In Simple Harmonic Motion: Recall And Use E = 2 1 Mω2 X0 2 For The Total Energy Of A System Undergoing Simple Harmonic Motion
- 11.48Oscillations: Damped And Forced Oscillations, Resonance: Understand That A Resistive Force Acting On An Oscillating System Causes Damping
- 11.49Oscillations: Damped And Forced Oscillations, Resonance: Understand And Use The Terms Light, Critical And Heavy Damping And Sketch Displacement–time Graphs Illustrating These Types Of Damping
- 11.50Oscillations: Damped And Forced Oscillations, Resonance: Understand That Resonance Involves A Maximum Amplitude Of Oscillations And That This Occurs When An Oscillating System Is Forced To Oscillate At Its Natural Frequency
- 11.51Electric Fields: Electric Fields And Field Lines: Understand That An Electric Field Is An Example Of A Field Of Force And Define Electric Field As Force Per Unit Positive Charge
- 11.52Electric Fields: Electric Fields And Field Lines: Recall And Use F = Qe For The Force On A Charge In An Electric Field
- 11.53Electric Fields: Electric Fields And Field Lines: Represent An Electric Field By Means Of Field Lines
- 11.54Electric Fields: Uniform Electric Fields: Recall And Use E = ∆v/∆d To Calculate The Field Strength Of The Uniform Field Between Charged Parallel Plates
- 11.55Electric Fields: Uniform Electric Fields: Describe The Effect Of A Uniform Electric Field On The Motion Of Charged Particles
- 11.56Electric Fields: Electric Force Between Point Charges: Understand That, For A Point Outside A Spherical Conductor, The Charge On The Sphere May Be Considered To Be A Point Charge At Its Centre
- 11.57Electric Fields: Electric Force Between Point Charges: Recall And Use Coulomb’s Law F = Q1q2 /(4πε0r 2 ) For The Force Between Two Point Charges In Free Space
- 11.58Electric Fields: Electric Field Of A Point Charge: Recall And Use E = Q/(4πε0r 2 ) For The Electric Field Strength Due To A Point Charge In Free Space
- 11.59Electric Fields: Electric Potential: Define Electric Potential At A Point As The Work Done Per Unit Positive Charge In Bringing A Small Test Charge From Infinity To The Point
- 11.60Electric Fields: Electric Potential: Recall And Use The Fact That The Electric Field At A Point Is Equal To The Negative Of Potential Gradient At That Point
- 11.61Electric Fields: Electric Potential: Use V = Q/(4πε0r) For The Electric Potential In The Field Due To A Point Charge
- 11.62Electric Fields: Electric Potential: Understand How The Concept Of Electric Potential Leads To The Electric Potential Energy Of Two Point Charges And Use Ep = Qq/(4πε0r)
- 11.63Capacitance: Capacitors And Capacitance: Define Capacitance, As Applied To Both Isolated Spherical Conductors And To Parallel Plate Capacitors
- 11.64Capacitance: Capacitors And Capacitance: Recall And Use C = Q/v
- 11.65Capacitance: Capacitors And Capacitance: v
- 11.66Capacitance: Capacitors And Capacitance: Use The Capacitance Formulae For Capacitors In Series And In Parallel
- 11.67Capacitance: Energy Stored In A Capacitor: Determine The Electric Potential Energy Stored In A Capacitor From The Area Under The Potential–charge Graph
- 11.68Capacitance: Energy Stored In A Capacitor: Recall And Use W = 2 1 Qv = 2 1 Cv2
- 11.69Capacitance: Discharging A Capacitor: Analyse Graphs Of The Variation With Time Of Potential Difference, Charge And Current For A Capacitor Discharging Through A Resistor
- 11.70Capacitance: Discharging A Capacitor:Recall And Use Τ = Rc For The Time Constant For A Capacitor Discharging Through A Resistor
- 11.71Capacitance: Discharging A Capacitor: Use Equations Of The Form X = X0 E–(T/rc) Where X Could Represent Current, Charge Or Potential Difference For A Capacitor Discharging Through A Resistor
- 11.72Magnetic Fields: Concept Of A Magnetic Field: Understand That A Magnetic Field Is An Example Of A Field Of Force Produced Either By Moving Charges Or By Permanent Magnets
- 11.73Magnetic Fields: Concept Of A Magnetic Field: Represent A Magnetic Field By Field Lines
- 11.74Magnetic Fields: Force On A Current-carrying Conductor: Understand That A Force Might Act On A Current-carrying Conductor Placed In A Magnetic Field
- 11.75Magnetic Fields: Force On A Current-carrying Conductor: Recall And Use The Equation F = Bil Sin Θ, With Directions As Interpreted By Fleming’s Left-hand Rule
- 11.76Magnetic Fields: Force On A Current-carrying Conductor: Define Magnetic Flux Density As The Force Acting Per Unit Current Per Unit Length On A Wire Placed At Rightangles To The Magnetic Field
- 11.77Magnetic Fields: Force On A Moving Charge: Determine The Direction Of The Force On A Charge Moving In A Magnetic Field
- 11.78Magnetic Fields: Force On A Moving Charge: Recall And Use F = Bqv Sin Θ
- 11.79Magnetic Fields: Force On A Moving Charge: Understand The Origin Of The Hall Voltage And Derive And Use The Expression Vh = Bi /(Ntq), Where T = Thickness
- 11.80Magnetic Fields: Force On A Moving Charge: Understand The Use Of A Hall Probe To Measure Magnetic Flux Density
- 11.81Magnetic Fields: Force On A Moving Charge: Describe The Motion Of A Charged Particle Moving In A Uniform Magnetic Field Perpendicular To The Direction Of Motion Of The Particle
- 11.82Magnetic Fields: Force On A Moving Charge: Explain How Electric And Magnetic Fields Can Be Used In Velocity Selection
- 11.83Magnetic Fields: Magnetic Fields Due To Currents: Sketch Magnetic Field Patterns Due To The Currents In A Long Straight Wire, A Flat Circular Coil And A Long Solenoid
- 11.84Magnetic Fields: Magnetic Fields Due To Currents: Understand That The Magnetic Field Due To The Current In A Solenoid Is Increased By A Ferrous Core
- 11.85Magnetic Fields: Magnetic Fields Due To Currents: Explain The Origin Of The Forces Between Current-carrying Conductors And Determine The Direction Of The Forces
- 11.86Magnetic Fields: Electromagnetic Induction: Define Magnetic Flux As The Product Of The Magnetic Flux Density And The Cross-sectional Area Perpendicular To The Direction Of The Magnetic Flux Density
- 11.87Magnetic Fields: Electromagnetic Induction: Recall And Use Φ = Ba
- 11.88Magnetic Fields: Electromagnetic Induction: Understand And Use The Concept Of Magnetic Flux Linkage
- 11.89Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That A Changing Magnetic Flux Can Induce An E.m.f. In A Circuit
- 11.90Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That The Induced E.m.f. Is In Such A Direction As To Oppose The Change Producing It
- 11.91Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: The Factors Affecting The Magnitude Of The Induced E.m.f.
- 11.92Magnetic Fields: Electromagnetic Induction: Recall And Use Faraday’s And Lenz’s Laws Of Electromagnetic Induction
- 11.93Alternating Currents: Characteristics Of Alternating Currents: Understand And Use The Terms Period, Frequency And Peak Value As Applied To An Alternating Current Or Voltage
- 11.94Alternating Currents: Characteristics Of Alternating Currents: Use Equations Of The Form X = X0 Sin Ωt Representing A Sinusoidally Alternating Current Or Voltage
- 11.95Alternating Currents: Characteristics Of Alternating Currents: Recall And Use The Fact That The Mean Power In A Resistive Load Is Half The Maximum Power For A Sinusoidal Alternating Current
- 11.96Alternating Currents: Characteristics Of Alternating Currents: Distinguish Between Root-mean-square (R.m.s.) And Peak Values And Recall And Use I R.m.s. = I0 / 2 And Vr.m.s. = V0 / 2 For A Sinusoidal Alternating Current
- 11.97Alternating Currents: Rectification And Smoothing: Distinguish Graphically Between Half-wave And Full-wave Rectification
- 11.98Alternating Currents: Rectification And Smoothing: Explain The Use Of A Single Diode For The Half-wave Rectification Of An Alternating Current
- 11.99Alternating Currents: Rectification And Smoothing: Explain The Use Of Four Diodes (Bridge Rectifier) For The Full-wave Rectification Of An Alternating Current
- 11.100Alternating Currents: Rectification And Smoothing: Analyse The Effect Of A Single Capacitor In Smoothing, Including The Effect Of The Values Of Capacitance And The Load Resistance
- 11.101Quantum Physics: Energy And Momentum Of A Photon: Understand That Electromagnetic Radiation Has A Particulate Nature
- 11.102Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Is A Quantum Of Electromagnetic Energy
- 11.103Quantum Physics: Energy And Momentum Of A Photon: Recall And Use E = Hf
- 11.104Quantum Physics: Energy And Momentum Of A Photon: Use The Electronvolt (Ev) As A Unit Of Energy
- 11.105Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Has Momentum And That The Momentum Is Given By P = E/c
- 11.106Quantum Physics: Photoelectric Effect: Understand That Photoelectrons May Be Emitted From A Metal Surface When It Is Illuminated By Electromagnetic Radiation
- 11.107Quantum Physics: Photoelectric Effect: Understand And Use The Terms Threshold Frequency And Threshold Wavelength
- 11.108Quantum Physics: Photoelectric Effect: Explain Photoelectric Emission In Terms Of Photon Energy And Work Function Energy
- 11.109Quantum Physics: Photoelectric Effect: Recall And Use Hf = Φ + 2 1 Mvmax 2
- 11.110Quantum Physics: Photoelectric Effect: Explain Why The Maximum Kinetic Energy Of Photoelectrons Is Independent Of Intensity, Whereas The Photoelectric Current Is Proportional To Intensity
- 11.111Quantum Physics: Wave-particle Duality: Understand That The Photoelectric Effect Provides Evidence For A Particulate Nature Of Electromagnetic Radiation While Phenomena Such As Interference And Diffraction Provide Evidence For A Wave Nature
- 11.112Quantum Physics: Wave-particle Duality: Describe And Interpret Qualitatively The Evidence Provided By Electron Diffraction For The Wave Nature Of Particles
- 11.113Quantum Physics: Wave-particle Duality: Understand The De Broglie Wavelength As The Wavelength Associated With A Moving Particle
- 11.114Quantum Physics: Wave-particle Duality: Recall And Use Λ = H/p
- 11.115Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand That There Are Discrete Electron Energy Levels In Isolated Atoms (E.g. Atomic Hydrogen)
- 11.116Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand The Appearance And Formation Of Emission And Absorption Line Spectra
- 11.117Quantum Physics: Energy Levels In Atoms And Line Spectra: Recall And Use Hf = E1 – E2
- 11.118Nuclear Physics: Mass Defect And Nuclear Binding Energy: Understand The Equivalence Between Energy And Mass As Represented By E = Mc2 And Recall And Use This Equation
- 11.119Nuclear Physics: Mass Defect And Nuclear Binding Energy: Represent Simple Nuclear Reactions By Nuclear Equations Of The Form 7n He O H 14 2 4 8 17 1 1 + + “
- 11.120Nuclear Physics: Mass Defect And Nuclear Binding Energy: Define And Use The Terms Mass Defect And Binding Energy
- 11.121Nuclear Physics: Mass Defect And Nuclear Binding Energy: Sketch The Variation Of Binding Energy Per Nucleon With Nucleon Number
- 11.122Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain What Is Meant By Nuclear Fusion And Nuclear Fission
- 11.123Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain The Relevance Of Binding Energy Per Nucleon To Nuclear Reactions, Including Nuclear Fusion And Nuclear Fission
- 11.124Nuclear Physics: Mass Defect And Nuclear Binding Energy: Calculate The Energy Released In Nuclear Reactions Using E = C2 ∆m
- 11.125Nuclear Physics: Radioactive Decay: Understand That Fluctuations In Count Rate Provide Evidence For The Random Nature Of Radioactive Decay
- 11.126Nuclear Physics: Radioactive Decay: Understand That Radioactive Decay Is Both Spontaneous And Random
- 11.127Nuclear Physics: Radioactive Decay: Define Activity And Decay Constant, And Recall And Use A = Λn
- 11.128Nuclear Physics: Radioactive Decay: Define Half-life
- 11.129Nuclear Physics: Radioactive Decay: Use Λ = 0.693/t 2 1
- 11.130Nuclear Physics: Radioactive Decay: Understand The Exponential Nature Of Radioactive Decay, And Sketch And Use The Relationship X = X0e–λt , Where X Could Represent Activity, Number Of Undecayed Nuclei Or Received Count Rate
- 11.131Medical Physics: Production And Use Of Ultrasound: Understand That A Piezo-electric Crystal Changes Shape When A P.d. Is Applied Across It And That The Crystal Generates An E.m.f. When Its Shape Changes
- 11.132Medical Physics: Production And Use Understand How Ultrasound Waves Are Generated And Detected By A Piezoelectric TransducerOf Ultrasound:
- 11.133Medical Physics: Production And Use Of Ultrasound: Understand How The Reflection Of Pulses Of Ultrasound At Boundaries Between Tissues Can Be Used To Obtain Diagnostic Information About Internal Structures
- 11.134Medical Physics: Production And Use Of Ultrasound: Define The Specific Acoustic Impedance Of A Medium As Z = Ρc, Where C Is The Speed Of Sound In The Medium
- 11.135Medical Physics: Production And Use Of Ultrasound: Use Ir / I0 = (Z1 – Z2) 2 /(Z1 + Z2) 2 For The Intensity Reflection Coefficient Of A Boundary Between Two Media
- 11.136Medical Physics: Production And Use Of Ultrasound: Recall And Use I = I0e–μx For The Attenuation Of Ultrasound In Matter
- 11.137Medical Physics: Production And Use Of X-rays: Explain That X-rays Are Produced By Electron Bombardment Of A Metal Target And Calculate The Minimum Wavelength Of X-rays Produced From The Accelerating P.d.
- 11.138Medical Physics: Production And Use Of X-rays: Understand The Use Of X-rays In Imaging Internal Body Structures, Including An Understanding Of The Term Contrast In X-ray Imaging
- 11.139Medical Physics: Production And Use Of X-rays: Recall And Use I = I0e–μx For The Attenuation Of X-rays In Matter
- 11.140Medical Physics: Production And Use Of X-rays: Understand That Computed Tomography (Ct) Scanning Produces A 3d Image Of An Internal Structure By First Combining Multiple X-ray Images Taken In The Same Section From Different Angles To Obtain A 2d Image Of The Section, Then Repeating This Process Along An Axis And Combining 2d Images Of Multiple Sections
- 11.141Medical Physics: Pet Scanning: Recall That A Tracer That Decays By Β+ Decay Is Used In Positron Emission Tomography (Pet Scanning)
- 11.142Medical Physics: Pet Scanning: Understand That Annihilation Occurs When A Particle Interacts With Its Antiparticle And That Mass–energy And Momentum Are Conserved In The Process
- 11.143Medical Physics: Pet Scanning: Explain That, In Pet Scanning, Positrons Emitted By The Decay Of The Tracer Annihilate When They Interact With Electrons In The Tissue, Producing A Pair Of Gamma-ray Photons Travelling In Opposite Directions
- 11.144Medical Physics: Pet Scanning: Calculate The Energy Of The Gamma-ray Photons Emitted During The Annihilation Of An Electron-positron Pair
- 11.145Medical Physics: Pet Scanning: Understand That The Gamma-ray Photons From An Annihilation Event Travel Outside The Body And Can Be Detected, And An Image Of The Tracer Concentration In The Tissue Can Be Created By Processing The Arrival Times Of The Gamma-ray Photons
- 11.146Astronomy And Cosmology: Standard Candles: Understand The Term Luminosity As The Total Power Of Radiation Emitted By A Star
- 11.147Astronomy And Cosmology: Standard Candles: Recall And Use The Inverse Square Law For Radiant Flux Intensity F In Terms Of The Luminosity L Of The Source F = L/(4πd2 )
- 11.148Astronomy And Cosmology: Standard Candles: Understand That An Object Of Known Luminosity Is Called A Standard Candle
- 11.149Astronomy And Cosmology: Standard Candles: Understand The Use Of Standard Candles To Determine Distances To Galaxies
- 11.150Astronomy And Cosmology: Stellar Radii: Recall And Use Wien’s Displacement Law Λmax ∝ 1/t To Estimate The Peak Surface Temperature Of A Star
- 11.151Astronomy And Cosmology: Stellar Radii: Use The Stefan–boltzmann Law L = 4πσr 2 T4
- 11.152Astronomy And Cosmology: Stellar Radii: Use Wien’s Displacement Law And The Stefan–boltzmann Law To Estimate The Radius Of A Star
- 11.153Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Understand That The Lines In The Emission And Absorption Spectra From Distant Objects Show An Increase In Wavelength From Their Known Values
- 11.154Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Use ∆λ / Λ . ∆f/f . V /c For The Redshift Of Electromagnetic Radiation From A Source Moving Relative To An Observer
- 11.155Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Explain Why Redshift Leads To The Idea That The Universe Is Expanding
- 11.156Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Recall And Use Hubble’s Law V . H0d And Explain How This Leads To The Big Bang Theory (Candidates Will Only Be Required To Use Si Units)
- Notes (Rearranged Version)Notes Arranged In A Different Style For Preparation Ease15
- Videos Lectures (Pre-Recorded)Videos Recorded In A Different Style For Preparation Ease0
- Paper 5 Skills / Formulae Sheet50
- 14.1Formulae Sheet: Circular Motion: Radian Measure And Angular Displacement Formulae
- 14.2Formulae Sheet: Circular Motion: Angular Speed And Period Relationships
- 14.3Formulae Sheet: Circular Motion: Linear Speed In Circular Motion
- 14.4Formulae Sheet: Circular Motion: Centripetal Acceleration Formulae
- 14.5Formulae Sheet: Circular Motion: Centripetal Force Formulae
- 14.6Formulae Sheet: Gravitational Fields: Newton’s Law Of Gravitation Formulae
- 14.7Formulae Sheet: Gravitational Fields: Gravitational Field Strength Due To A Point Mass
- 14.8Formulae Sheet: Gravitational Fields: Variation Of Gravitational Field Strength With Distance
- 14.9Formulae Sheet: Gravitational Fields: Gravitational Potential Formulae
- 14.10Formulae Sheet: Gravitational Fields: Gravitational Potential Energy Formulae
- 14.11Formulae Sheet: Gravitational Fields: Orbital Motion And Satellite Speed Formulae
- 14.12Formulae Sheet: Gravitational Fields: Geostationary Orbit Conditions And Formulae
- 14.13Formulae Sheet: Thermal Physics: Temperature Conversion Formulae (Kelvin–Celsius)
- 14.14Formulae Sheet: Thermal Physics: Specific Heat Capacity Formulae
- 14.15Formulae Sheet: Thermal Physics: Specific Latent Heat Formulae
- 14.16Formulae Sheet: Ideal Gases: Ideal Gas Equation Using Amount Of Substance
- 14.17Formulae Sheet: Ideal Gases: Ideal Gas Equation Using Molecular Form
- 14.18Formulae Sheet: Ideal Gases: Relationship Between Gas Constants R, k And Nₐ
- 14.19Formulae Sheet: Ideal Gases: Root Mean Square Speed Formula
- 14.20Formulae Sheet: Ideal Gases: Mean Translational Kinetic Energy Formula
- 14.21Formulae Sheet: Thermodynamics: Internal Energy Change Formulae
- 14.22Formulae Sheet: Thermodynamics: Work Done By A Gas At Constant Pressure
- 14.23Formulae Sheet: Thermodynamics: First Law Of Thermodynamics Formula
- 14.24Formulae Sheet: Oscillations (SHM): Angular Frequency And Period Relationships
- 14.25Formulae Sheet: Oscillations (SHM): SHM Acceleration Formula
- 14.26Formulae Sheet: Oscillations (SHM): SHM Displacement Equation
- 14.27Formulae Sheet: Oscillations (SHM): SHM Velocity Formulae
- 14.28Formulae Sheet: Oscillations (SHM): Maximum Velocity And Maximum Acceleration Formulae
- 14.29Formulae Sheet: Oscillations (SHM): Total Energy Of SHM System
- 14.30Formulae Sheet: Oscillations (SHM): Energy Distribution Formulae In SHM
- 14.31Formulae Sheet: Electric Fields: Electric Field Strength Definition Formula
- 14.32Formulae Sheet: Electric Fields: Uniform Electric Field Between Parallel Plates
- 14.33Formulae Sheet: Electric Fields: Force On A Charge In An Electric Field
- 14.34Formulae Sheet: Electric Fields: Coulomb’s Law Formula
- 14.35Formulae Sheet: Electric Fields: Electric Field Strength Of A Point Charge
- 14.36Formulae Sheet: Electric Fields: Electric Potential Formula
- 14.37Formulae Sheet: Electric Fields: Electric Potential Energy Formula
- 14.38Formulae Sheet: Electric Fields: Relationship Between Electric Field And Potential Gradient
- 14.39Formulae Sheet: Capacitance: Capacitance Definition Formula
- 14.40Formulae Sheet: Capacitance: Capacitance Of Capacitors In Series
- 14.41Formulae Sheet: Capacitance: Capacitance Of Capacitors In Parallel
- 14.42Formulae Sheet: Capacitance: Energy Stored In A Capacitor Formula
- 14.43Formulae Sheet: Capacitance: Capacitor Discharge Time Constant
- 14.44Formulae Sheet: Capacitance: Exponential Decay Equations For Discharging Capacitors
- 14.45Formulae Sheet: Magnetic Fields & Electromagnetism: Force On A Current-Carrying Conductor Formula
- 14.46Formulae Sheet: Magnetic Fields & Electromagnetism: Magnetic Flux And Flux Linkage Formulae
- 14.47Formulae Sheet: Magnetic Fields & Electromagnetism: Induced EMF Using Faraday’s Law
- 14.48Formulae Sheet: Magnetic Fields & Electromagnetism: Motion Of Charged Particles In Magnetic Fields Formulae
- 14.49Formulae Sheet: Alternating Currents: RMS And Peak Value Relationships For AC
- 14.50Formulae Sheet: Alternating Currents: Mean Power Formula For Sinusoidal Alternating Currents
- Practice Questions/ Practice ExamsPractice Questions/ Exams Based Both On Actual Exam Pattern And On Topical Content To Boost Preparation And Improve Performance157
- 15.1Practice Questions: Motion In A Circle: Kinematics Of Uniform Circular Motion: Define The Radian And Express Angular Displacement In Radians
- 15.2Practice Questions: Motion In A Circle: Kinematics Of Uniform Circular Motion: Understand And Use The Concept Of Angular Speed
- 15.3Practice Questions: Motion In A Circle: Kinematics Of Uniform Circular Motion: Recall And Use Ω = 2π/t And V = Rω
- 15.4Practice Questions: Motion In A Circle: Centripetal Acceleration: Understand That A Force Of Constant Magnitude That Is Always Perpendicular To The Direction Of Motion Causes Centripetal Acceleration
- 15.5Practice Questions: Motion In A Circle: Centripetal Acceleration: Understand That Centripetal Acceleration Causes Circular Motion With A Constant Angular Speed
- 15.6Practice Questions: Motion In A Circle: Centripetal Acceleration: Recall And Use A = Rω2 And A = V2 /r
- 15.7Practice Questions: Motion In A Circle: Centripetal Acceleration: Recall And Use F = Mrω2 And F = Mv2 /r
- 15.8Practice Questions: Gravitational Fields: Gravitational Field: Understand That A Gravitational Field Is An Example Of A Field Of Force And Define Gravitational Field As Force Per Unit Mass
- 15.9Practice Questions: Gravitational Fields: Gravitational Field: Represent A Gravitational Field By Means Of Field Lines
- 15.10Practice Questions: Gravitational Fields: Gravitational Force Between Point Masses: Understand That, For A Point Outside A Uniform Sphere, The Mass Of The Sphere May Be Considered To Be A Point Mass At Its Centre
- 15.11Practice Questions: Gravitational Fields: Gravitational Force Between Point Masses: Recall And Use Newton’s Law Of Gravitation F = Gm1m2 /r 2 For The Force Between Two Point Masses
- 15.12Practice Questions: Gravitational Fields: Gravitational Force Between Point Masses: Analyse Circular Orbits In Gravitational Fields By Relating The Gravitational Force To The Centripetal Acceleration It Causes
- 15.13Practice Questions: Gravitational Fields: Gravitational Force Between Point Masses: Understand That A Satellite In A Geostationary Orbit Remains At The Same Point Above The Earth’s Surface, With An Orbital Period Of 24 Hours, Orbiting From West To East, Directly Above The Equator
- 15.14Practice Questions: Gravitational Fields: Gravitational Field Of A Point Mass: Derive, From Newton’s Law Of Gravitation And The Definition Of Gravitational Field, The Equation G = Gm/r 2 For The Gravitational Field Strength Due To A Point Mass
- 15.15Practice Questions: Gravitational Fields: Gravitational Field Of A Point Mass: Recall And Use G = Gm/r 2
- 15.16Practice Questions: Gravitational Fields: Gravitational Field Of A Point Mass: Understand Why G Is Approximately Constant For Small Changes In Height Near The Earth’s Surface
- 15.17Practice Questions: Gravitational Fields: Gravitational Potential: Define Gravitational Potential At A Point As The Work Done Per Unit Mass In Bringing A Small Test Mass From Infinity To The Point
- 15.18Practice Questions: Gravitational Fields: Gravitational Potential: Use Φ = –gm/r For The Gravitational Potential In The Field Due To A Point Mass
- 15.19Practice Questions: Gravitational Fields: Gravitational Potential: Understand How The Concept Of Gravitational Potential Leads To The Gravitational Potential Energy Of Two Point Masses And Use Ep = –gmm/r
- 15.20Practice Questions: Temperature: Thermal Equilibrium: Understand That (Thermal) Energy Is Transferred From A Region Of Higher Temperature To A Region Of Lower Temperature
- 15.21Practice Questions: Temperature: Thermal Equilibrium: Understand That Regions Of Equal Temperature Are In Thermal Equilibrium
- 15.22Practice Questions: Temperature: Temperature Scales: Understand That A Physical Property That Varies With Temperature May Be Used For The Measurement Of Temperature And State Examples Of Such Properties, Including The Density Of A Liquid, Volume Of A Gas At Constant Pressure, Resistance Of A Metal, E.m.f. Of A Thermocouple
- 15.23Practice Questions: Temperature: Temperature Scales: Understand That The Scale Of Thermodynamic Temperature Does Not Depend On The Property Of Any Particular Substance
- 15.24Practice Questions: Temperature: Temperature Scales: Convert Temperatures Between Kelvin And Degrees Celsius And Recall That T/k = Θ/ °c + 273.15
- 15.25Practice Questions: Temperature: Temperature Scales: Understand That The Lowest Possible Temperature Is Zero Kelvin On The Thermodynamic Temperature Scale And That This Is Known As Absolute Zero
- 15.26Practice Questions: Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Heat Capacity
- 15.27Practice Questions: Temperature: Specific Heat Capacity And Specific Latent Heat: Define And Use Specific Latent Heat And Distinguish Between Specific Latent Heat Of Fusion And Specific Latent Heat Of Vaporisation
- 15.28Practice Questions: Ideal Gases: The Mole: Understand That Amount Of Substance Is An Si Base Quantity With The Base Unit Mol
- 15.29Practice Questions: Ideal Gases: The Mole: Use Molar Quantities Where One Mole Of Any Substance Is The Amount Containing A Number Of Particles Of That Substance Equal To The Avogadro Constant Na
- 15.30Practice Questions: Ideal Gases: Equation Of State: Understand That A Gas Obeying Pv ∝ T, Where T Is The Thermodynamic Temperature, Is Known As An Ideal Gas
- 15.31Practice Questions: Ideal Gases: Equation Of State: Recall And Use The Equation Of State For An Ideal Gas Expressed As Pv = Nrt, Where N = Amount Of Substance (Number Of Moles) And As Pv = Nkt, Where N = Number Of Molecules
- 15.32Practice Questions: Ideal Gases: Equation Of State: Recall That The Boltzmann Constant K Is Given By K = R/na
- 15.33Practice Questions: Ideal Gases: Kinetic Theory Of Gases: State The Basic Assumptions Of The Kinetic Theory Of Gases
- 15.34Practice Questions: Ideal Gases: Kinetic Theory Of Gases: Explain How Molecular Movement Causes The Pressure Exerted By A Gas And Derive And Use The Relationship Pv = 3 1 Nm, Where Is The Mean-square Speed (A Simple Model Considering One-dimensional Collisions And Then Extending To Three Dimensions Using 3 1 = Is Sufficient)
- 15.35Practice Questions: Ideal Gases: Kinetic Theory Of Gases: Understand That The Root-mean-square Speed Cr.m.s. Is Given By C 2
- 15.36Practice Questions: Ideal Gases: Kinetic Theory Of Gases: Compare Pv = 3 1 Nm With Pv = Nkt To Deduce That The Average Translational Kinetic Energy Of A Molecule Is 2 3 Kt, And Recall And Use This Expression
- 15.37Practice Questions: Thermodynamics: Internal Energy: Understand That Internal Energy Is Determined By The State Of The System And That It Can Be Expressed As The Sum Of A Random Distribution Of Kinetic And Potential Energies Associated With The Molecules Of A System
- 15.38Practice Questions: Thermodynamics: Internal Energy: Relate A Rise In Temperature Of An Object To An Increase In Its Internal Energy
- 15.39Practice Questions: Thermodynamics: The First Law Of Thermodynamics: Recall And Use W = P∆v For The Work Done When The Volume Of A Gas Changes At Constant Pressure And Understand The Difference Between The Work Done By The Gas And The Work Done On The Gas
- 15.40Practice Questions: Thermodynamics: The First Law Of Thermodynamics: Recall And Use The First Law Of Thermodynamics ∆u = Q + W Expressed In Terms Of The Increase In Internal Energy, The Heating Of The System (Energy Transferred To The System By Heating) And The Work Done On The System
- 15.41Practice Questions: Oscillations: Simple Harmonic Oscillations: Understand And Use The Terms Displacement, Amplitude, Period, Frequency, Angular Frequency And Phase Difference In The Context Of Oscillations, And Express The Period In Terms Of Both Frequency And Angular Frequency
- 15.42Practice Questions: Oscillations: Simple Harmonic Oscillations: Understand That Simple Harmonic Motion Occurs When Acceleration Is Proportional To Displacement From A Fixed Point And In The Opposite Direction
- 15.43Practice Questions: Oscillations: Simple Harmonic Oscillations: Use A = –ω2 X And Recall And Use, As A Solution To This Equation, X = X0 Sin Ωt
- 15.44Practice Questions: Oscillations: Simple Harmonic Oscillations: Use The Equations V = V0 Cos Ωt And V = ±ω ( ) X X 0 2 2 −
- 15.45Practice Questions: Oscillations: Simple Harmonic Oscillations: Analyse And Interpret Graphical Representations Of The Variations Of Displacement, Velocity And Acceleration For Simple Harmonic Motion
- 15.46Practice Questions: Oscillations: Energy In Simple Harmonic Motion: Describe The Interchange Between Kinetic And Potential Energy During Simple Harmonic Motion
- 15.47Practice Questions: Oscillations: Energy In Simple Harmonic Motion: Recall And Use E = 2 1 Mω2 X0 2 For The Total Energy Of A System Undergoing Simple Harmonic Motion
- 15.48Practice Questions: Oscillations: Damped And Forced Oscillations, Resonance: Understand That A Resistive Force Acting On An Oscillating System Causes Damping
- 15.49Practice Questions: Oscillations: Damped And Forced Oscillations, Resonance: Understand And Use The Terms Light, Critical And Heavy Damping And Sketch Displacement–time Graphs Illustrating These Types Of Damping
- 15.50Practice Questions: Oscillations: Damped And Forced Oscillations, Resonance: Understand That Resonance Involves A Maximum Amplitude Of Oscillations And That This Occurs When An Oscillating System Is Forced To Oscillate At Its Natural Frequency
- 15.51Practice Questions: Electric Fields: Electric Fields And Field Lines: Understand That An Electric Field Is An Example Of A Field Of Force And Define Electric Field As Force Per Unit Positive Charge
- 15.52Practice Questions: Electric Fields: Electric Fields And Field Lines: Recall And Use F = Qe For The Force On A Charge In An Electric Field
- 15.53Practice Questions: Electric Fields: Electric Fields And Field Lines: Represent An Electric Field By Means Of Field Lines
- 15.54Practice Questions: Electric Fields: Uniform Electric Fields: Recall And Use E = ∆v/∆d To Calculate The Field Strength Of The Uniform Field Between Charged Parallel Plates
- 15.55Practice Questions: Electric Fields: Uniform Electric Fields: Describe The Effect Of A Uniform Electric Field On The Motion Of Charged Particles
- 15.56Practice Questions: Electric Fields: Electric Force Between Point Charges: Understand That, For A Point Outside A Spherical Conductor, The Charge On The Sphere May Be Considered To Be A Point Charge At Its Centre
- 15.57Practice Questions: Electric Fields: Electric Force Between Point Charges: Recall And Use Coulomb’s Law F = Q1q2 /(4πε0r 2 ) For The Force Between Two Point Charges In Free Space
- 15.58Practice Questions: Electric Fields: Electric Field Of A Point Charge: Recall And Use E = Q/(4πε0r 2 ) For The Electric Field Strength Due To A Point Charge In Free Space
- 15.59Practice Questions: Electric Fields: Electric Potential: Define Electric Potential At A Point As The Work Done Per Unit Positive Charge In Bringing A Small Test Charge From Infinity To The Point
- 15.60Practice Questions: Electric Fields: Electric Potential: Recall And Use The Fact That The Electric Field At A Point Is Equal To The Negative Of Potential Gradient At That Point
- 15.61Practice Questions: Electric Fields: Electric Potential: Use V = Q/(4πε0r) For The Electric Potential In The Field Due To A Point Charge
- 15.62Practice Questions: Electric Fields: Electric Potential: Understand How The Concept Of Electric Potential Leads To The Electric Potential Energy Of Two Point Charges And Use Ep = Qq/(4πε0r)
- 15.63Practice Questions: Capacitance: Capacitors And Capacitance: Define Capacitance, As Applied To Both Isolated Spherical Conductors And To Parallel Plate Capacitors
- 15.64Practice Questions: Capacitance: Capacitors And Capacitance: Recall And Use C = Q/v
- 15.65Practice Questions: Capacitance: Capacitors And Capacitance: v
- 15.66Practice Questions: Capacitance: Capacitors And Capacitance: Use The Capacitance Formulae For Capacitors In Series And In Parallel
- 15.67Practice Questions: Capacitance: Energy Stored In A Capacitor: Determine The Electric Potential Energy Stored In A Capacitor From The Area Under The Potential–charge Graph
- 15.68Practice Questions: Capacitance: Energy Stored In A Capacitor: Recall And Use W = 2 1 Qv = 2 1 Cv2
- 15.69Practice Questions: Capacitance: Discharging A Capacitor: Analyse Graphs Of The Variation With Time Of Potential Difference, Charge And Current For A Capacitor Discharging Through A Resistor
- 15.70Practice Questions: Capacitance: Discharging A Capacitor:Recall And Use Τ = Rc For The Time Constant For A Capacitor Discharging Through A Resistor
- 15.71Practice Questions: Capacitance: Discharging A Capacitor: Use Equations Of The Form X = X0 E–(T/rc) Where X Could Represent Current, Charge Or Potential Difference For A Capacitor Discharging Through A Resistor
- 15.72Practice Questions: Magnetic Fields: Concept Of A Magnetic Field: Understand That A Magnetic Field Is An Example Of A Field Of Force Produced Either By Moving Charges Or By Permanent Magnets
- 15.73Practice Questions: Magnetic Fields: Concept Of A Magnetic Field: Represent A Magnetic Field By Field Lines
- 15.74Practice Questions: Magnetic Fields: Force On A Current-carrying Conductor: Understand That A Force Might Act On A Current-carrying Conductor Placed In A Magnetic Field
- 15.75Practice Questions: Magnetic Fields: Force On A Current-carrying Conductor: Recall And Use The Equation F = Bil Sin Θ, With Directions As Interpreted By Fleming’s Left-hand Rule
- 15.76Practice Questions: Magnetic Fields: Force On A Current-carrying Conductor: Define Magnetic Flux Density As The Force Acting Per Unit Current Per Unit Length On A Wire Placed At Rightangles To The Magnetic Field
- 15.77Practice Questions: Magnetic Fields: Force On A Moving Charge: Determine The Direction Of The Force On A Charge Moving In A Magnetic Field
- 15.78Practice Questions: Magnetic Fields: Force On A Moving Charge: Recall And Use F = Bqv Sin Θ
- 15.79Practice Questions: Magnetic Fields: Force On A Moving Charge: Understand The Origin Of The Hall Voltage And Derive And Use The Expression Vh = Bi /(Ntq), Where T = Thickness
- 15.80Practice Questions: Magnetic Fields: Force On A Moving Charge: Understand The Use Of A Hall Probe To Measure Magnetic Flux Density
- 15.81Practice Questions: Magnetic Fields: Force On A Moving Charge: Describe The Motion Of A Charged Particle Moving In A Uniform Magnetic Field Perpendicular To The Direction Of Motion Of The Particle
- 15.82Practice Questions: Magnetic Fields: Force On A Moving Charge: Explain How Electric And Magnetic Fields Can Be Used In Velocity Selection
- 15.83Practice Questions: Magnetic Fields: Magnetic Fields Due To Currents: Sketch Magnetic Field Patterns Due To The Currents In A Long Straight Wire, A Flat Circular Coil And A Long Solenoid
- 15.84Practice Questions: Magnetic Fields: Magnetic Fields Due To Currents: Understand That The Magnetic Field Due To The Current In A Solenoid Is Increased By A Ferrous Core
- 15.85Practice Questions: Magnetic Fields: Magnetic Fields Due To Currents: Explain The Origin Of The Forces Between Current-carrying Conductors And Determine The Direction Of The Forces
- 15.86Practice Questions: Magnetic Fields: Electromagnetic Induction: Define Magnetic Flux As The Product Of The Magnetic Flux Density And The Cross-sectional Area Perpendicular To The Direction Of The Magnetic Flux Density
- 15.87Practice Questions: Magnetic Fields: Electromagnetic Induction: Recall And Use Φ = Ba
- 15.88Practice Questions: Magnetic Fields: Electromagnetic Induction: Understand And Use The Concept Of Magnetic Flux Linkage
- 15.89Practice Questions: Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That A Changing Magnetic Flux Can Induce An E.m.f. In A Circuit
- 15.90Practice Questions: Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: That The Induced E.m.f. Is In Such A Direction As To Oppose The Change Producing It
- 15.91Practice Questions: Magnetic Fields: Electromagnetic Induction: Understand And Explain Experiments That Demonstrate: The Factors Affecting The Magnitude Of The Induced E.m.f.
- 15.92Practice Questions: Magnetic Fields: Electromagnetic Induction: Recall And Use Faraday’s And Lenz’s Laws Of Electromagnetic Induction
- 15.93Practice Questions: Alternating Currents: Characteristics Of Alternating Currents: Understand And Use The Terms Period, Frequency And Peak Value As Applied To An Alternating Current Or Voltage
- 15.94Practice Questions: Alternating Currents: Characteristics Of Alternating Currents: Use Equations Of The Form X = X0 Sin Ωt Representing A Sinusoidally Alternating Current Or Voltage
- 15.95Practice Questions: Alternating Currents: Characteristics Of Alternating Currents: Recall And Use The Fact That The Mean Power In A Resistive Load Is Half The Maximum Power For A Sinusoidal Alternating Current
- 15.96Practice Questions: Alternating Currents: Characteristics Of Alternating Currents: Distinguish Between Root-mean-square (R.m.s.) And Peak Values And Recall And Use I R.m.s. = I0 / 2 And Vr.m.s. = V0 / 2 For A Sinusoidal Alternating Current
- 15.97Practice Questions: Alternating Currents: Rectification And Smoothing: Distinguish Graphically Between Half-wave And Full-wave Rectification
- 15.98Practice Questions: Alternating Currents: Rectification And Smoothing: Explain The Use Of A Single Diode For The Half-wave Rectification Of An Alternating Current
- 15.99Practice Questions: Alternating Currents: Rectification And Smoothing: Explain The Use Of Four Diodes (Bridge Rectifier) For The Full-wave Rectification Of An Alternating Current
- 15.100Practice Questions: Alternating Currents: Rectification And Smoothing: Analyse The Effect Of A Single Capacitor In Smoothing, Including The Effect Of The Values Of Capacitance And The Load Resistance
- 15.101Practice Questions: Quantum Physics: Energy And Momentum Of A Photon: Understand That Electromagnetic Radiation Has A Particulate Nature
- 15.102Practice Questions: Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Is A Quantum Of Electromagnetic Energy
- 15.103Practice Questions: Quantum Physics: Energy And Momentum Of A Photon: Recall And Use E = Hf
- 15.104Practice Questions: Quantum Physics: Energy And Momentum Of A Photon: Use The Electronvolt (Ev) As A Unit Of Energy
- 15.105Practice Questions: Quantum Physics: Energy And Momentum Of A Photon: Understand That A Photon Has Momentum And That The Momentum Is Given By P = E/c
- 15.106Practice Questions: Quantum Physics: Photoelectric Effect: Understand That Photoelectrons May Be Emitted From A Metal Surface When It Is Illuminated By Electromagnetic Radiation
- 15.107Practice Questions: Quantum Physics: Photoelectric Effect: Understand And Use The Terms Threshold Frequency And Threshold Wavelength
- 15.108Practice Questions: Quantum Physics: Photoelectric Effect: Explain Photoelectric Emission In Terms Of Photon Energy And Work Function Energy
- 15.109Practice Questions: Quantum Physics: Photoelectric Effect: Recall And Use Hf = Φ + 2 1 Mvmax 2
- 15.110Practice Questions: Quantum Physics: Photoelectric Effect: Explain Why The Maximum Kinetic Energy Of Photoelectrons Is Independent Of Intensity, Whereas The Photoelectric Current Is Proportional To Intensity
- 15.111Practice Questions: Quantum Physics: Wave-particle Duality: Understand That The Photoelectric Effect Provides Evidence For A Particulate Nature Of Electromagnetic Radiation While Phenomena Such As Interference And Diffraction Provide Evidence For A Wave Nature
- 15.112Practice Questions: Quantum Physics: Wave-particle Duality: Describe And Interpret Qualitatively The Evidence Provided By Electron Diffraction For The Wave Nature Of Particles
- 15.113Practice Questions: Quantum Physics: Wave-particle Duality: Understand The De Broglie Wavelength As The Wavelength Associated With A Moving Particle
- 15.114Practice Questions: Quantum Physics: Wave-particle Duality: Recall And Use Λ = H/p
- 15.115Practice Questions: Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand That There Are Discrete Electron Energy Levels In Isolated Atoms (E.g. Atomic Hydrogen)
- 15.116Practice Questions: Quantum Physics: Energy Levels In Atoms And Line Spectra: Understand The Appearance And Formation Of Emission And Absorption Line Spectra
- 15.117Practice Questions: Quantum Physics: Energy Levels In Atoms And Line Spectra: Recall And Use Hf = E1 – E2
- 15.118Practice Questions: Nuclear Physics: Mass Defect And Nuclear Binding Energy: Understand The Equivalence Between Energy And Mass As Represented By E = Mc2 And Recall And Use This Equation
- 15.119Practice Questions: Nuclear Physics: Mass Defect And Nuclear Binding Energy: Represent Simple Nuclear Reactions By Nuclear Equations Of The Form 7n He O H 14 2 4 8 17 1 1 + + “
- 15.120Practice Questions: Nuclear Physics: Mass Defect And Nuclear Binding Energy: Define And Use The Terms Mass Defect And Binding Energy
- 15.121Practice Questions: Nuclear Physics: Mass Defect And Nuclear Binding Energy: Sketch The Variation Of Binding Energy Per Nucleon With Nucleon Number
- 15.122Practice Questions: Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain What Is Meant By Nuclear Fusion And Nuclear Fission
- 15.123Practice Questions: Nuclear Physics: Mass Defect And Nuclear Binding Energy: Explain The Relevance Of Binding Energy Per Nucleon To Nuclear Reactions, Including Nuclear Fusion And Nuclear Fission
- 15.124Practice Questions: Nuclear Physics: Mass Defect And Nuclear Binding Energy: Calculate The Energy Released In Nuclear Reactions Using E = C2 ∆m
- 15.125Practice Questions: Nuclear Physics: Radioactive Decay: Understand That Fluctuations In Count Rate Provide Evidence For The Random Nature Of Radioactive Decay
- 15.126Practice Questions: Nuclear Physics: Radioactive Decay: Understand That Radioactive Decay Is Both Spontaneous And Random
- 15.127Practice Questions: Nuclear Physics: Radioactive Decay: Define Activity And Decay Constant, And Recall And Use A = Λn
- 15.128Practice Questions: Nuclear Physics: Radioactive Decay: Define Half-life
- 15.129Practice Questions: Nuclear Physics: Radioactive Decay: Use Λ = 0.693/t 2 1
- 15.130Practice Questions: Nuclear Physics: Radioactive Decay: Understand The Exponential Nature Of Radioactive Decay, And Sketch And Use The Relationship X = X0e–λt , Where X Could Represent Activity, Number Of Undecayed Nuclei Or Received Count Rate
- 15.131Practice Questions: Medical Physics: Production And Use Of Ultrasound: Understand That A Piezo-electric Crystal Changes Shape When A P.d. Is Applied Across It And That The Crystal Generates An E.m.f. When Its Shape Changes
- 15.132Practice Questions: Medical Physics: Production And Use Understand How Ultrasound Waves Are Generated And Detected By A Piezoelectric TransducerOf Ultrasound:
- 15.133Practice Questions: Medical Physics: Production And Use Of Ultrasound: Understand How The Reflection Of Pulses Of Ultrasound At Boundaries Between Tissues Can Be Used To Obtain Diagnostic Information About Internal Structures
- 15.134Practice Questions: Medical Physics: Production And Use Of Ultrasound: Define The Specific Acoustic Impedance Of A Medium As Z = Ρc, Where C Is The Speed Of Sound In The Medium
- 15.135Practice Questions: Medical Physics: Production And Use Of Ultrasound: Use Ir / I0 = (Z1 – Z2) 2 /(Z1 + Z2) 2 For The Intensity Reflection Coefficient Of A Boundary Between Two Media
- 15.136Practice Questions: Medical Physics: Production And Use Of Ultrasound: Recall And Use I = I0e–μx For The Attenuation Of Ultrasound In Matter
- 15.137Practice Questions: Medical Physics: Production And Use Of X-rays: Explain That X-rays Are Produced By Electron Bombardment Of A Metal Target And Calculate The Minimum Wavelength Of X-rays Produced From The Accelerating P.d.
- 15.138Practice Questions: Medical Physics: Production And Use Of X-rays: Understand The Use Of X-rays In Imaging Internal Body Structures, Including An Understanding Of The Term Contrast In X-ray Imaging
- 15.139Practice Questions: Medical Physics: Production And Use Of X-rays: Recall And Use I = I0e–μx For The Attenuation Of X-rays In Matter
- 15.140Practice Questions: Medical Physics: Production And Use Of X-rays: Understand That Computed Tomography (Ct) Scanning Produces A 3d Image Of An Internal Structure By First Combining Multiple X-ray Images Taken In The Same Section From Different Angles To Obtain A 2d Image Of The Section, Then Repeating This Process Along An Axis And Combining 2d Images Of Multiple Sections
- 15.141Practice Questions: Medical Physics: Pet Scanning: Understand That A Tracer Is A Substance Containing Radioactive Nuclei That Can Be Introduced Into The Body And Is Then Absorbed By The Tissue Being Studied
- 15.142Practice Questions: Medical Physics: Pet Scanning: Recall That A Tracer That Decays By Β+ Decay Is Used In Positron Emission Tomography (Pet Scanning)
- 15.143Practice Questions: Medical Physics: Pet Scanning: Understand That Annihilation Occurs When A Particle Interacts With Its Antiparticle And That Mass–energy And Momentum Are Conserved In The Process
- 15.144Practice Questions: Medical Physics: Pet Scanning: Explain That, In Pet Scanning, Positrons Emitted By The Decay Of The Tracer Annihilate When They Interact With Electrons In The Tissue, Producing A Pair Of Gamma-ray Photons Travelling In Opposite Directions
- 15.145Practice Questions: Medical Physics: Pet Scanning: Calculate The Energy Of The Gamma-ray Photons Emitted During The Annihilation Of An Electron-positron Pair
- 15.146Practice Questions: Medical Physics: Pet Scanning: Understand That The Gamma-ray Photons From An Annihilation Event Travel Outside The Body And Can Be Detected, And An Image Of The Tracer Concentration In The Tissue Can Be Created By Processing The Arrival Times Of The Gamma-ray Photons
- 15.147Practice Questions: Astronomy And Cosmology: Standard Candles: Understand The Term Luminosity As The Total Power Of Radiation Emitted By A Star
- 15.148Practice Questions: Astronomy And Cosmology: Standard Candles: Recall And Use The Inverse Square Law For Radiant Flux Intensity F In Terms Of The Luminosity L Of The Source F = L/(4πd2 )
- 15.149Practice Questions: Astronomy And Cosmology: Standard Candles: Understand That An Object Of Known Luminosity Is Called A Standard Candle
- 15.150Practice Questions: Astronomy And Cosmology: Standard Candles: Understand The Use Of Standard Candles To Determine Distances To Galaxies
- 15.151Practice Questions: Astronomy And Cosmology: Stellar Radii: Recall And Use Wien’s Displacement Law Λmax ∝ 1/t To Estimate The Peak Surface Temperature Of A Star
- 15.152Practice Questions: Astronomy And Cosmology: Stellar Radii: Use The Stefan–boltzmann Law L = 4πσr 2 T4
- 15.153Practice Questions: Astronomy And Cosmology: Stellar Radii: Use Wien’s Displacement Law And The Stefan–boltzmann Law To Estimate The Radius Of A Star
- 15.154Practice Questions: Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Understand That The Lines In The Emission And Absorption Spectra From Distant Objects Show An Increase In Wavelength From Their Known Values
- 15.155Practice Questions: Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Use ∆λ / Λ . ∆f/f . V /c For The Redshift Of Electromagnetic Radiation From A Source Moving Relative To An Observer
- 15.156Practice Questions: Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Explain Why Redshift Leads To The Idea That The Universe Is Expanding
- 15.157Practice Questions: Astronomy And Cosmology: Hubble’s Law And The Big Bang Theory: Recall And Use Hubble’s Law V . H0d And Explain How This Leads To The Big Bang Theory (Candidates Will Only Be Required To Use Si Units)
- Mock Tests/ Mock ExamsMock Exams For Final Preparation0
- Class RecordingsClass Recordings From Previous Sessions/ Current Session For Content0
- Other MaterialOther Useful Material For Exams0
- Notes + Written Material For Contents of The Syllabus Version 2Notes for Chapters + Written Resources Regarding The Content Version 244
- 19.1Kinematics Of Uniform Circular Motion
- 19.2Centripetal Acceleration
- 19.3Gravitational Field
- 19.4Gravitational Force Between Point Masses
- 19.5Gravitational Field Of A Point Mass
- 19.6Gravitational Potential
- 19.7Thermal Equilibrium
- 19.8Temperature Scales
- 19.9Specific Heat Capacity And Specific Latent Heat
- 19.10The Mole
- 19.11Equation Of State
- 19.12Kinetic Theory Of Gases
- 19.13Internal Energy
- 19.14The First Law Of Thermodynamics
- 19.15Simple Harmonic Oscillations
- 19.16Energy In Simple Harmonic Motion
- 19.17Damped And Forced Oscillations, Resonance
- 19.18Electric Fields And Field Lines
- 19.19Uniform Electric Fields
- 19.20Electric Force Between Point Charges
- 19.21Electric Field Of A Point Charge
- 19.22Electric Potential
- 19.23Capacitors And Capacitance
- 19.24Energy Stored In A Capacitor
- 19.25Discharging A Capacitor
- 19.26Concept Of A Magnetic Field
- 19.27Force On A Current-Carrying Conductor
- 19.28Force On A Moving Charge
- 19.29Magnetic Fields Due To Currents
- 19.30Electromagnetic Induction
- 19.31Characteristics Of Alternating Currents
- 19.32Rectification And Smoothing
- 19.33Energy And Momentum Of A Photon
- 19.34Photoelectric Effect
- 19.35Wave-Particle Duality
- 19.36Energy Levels In Atoms And Line Spectra
- 19.37Mass Defect And Nuclear Binding Energy
- 19.38Radioactive Decay
- 19.39Production And Use Of Ultrasound
- 19.40Production And Use Of X-Rays
- 19.41PET Scanning
- 19.42Standard Candles
- 19.43Stellar Radii
- 19.44Hubble’s Law And The Big Bang Theory
- Cheat Sheets Version 2Short, Quick Revision Cheat Sheets Version 215
- Practice Questions/ Practice Exams Version 2Practice Questions/ Exams Based Both On Actual Exam Pattern And On Topical Content To Boost Preparation And Improve Performance Version 215
- 21.1Motion In A Circle
- 21.2Gravitational Fields
- 21.3Temperature
- 21.4Ideal Gases
- 21.5Thermodynamics
- 21.6Oscillations
- 21.7Electric Fields
- 21.8Capacitance
- 21.9Magnetic Fields
- 21.10Alternating Current
- 21.11Quantum Physics
- 21.12Nuclear Physics
- 21.13Medial Physical
- 21.14Astronomy And Cosmology3 Days
- 21.15Practical Skills3 Days
Practice Questions: Nuclear Physics: Radioactive Decay: Understand The Exponential Nature Of Radioactive Decay, And Sketch And Use The Relationship X = X0e–λt , Where X Could Represent Activity, Number Of Undecayed Nuclei Or Received Count Rate
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Practice Questions: Medical Physics: Production And Use Understand How Ultrasound Waves Are Generated And Detected By A Piezoelectric TransducerOf Ultrasound:
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