Damped And Forced Oscillations, Resonance (Copy)
Definition and Nature of Damping
- Damping refers to the process by which the energy of an oscillating system is gradually lost to the surroundings
- It typically happens due to resistive forces, such as:
- Air resistance
- Friction
- Viscous drag
- These forces oppose the motion of the oscillating system and remove energy from it
- As energy is lost, the amplitude of oscillation decreases over time
Types of Damping
1. Light Damping (Underdamping)
- Occurs when damping is present but relatively small
- System continues to oscillate but with gradually decreasing amplitude
- The motion is still oscillatory
- Energy is removed slowly
Displacement–Time Graph Characteristics:
- Graph shows sinusoidal oscillations
- Amplitude decreases exponentially over time
Written and Compiled By Sir Hunain Zia, World Record Holder With 154 Total A Grades, 7 Distinctions and 11 World Records For Educate A Change A2 Level Physics Full Scale Course
2. Critical Damping
- The system returns to equilibrium in the shortest possible time without oscillating
- It is the threshold between oscillatory and non-oscillatory motion
- Used in systems where rapid damping is desirable:
- Car suspension systems
- Door dampers
Displacement–Time Graph Characteristics:
- No oscillation is observed
- Displacement falls to zero quickly but smoothly
3. Heavy Damping (Overdamping)
- Damping is so large that the system returns to equilibrium very slowly
- There is no oscillation
- The resistive force is very large compared to the restoring force
Displacement–Time Graph Characteristics:
- A slow, non-oscillatory return to equilibrium
- Much slower than critically damped systems
Comparison Table: Types of Damping
| Damping Type | Oscillation Present? | Return to Equilibrium | Example Application |
|---|---|---|---|
| Light Damping | Yes | Gradual | Guitar strings, pendulums |
| Critical Damping | No | Fastest possible | Car shock absorbers |
| Heavy Damping | No | Slow | Swing doors, soft-close lids |
Written and Compiled By Sir Hunain Zia, World Record Holder With 154 Total A Grades, 7 Distinctions and 11 World Records For Educate A Change A2 Level Physics Full Scale Course
Definition and Nature of Forced Oscillations
- A forced oscillation occurs when a system is made to vibrate by a periodic external driving force
- The system is not oscillating freely but is responding to the external force
- The driving frequency is the frequency of the external force
- The amplitude of the oscillation depends on:
- The natural frequency of the system
- The frequency of the driving force
- The amount of damping
Natural Frequency
- Every oscillating system has its own natural frequency, which is the frequency it oscillates at when not subjected to an external force
- Given by:
- For spring-mass system: f = (1 / 2π) × √(k/m)
- For a simple pendulum: f = (1 / 2π) × √(g/L)
- Resonance occurs when the driving frequency = natural frequency
Resonance
- Resonance is the phenomenon where a system subjected to a periodic driving force vibrates with maximum amplitude when the driving frequency equals the natural frequency
- At resonance:
- Energy transfer is most efficient
- Amplitude increases significantly
- Amplitude becomes limited only by the damping present
Written and Compiled By Sir Hunain Zia, World Record Holder With 154 Total A Grades, 7 Distinctions and 11 World Records For Educate A Change A2 Level Physics Full Scale Course
Amplitude vs Frequency Graph (Resonance Curve)
- The graph shows how amplitude varies with the driving frequency
- Undamped System:
- Sharp peak at resonance
- Infinite amplitude theoretically
- Lightly Damped System:
- High, sharp peak
- Narrow bandwidth (sharp resonance)
- Heavily Damped System:
- Low, broad peak
- No sharp resonance
Phase Difference in Forced Oscillations
| Driving Frequency (f_d) | Phase Difference (φ) between driver and system |
|---|---|
| f_d << natural frequency | System in phase with driver (φ ≈ 0) |
| f_d = natural frequency (resonance) | System lags by π/2 (φ = 90°) |
| f_d >> natural frequency | System lags by π (φ = 180°) |
Graphical Summary
- Displacement vs Time for different damping levels:
- Light damping: decreasing sinusoidal
- Critical damping: non-oscillatory, sharp fall
- Heavy damping: non-oscillatory, slow fall
- Amplitude vs Frequency:
- Peak at resonance shifts and lowers with increasing damping
- Width of resonance curve increases with damping
Written and Compiled By Sir Hunain Zia, World Record Holder With 154 Total A Grades, 7 Distinctions and 11 World Records For Educate A Change A2 Level Physics Full Scale Course
Practical Examples of Resonance
| System | Natural Frequency Driven? | Result of Resonance |
|---|---|---|
| Glass + Sound Waves | Yes (singing at natural freq) | Glass may shatter due to high amplitude |
| Radio Receiver | Tuned circuit | Allows selective reception of one frequency |
| Bridges (e.g. Tacoma) | Wind or soldiers’ marching | Violent vibrations, possible structural failure |
| MRI Machines | Magnetic field oscillations | Resonates with atomic nuclei for imaging |
Damping and Resonance Applications
- Desirable resonance:
- Musical instruments (tuned for resonance)
- Radios, clocks (need sharp resonance for accuracy)
- Undesirable resonance:
- Bridges (e.g., Millennium Bridge in London)
- Machinery (causes fatigue or failure)
- Buildings during earthquakes
- Damping is used to:
- Reduce unwanted oscillations
- Prevent damage in structures
- Increase system stability
Written and Compiled By Sir Hunain Zia, World Record Holder With 154 Total A Grades, 7 Distinctions and 11 World Records For Educate A Change A2 Level Physics Full Scale Course
Key Equations and Concepts Recap
- Natural frequency (spring system):
f = (1 / 2π) × √(k/m) - Total energy in SHM:
E = ½mω²x₀² - Driving frequency = natural frequency ⇒ Resonance
- Damping reduces amplitude and shifts the resonance peak to a lower frequency
