TOPIC 10: OSCILLATIONS Flashcards

1
Q

[Definition] Oscillation

A

An oscillation is a to-and-fro motion between two limits

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2
Q

[Definition] Free Oscillations

A

Free oscillations are oscillations with constant amplitude AND without energy loss or gain as there is no driving or resistive forces acting on it

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3
Q

[Definition] Natural Frequency

A

Natural frequency is the frequency at which a body will vibrate when there is no driving or resistive forces acting on it

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4
Q

[Definition] Equilibrium Position

Quantities of Oscillation

A

Position where no net force acts on the oscillating mass

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5
Q

[Definition] Displacement, x

Quantities of Oscillation

A

Distance in a specified direction from equilibrium position of oscillating mass

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6
Q

[Definition] Amplitude, x₀

Quantities of Oscillation

A

Maximum distance from equilibrium position

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7
Q

[Definition] Period, T

Quantities of Oscillation

A

Time taken for one complete oscillation of the oscillating mass

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8
Q

[Definition] Frequency, f

Quantities of Oscillation

A

Number of complete oscillations per unit time

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9
Q

[Definition] Phase, ϕ

Quantities of Oscillation

A

An angular measure of the fraction of a cycle completed by the oscillating mass

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10
Q

[Definition] Phase Difference, Δϕ

Quantities of Oscillation

A

Measure of how much an oscillation is out of step with another oscillation

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11
Q

[Definition] Angular frequency

Quantities of Oscillation

A

Defined as the product of 2π and frequency

ω = 2πf (units: radian s⁻¹)

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12
Q

[Definition] Simple Harmonic Motion

A

SHM is a type of oscillatory motion where the acceleration is directly proportional to the displacement from the equilibrium position and directed opposite to displacement

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13
Q

[Formula] Main Formulas of Oscillation

Variation with x

A

a = - ω²x
v = ±√(x₀² - x²)

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14
Q

[Formula] Main Formulas of Oscillation

Variation with t

A

If x = 0
x = x₀ sin(ωt)
v = ωx₀ cos(ωt)
a = - ω²x₀ sin(ωt)

If x = x₀
x = x₀ cos(ωt)
v = - ωx₀ sin(ωt)
a = - ω²x₀ cos(ωt)

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15
Q

Finding equations for horizontal spring-mass systems

A

Combine with topic on Forces

F = ma = kx
a = - ω²x

to find ω, f, T etc

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16
Q

Finding equations for vertical spring-mass systems

A

Combine with topic on Forces
F = ma
kx = ma
a = - ω²x
to find ω, f, T etc

17
Q

Finding equations for simple pendulum

A

Combine with topic on Forces
F = ma
mg sinθ = ma
a = - ω²x
to find ω, f, T etc

18
Q

Finding energy of oscillations

A
  1. Always find kinetic energy first
  2. Followed by total energy (when Ek max)
  3. Potential energy

Same for both (variation with displacement / time)

19
Q

[Definition] Damped Oscillations

A

Damped oscillations are oscillations in which the amplitude decreases with time as a result of dissipative forces that reduces the total energy of the oscillations

20
Q

Light to Critical to Heavy Damping

A

Light to Critical to Heavy Damping:
Light: More time needed to return to equilbrium
Critical: Shortest possible time (no oscillation)
Heavy: More time than critical (no oscillation)

21
Q

[Definition] Forced Oscillations

A

Forced oscillations are oscillations where there is a continuous input of energy by an external periodic force that maintains the oscillation amplitude

22
Q

Amplitude - driving frequency graph

A

Increases from non-zero y-intercept to max (at natural frequency), then decreases to near zero

23
Q

[Definition] Resonance

A

Resonance is a phenomenon in which the amplitude of an oscillatory motion is at maximum because there is maximum rate of transfer of energy from the external driver to the oscillating system.

This occurs when the driving frequency of the external periodic force equals to the natural frequency.

24
Q

Amplitude - driving frequency graph of no damping to increased damping

A
  1. Max amplitude decreases
  2. Max amplitude shifts to left (cos period longer, so frequency decreases)
  3. Flatter curve