Oscillations and Waves 1 Flashcards

1
Q

Simple Harmonic Motion

Definition

A

Fx = -kx = max

In simple harmonic motion, the acceleration is both proportional to and oppositely directed from, the displacement from the equilibrium position

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

Simple Harmonic Motion

Position Function

A

x = A cos(ωt + 𝛿)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

Simple Harmonic Motion

Angular Frequency

A

ω = 2πf = 2π/T

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

Simple Harmonic Motion

Mechanical Energy

A

E = K + U = 1/2 kA²

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

Simple Harmonic Motion and Circular Motion

A

If a particle moves in a circle with constant speed, the projection of the particle onto a diameter of the circle moves in simple harmonic motion.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Simple Harmonic Motion

General Motion and Equilibrium

A

If an object is given a small displacement from a position of stable equilibrium, it typically oscillates about this position with simple harmonic motion.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

Natural Frequency

Mass on a String

A

ω0 = √(k/m)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Natural Frequency

Simple Pendulum

A

ω0 = √(g/L)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Natural Frequency

Torsional Oscillator

A

ω0 = √(κ/I)

I = moment of inertia
κ = torsional constant
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Torsional Constant

A

For small oscillations of a physical pendulum
κ = MgD
where D is the distance of the axis of rotation from the centre of mass

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Damped Oscillations

Definition

A

In the oscillations of real systems, motion is damped because of dissipative forces.
If the damping is greater than some critical value, the system does not oscillate when disturbed it simply returns to its equilibrium position.
The motion of a weakly damped system is nearly simple harmonic motion with an amplitude that decreases exponentially with time.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

Damped Oscillations

Frequency

A

ω’ = ω0 √(1 - 1/4Q²)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

Damped Oscillations

Energy

A

E = E0 e^(-t/τ)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

Damped Oscillations

Amplitude

A

A = A0 e^-(t/2τ)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

Damped Oscillations

Decay Time

A

τ = m / b

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Q Factor

A

Q = τω0

17
Q

Q Factor for Weak Damping

A

Q ≈ 2π / (|ΔE|/E) where ΔE/E &laquo_space;1

18
Q

Driven Oscillations

Definition

A

When an underdamped (b

19
Q

Resonance Frequency

A

ω = ω0

where ω0 is the natural frequency and ω is the driving frequency

20
Q

Resonance Frequency for Weak Damping

A

Δω/ω0 = 1/Q

21
Q

Driven Oscillations

Position Function

A

x = A cos(ωt - 𝛿)

22
Q

Driven Oscillations

Amplitude

A

A = F0 / √[m²(ω0²-ω²) + b²ω²]

23
Q

Driven Oscillations

Phase Constant

A

tan 𝛿 = bω / m(ω0² - ω²)