lectures Flashcards

1
Q

hookes law

A

F=-kx x=displacement k=spring constant

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2
Q

what force does hookes law describe

A

force used to stretch spring / restoring force towadrs equilibrium

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3
Q

equation of motion for undamped shm for mass on spring

A

a= -(k/m)x

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4
Q

shm equation

A

a=-omega^2x

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5
Q

solution to shm equation

A

x=A cos(omega t +phi) but only when omega=(k/m)^-1/2

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6
Q

to find equation of resonant frequency for mass on spring

A

omega=(k/m)^-1/2 f=(1/2pi)(k/m)^-1/2

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7
Q

shm phase relations between displacement acceleration and velocity

A

velocity lags pi/2 behind displacement and acceleration lags pi/2 behind velocity

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8
Q

potential energy for shm

A

kx^2/2

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9
Q

total energy for shm

A

E=ke+1/2kx^2= kA^2/2

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10
Q

damping force equation

A

F=-bv

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11
Q

equation of motion for a damped system

A

ma + bv+ kx=0

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12
Q

solution to damped harmonic motion

A

x=Cexp(alpha t)

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13
Q

solved equation of motion

A

x= C exp(-bt/2m) 1 exp(sqrt(b^2/4m^2 -k/m)t)

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14
Q

damping term of equation of motion

A

b^2/4m^2

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15
Q

stifness term of equation of motion

A

-k/m

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16
Q

when the system is heavily damped

A

damping term dominates- dead beat motion ocurs - non oscilatory motion b^2/4m^2 > k/m

17
Q

critical damping

A

when b^2/4m^2 = -k/m system returns to zero a in min time. non oscilatory motion

18
Q

light damping

A

decaying oscilatory motion b^2/4m^2 < k/m

19
Q

light damping equation

A

x= Cexp(-bt/2m).exp(j omega’ t) where omega’ = sqrt(k/m -b^2/4m^2)

20
Q

light damping equation real part

A

x=Cexp(-bt/2m). cos(omega’t +0)

21
Q

logarithmic decrement

A

the natural log of the ratio of the amplitudes of any two successive peaks

22
Q

logarithmic decrement equation

A

ln(x0/x1)=bT’/2m T’=2pi/omega’

23
Q

mechanical impedence

A

complex quantity that represents the resistance of a system to a force that gets it moving

24
Q

mechanical impedence equation

A

F/v = b+j(omega m +t)

25
Q

forced oscilation equation of motion

A

ma+mv+kx=Fcos(omega t)=Fexp(jomegat)

26
Q

forced oscilation equation of motion solution

A

-jFexp(j(omega t - phi)/omega |Z|

27
Q

analysis of forced shm

A

if phi =0 force would lead displacement by 90 degrees

28
Q

for froced shm at low frequencies

A

x tendes to F/k motion is stifness controled

29
Q

for forced shm at high frequancies

A

x tendes to 0 motion is mass controlled

30
Q

velocity resonce of forced shm occus at

A

sqrt(k/m)

31
Q

power supplied by driving force. inst

A

p=Fv=F^2cos(omega t)cos(omega t- phi)/|Z|

32
Q

average power supplied by driving force

A

F^2cos(phi)/2|Z| cos(phi)=power factor or bF^2/2|Z|^2

33
Q

frequancy at max power dissapated

A

sqrt(k/m)

34
Q

q value

A

size of q value tells us the sharpness of the resonave peak Q=omega max/ omega2 - omega 1 =omega max/mb

35
Q

average power supplied by driving force max

A

F^2/2b