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A pendulum of mass m= 0.8 kg and length l=1 m is hanging from the ceiling. The massless string of the pendulum is attached at p...Asked by Anonymous
A pendulum of mass m= 0.8 kg and length l=1 m is hanging from the ceiling. The massless string of the pendulum is attached at point P. The bob of the pendulum is a uniform shell (very thin hollow sphere) of radius r=0.4 m, and the length l of the pendulum is measured from the center of the bob. A spring with spring constant k= 7 N/m is attached to the bob (center). The spring is relaxed when the bob is at its lowest point (θ=0). In this problem, we can use the small-angle approximation sinθ≃θ and cosθ≃1. Note that the direction of the spring force on the pendulum is horizontal to a very good approximation for small angles θ. (See figure)
Take g= 10 m/s2
(a) Calculate the magnitude of the net torque on the pendulum with respect to the point P when θ=5∘. (magnitude; in Nm)
|τP|=
(b) What is the magnitude of the angular acceleration α=θ¨ of the pendulum when θ=5∘? (magnitude; in radians/s2)
|α|=
(c) What is the period of oscillation T of the pendulum? (in seconds)
T=
Take g= 10 m/s2
(a) Calculate the magnitude of the net torque on the pendulum with respect to the point P when θ=5∘. (magnitude; in Nm)
|τP|=
(b) What is the magnitude of the angular acceleration α=θ¨ of the pendulum when θ=5∘? (magnitude; in radians/s2)
|α|=
(c) What is the period of oscillation T of the pendulum? (in seconds)
T=
Answers
Answered by
Damon
Is this an 8:01 problem ? If not I will do it.
Answered by
Damon
If it is not I will help.
Answered by
shaka
no it isn't
Answered by
Damon
Thanks
Answered by
Damon
Lets do moments of inertia about the pivot point
First the moment of inertia of this thin shell about a horizontal line through its center is (2/3) mR^2
for derivation see http://hyperphysics.phy-astr.gsu.edu/hbase/isph.html
This has to be transferred up to the pivot point using the parallel axis theorem
I = m L^2 + (2/3) m R^2
here
m = .8
L = 1
R = .4
so
I = .8 + .085 = .885
First the moment of inertia of this thin shell about a horizontal line through its center is (2/3) mR^2
for derivation see http://hyperphysics.phy-astr.gsu.edu/hbase/isph.html
This has to be transferred up to the pivot point using the parallel axis theorem
I = m L^2 + (2/3) m R^2
here
m = .8
L = 1
R = .4
so
I = .8 + .085 = .885
Answered by
Anonymous
but how do you get alpha?
Answered by
Damon
Now let's do Moments about the pivot point
let angle theta = T
restoring Force = - k x - m g sin T
but sin t is about T in radians for small T
so
F = -k x - m g T
x is about L T
so
F = -k L T - m g T
moment = M = F L = -(k L^2 + mgL)T
moment = I alpha
-(k L^2 + mgL)T = .885 d^2T/dt^2
well calculate the coefficient of T on the left
-(7 + 8) T = .885 d^2T/dt^2
.885 d^2T/dt^2 = - 15 T
let T = A sin ( w t)
then d^2T/dt^2 = - w^2 T
so
.885 w^2 = 15
w = 2 pi f = 2 pi/period = 4.11
let angle theta = T
restoring Force = - k x - m g sin T
but sin t is about T in radians for small T
so
F = -k x - m g T
x is about L T
so
F = -k L T - m g T
moment = M = F L = -(k L^2 + mgL)T
moment = I alpha
-(k L^2 + mgL)T = .885 d^2T/dt^2
well calculate the coefficient of T on the left
-(7 + 8) T = .885 d^2T/dt^2
.885 d^2T/dt^2 = - 15 T
let T = A sin ( w t)
then d^2T/dt^2 = - w^2 T
so
.885 w^2 = 15
w = 2 pi f = 2 pi/period = 4.11
Answered by
Damon
Hey, I am kind of slow and can not do everything at once.
Check arithmetic!
Check arithmetic!
Answered by
Damon
when you do these, use T in RADIANS
5 degrees *pi/180
(a) Calculate the magnitude of the net torque on the pendulum with respect to the point P when θ=5∘. (magnitude; in Nm)
Torque = -15T where T = 5 * pi/180
|τP|=
(b) What is the magnitude of the angular acceleration α=θ¨ of the pendulum when θ=5∘? (magnitude; in radians/s2)
alpha = d^2T/dt^2 = - 15 T /.885
|α|=
5 degrees *pi/180
(a) Calculate the magnitude of the net torque on the pendulum with respect to the point P when θ=5∘. (magnitude; in Nm)
Torque = -15T where T = 5 * pi/180
|τP|=
(b) What is the magnitude of the angular acceleration α=θ¨ of the pendulum when θ=5∘? (magnitude; in radians/s2)
alpha = d^2T/dt^2 = - 15 T /.885
|α|=
Answered by
vivipop
Hey Damon, i just want to say thank you for making me believe in myself one more time. i got this but i didn't think my workings were right,so i was scared to key in my answers. Now,i am sooo confident in myself. thank you.
Answered by
Anonymous
how is the period found?
Answered by
shaka
this is an exercise of the exam, somoone posted in my name. no problem though . cheaters are fooling themselves.
Answered by
shaka
I really pity these fools, who do not have a clue about anything...
Answered by
shaka
are you the real shaka? or are you a saboture
Answered by
shaka
the fact that your browsing these forums means you are a cheater as well
Answered by
Damon
At this point anyone who needs help finding the period is in serious trouble.
Answered by
fighter
hey DAMON can u please tell about C part of the question
Answered by
Damon
I did.
Answered by
C++MeetsJava
This problem is really all about an expression summarizing harmonic motion.
So your period for this problem is oddly similar to
T = 2pi * sqrt (m/k)
but now m = moment of inertia
and k = expanded coefficient, that was given above by Mr. Damon
Also make sure that you end up with seconds as units
So your period for this problem is oddly similar to
T = 2pi * sqrt (m/k)
but now m = moment of inertia
and k = expanded coefficient, that was given above by Mr. Damon
Also make sure that you end up with seconds as units
Answered by
C++MeetsJava
this will surely hurt more than help but here you go
Period = 2*pi sqrt([kl^2+mgl]/[(2mr^2)/3+ ml^2)
Period = 2*pi sqrt([kl^2+mgl]/[(2mr^2)/3+ ml^2)
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