lectures Flashcards
hookes law
F=-kx x=displacement k=spring constant
what force does hookes law describe
force used to stretch spring / restoring force towadrs equilibrium
equation of motion for undamped shm for mass on spring
a= -(k/m)x
shm equation
a=-omega^2x
solution to shm equation
x=A cos(omega t +phi) but only when omega=(k/m)^-1/2
to find equation of resonant frequency for mass on spring
omega=(k/m)^-1/2 f=(1/2pi)(k/m)^-1/2
shm phase relations between displacement acceleration and velocity
velocity lags pi/2 behind displacement and acceleration lags pi/2 behind velocity
potential energy for shm
kx^2/2
total energy for shm
E=ke+1/2kx^2= kA^2/2
damping force equation
F=-bv
equation of motion for a damped system
ma + bv+ kx=0
solution to damped harmonic motion
x=Cexp(alpha t)
solved equation of motion
x= C exp(-bt/2m) 1 exp(sqrt(b^2/4m^2 -k/m)t)
damping term of equation of motion
b^2/4m^2
stifness term of equation of motion
-k/m
when the system is heavily damped
damping term dominates- dead beat motion ocurs - non oscilatory motion b^2/4m^2 > k/m
critical damping
when b^2/4m^2 = -k/m system returns to zero a in min time. non oscilatory motion
light damping
decaying oscilatory motion b^2/4m^2 < k/m
light damping equation
x= Cexp(-bt/2m).exp(j omega’ t) where omega’ = sqrt(k/m -b^2/4m^2)
light damping equation real part
x=Cexp(-bt/2m). cos(omega’t +0)
logarithmic decrement
the natural log of the ratio of the amplitudes of any two successive peaks
logarithmic decrement equation
ln(x0/x1)=bT’/2m T’=2pi/omega’
mechanical impedence
complex quantity that represents the resistance of a system to a force that gets it moving
mechanical impedence equation
F/v = b+j(omega m +t)
forced oscilation equation of motion
ma+mv+kx=Fcos(omega t)=Fexp(jomegat)
forced oscilation equation of motion solution
-jFexp(j(omega t - phi)/omega |Z|
analysis of forced shm
if phi =0 force would lead displacement by 90 degrees
for froced shm at low frequencies
x tendes to F/k motion is stifness controled
for forced shm at high frequancies
x tendes to 0 motion is mass controlled
velocity resonce of forced shm occus at
sqrt(k/m)
power supplied by driving force. inst
p=Fv=F^2cos(omega t)cos(omega t- phi)/|Z|
average power supplied by driving force
F^2cos(phi)/2|Z| cos(phi)=power factor or bF^2/2|Z|^2
frequancy at max power dissapated
sqrt(k/m)
q value
size of q value tells us the sharpness of the resonave peak Q=omega max/ omega2 - omega 1 =omega max/mb
average power supplied by driving force max
F^2/2b