Undamped motion: mass and spring system

AI Thread Summary
The discussion revolves around solving a mass-spring system problem involving undamped motion. Key points include determining the equilibrium position, natural frequency, period, and the position of the mass as a function of time. Participants emphasize the importance of consistent directionality for displacement, force, and acceleration in calculations. A correction was made regarding the initial velocity's sign, leading to a revised equation for position over time. The final expression for position was confirmed to align with expected outcomes, highlighting the significance of setting the equilibrium point as the reference for future problems.
Feodalherren
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Homework Statement


A mass of 10 kg is hanging from a spring with k=2500N/m that is attached to a roof (see pic).
The length of the spring when it is not in tension is l0=0.5 m.
At the time t=0, the mass has a speed of v0=0.5 m/s when it passes the system's equilibrium position.

Determine

a) The equilibrium position
b) The natural frequency, fn
c) The period, T
d) The position of the mass as a function of time, t, measured from the roof - draw an approximate graph.

Homework Equations


F=ma

Undamped motion
Wn^2 = k/m
fn=Wn/2pi
T=1/fn
x''+(Wn^2)x=C
x(t)=Acos(Wn t) + Bsin(Wn t) + c/(Wn^2)

The Attempt at a Solution


I think I did this correctly. In part b I'm not really sure how to deal with the fact that the formula seems to be giving me Wn^2 = - k/m , but I just took the absolute value.

cpoD1-b.jpg

gUd4utp.jpg


I have no idea why the images keep being uploaded sideways. Incredibly annoying but I can't seem to fix it.
 
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First, the problem is not defined since the polarity of dx/dt(0) is not given. Maybe the missing pic does? ("Speed" is a magnitude term. What's needed is "velocity".)

Irrespective of that, however, look at your equation for x(t) in part (d). What should x(0) be?
 
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Feodalherren said:
the formula seems to be giving me Wn^2 = - k/m
You have not been consistent about which direction is positive. You show the tension as kx up. If the displacement x is down then the force is up, but if the displacement is up the force is down. So the tension should be -kx.
 
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Oh yeah sorry, I forgot to draw in the velocity. The velocity is supposed to be negative - the mass is moving down at 0.5m/s. So then the only mistake is that v0 should be -0.5?
 
rude man said:
Redo your calculations with the correct velocity and pay attention to what haruspex said about coordinate consistency. Then, as a check, reconsider my question: " look at your equation for x(t) in part (d). What should x(0) be?"

Yeah I did. I don't really see what I did wrong with the force balance, I put kx as positive since it is pulling the weight up since we're saying that at t=0 it already passed the equilibrium position of l0. x(0) = -0.53924 no?
 
Feodalherren said:
I put kx as positive since it is pulling the weight up
You need to measure displacement, force and acceleration as positive in the same direction. Up or down, pick one and stick to it.
Either way, when the displacement is positive the force is negative, and vice versa. The force is -kx, not kx.
 
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haruspex said:
You need to measure displacement, force and acceleration as positive in the same direction. Up or down, pick one and stick to it.
Either way, when the displacement is positive the force is negative, and vice versa. The force is -kx, not kx.
Aaaah yeah, now I get it. Duh! Let me do some math and get back to you. Thanks.
 
I ended up getting

X(t) = 0.5 cos (15.811t) + 0.0316 sin (15.811 t) + 0.03924

I decided just to call down positive and solve it like that instead. The results seem to agree with what it should be in the x(0) case so that's cool. Thanks for the help! Much appreciated.
 
For future problems like part (d) , it is probably easier to set x=0 at the equilibrium point. The expression for x(t), and setting x'(0) to the initial condition, wil be simpler. Also, you can then quickly check for x=0 at t=0 and, if damping is present, at t=∞. But what you did was fine.
 
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