Oscillations and Waves Flashcards

1
Q

Differential equation for mass on a spring

A

d^2x/dt^2=-k/m*x

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2
Q

Differential equation for pendulum

A

d^2(theta)/dt^2=-g/l*theta

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3
Q

Differential equation for LC circuit

A

d^2i/dt^2=-1/LC*i

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4
Q

What is the general solution for a harmonic oscillator

A

Acos(w0*t+phi)
for any displacement eg. x, theta, etc.

Comes from the superposition from the two general solutions.

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5
Q

How are circular motion and harmonic motion linked

A

harmonic motion is circular motion projected onto the real (x) axis

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6
Q

What is the total energy of a naturally oscillating system

A

1/2mw0^2*A^2

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7
Q

what is w0 for a spring

A

sqrt(k/m)

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8
Q

what is w0 for a pendulum

A

sqrt(g/l)

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9
Q

what is the damping coefficient

A

gamma=b/m where b is the constant of proportionality of the linear damping term

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10
Q

what is the term added to the equation for a damped harmonic oscillator

A

-b*velocity [x dot]

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11
Q

what is the quadratic solution for w for a damped oscillating system

A

w=i(gamma)/2 ± sqrt((wo)^2-(gamma/2)^2)

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12
Q

what is the case for light damping

A

gamma/2 < w0

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13
Q

what is the light damping solution

A

Ae^(-gammat/2) cos(wdt+phi)

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14
Q

what does an increased damping coefficient mean for a lightly damped system

A

a decreased time to get to equilibrium

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15
Q

what is the case for heavy damping

A

gamma/2 > w0

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16
Q

what is the heavy damping solution

A

Be^-t(gamma+)/2 + Ce^-t(gamma-)/2

17
Q

what does an increased damping co-efficient mean for a heavy damped system

A

an increased time to get to equilibrium

18
Q

what is the case for critical damping

A

gamma/2=w0

19
Q

what is the critical damping solution

A

(B+C)e^-t(gamma)/2

20
Q

what is particular about critical damping

A

there is no oscillation, there is just a decay

21
Q

what is the form of the external driver force

A

Focos(wt)

22
Q

what is the solution, and parameters, doe the driven oscillator
what type of solution is this

A

x=Acos(wt+phi)

STEADY STATE SOLUTION
where:

A=(Fo/m)/sqrt((w0^2-w^2)^2+w^2(gamma)^2)

phi=tan^-1(-w(gamma)/w0^2-w^2)

23
Q

when does resonance occur

A

w=w0

24
Q

What happens to phi over the resonance ‘cycle’

A

below resonance, phi=0 [driving force too slow]
at resonance, phi=-pi/2
above resonance, phi=-pi [driving force too fast]

25
Q

what determines the width of the resonance amplitude peak

A

gamma (damping co-efficient)

26
Q

what is a special case for the driven harmonic oscillator and what are the solutions

A

at resonance, w=w0:

A=(Fo/2mw0)/sqrt((w-w0)^2+(gamma/2)^2)

phi=tan^-1(gamma/w-w0)

27
Q

what is the equation for Q

A

Q=w0/gamma