Solve Spring Problem: Position, Work Done, and Kinetic Energy

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The discussion revolves around a physics problem involving a block connected to a spring on a frictionless surface, where an applied force stretches the spring until the block stops. Key points include the calculations for the block's position when it stops, the work done by the applied force, and the work done by the spring force. The consensus is that the maximum kinetic energy occurs when the block is in motion, specifically at the point where the spring force equals the applied force, not when the block stops. Ultimately, the correct position of the block when it stops is determined to be 0.12 m, with corresponding work values of 36 J for both the applied and spring forces, and maximum kinetic energy calculated at 0.09 J.
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here is the problem:
A block lies on a frictionless, horizontal surface, with one side connected to a wall by a spring, with a spring constant of 50 N/m. Initially, the spring is at its relaxed length and the block is stattionary at position x = 0. Then an applied force with a constant magnitiude of 3.0 Npulls the block in the positive direction on the X axis, stretching the spring until the block stops.
When that stopping point is reached, what are...
a) The position of the block
b) The work that has been done on the block by the appleid force
c) The work that has been done on this block by the spring force
During the blocks displacment, that are...
d) The block's position when its kenetic energy is maximum
e) The vlaue of that maximum kinetic energy?
On questions a) through c), I think I got correct, here are my answer:
a) .06 m
spring force opposing the applied force = -3 N, and spring force = -k*d.
So set force = -3, then solve for d, distance

b) .18 J
Work = F * d, we got distance from part a), and the force is given as 3 N

c) -.09 J
the work done by a spring when the object is stationary before and after, is given by, W = 1/2*k*x^2, so plug in the values we know, k=-50, x = .06


Parts d) and e) are more tricky,
the kinetic energy is maximized when the object is moving the fastest, in other words, when acceleration = 0, thus net force = 0.
this occurs at the very end, when the spring force cancels out the applied force, but that this point, the object has come to a stop, this KE = 0.
How do I find this?
When originally doing this problem, I just assumed that it would reach its maximum velocty at the end (.06 m), but on closer inpection, I realized that it would have no velocity there. I solved for it anyway at that location..
d) .06 m
e) .09 J
change in Ke = Word done by the applied force, plus work done by the spring, so it is .18 J - .09 J = .09 J.
 
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This question is tricky, but not in the way you're thinking. Read the question more carefully. Even your answer to a) is wrong. The first part pertains to when the block stops. Will the net force on the block necessarily be zero at this point ? What can you say instead about the kinetic energy when the block stops ? Come up with an equation to relate the net work done on the block from the start to the point of the block stopping to its kinetic energy at anyone time, and see what you get for answer a).
 
Will the net force on the block necessarily be zero at this point ?
well obviously you think it doesn't necesarily, otherwise you wouldn't ask me the question, but I still think yes.
if a constant force is being applied to the block, then the block will begin to accelerate...eventually the spring force will match the constant force, so then it is just mving at a constant speed, ...eventually it should reach an equalibrium between moving toward/away from the wall it is attached to and that point should be where the net force = 0, velocity = 0, wouldn't that be where the spring force = the applied force?

well, when the block stops moving, it will have a kinetic energy of 0 J.
when it just begins (still hasnt began to move yet), it still has a kinetic energy of 0 J. so some where in between the kinetic energy must be maximized, and at that point it has reached it highest velocity, therefiore no acceleration, therefore, net force = 0. if that is true then perhaps this is the part of the question for which the distance of .06 m is correct?
 
your prt a is wrong...
hints
the point it stops is not its equilibium point... the spring has over strech and the block will bronce back... you have to visiulize the problem b4 pluging the number in the formulas

edit:
eventually it should reach an equalibrium between moving toward/away from the wall it is attached to and that point should be where the net force = 0, velocity = 0,
when the velocity is zero, is the necessary the acceleration is also zero
 
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Hi,
You are wrong, mrjeffy321. When the spring force = the applied force. It does not mean the block will stop moving immediately. It will continue moving.
After that the spring force > the applied force, and the acceleration is negative. That will cause the block slowing down to a stop. Get it?
Hope it help,
Viet Dao,
 
Well the way I understand the problem is that the block never actually bounces all the way back, but insted just goes back and forth a couple times eventually reaching equalibrium and stoping. and then where it stops is a certain, unknown (to me) distance from the wall. but now I see that I had initially envisioned the problem incorrectly, now I can at least visualize it.

well atleast am I correct in thinking that it's "equalibrium point" is the lcation that the block has the most kinetic energy?, and if that is true, wouldn't that location be in between (centered) the stoping place and the wall?
 
anyway, can anyone give me a very strong push in the right direction in finding these answers
 
Visualise the forces acting on the block and its velocity as a function of its displacement from the start.

At all times there are two forces acting on the block, a constant applied force, magnitude 3 N in the positive direction (say), and a varying force due to spring tension acting in the negative direction.

Initially, the block is at rest, its Kinetic energy (KE) is zero, and the force acting on it is +3N. It starts accelerating in the positive direction at a rate given by 3N/m where m is the mass of the block. This initial acceleration is the maximum positive acceleration.

As the block moves in the positive x direction, the spring stretches and the tension in it increases in proportion to it (Hooke's law). As a result, the spring force acting in the negative direction gradually increases, and the acceleration in the +x direction becomes less and less the more the block moves out. Nevertheless, as long as the acceleration is positive, the block still continues to speed up.

A point comes when the force the spring exerts on the block exactly cancels out the 3N force. Here the net force is zero, and the acceleration of the block is therefore zero. At this instant in time, the block is NOT at rest, it is still travelling. Because it has been accelerating all this time and has not yet begun decelerating this is its maximum velocity. The KE is also maximum at this point.

The momentum of the block carries it beyond the above equilibrium point. As the block stretches the spring just a little further, you will now note that the spring force is greater in magnitude than the +3N force. Consequently, the block starts decelerating (slowing down). The block does not immediately stop and bounce back, but keeps going until the decelerating net force acting on it is enough to shave off all of its velocity and bring it to rest. When it comes to rest, the velocity is zero, KE is zero, but there is a negative force acting on the block to pull it back.

That's the point you need to consider for the first part of the problem. It is incorrect to equate the spring force to 3N to solve for that point, because the net force is NOT zero at that point. The only think you do know is that the kinetic energy is zero at that point, and therefore the net work done on the object by the two forces acting on it is zero at that point. Can you go from there ?
 
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The way i see this problem,it's not as simple as it looks.Not simple at all.Do you know to solve Cauchy problems in HS??I didn't.I learned that in first year of college.The block is oscillating under the influence of an external force.Those are FORCED OSCILLATIONS.I never seen problems with forced oscillations in HS.
They involve solving the following Cauchy problem:
\frac{d^{2}x(t)}{dt^{2}}+\omega^{2}x(t)=F (1)

\omega=:\sqrt{\frac{k}{m}} (2)

x(0)=0;\frac{dx(t)}{dt}|_{t=0} =0 (3)

Maybe someone else will come up with a simpler solution...

Daniel.

PS.The answer to "a" is 0.12m.Twice the amplitude of oscillation.
 
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  • #10
Further hints :

At the point when the block stops (let that be x_1, what is the work done by the +3N force ? Use W = Fx.

At the same point, what is the work done by the spring force ? Use W = -\frac{1}{2}kx^2.

The sum of those two is the net work done on the block, equate to zero, and solve for x_1.

The answers to b) and c) are equal, and they've already been calculated by the above.

For d), you can do what you did in your original attempt, equate the spring force to 3N and solve for the force-equilibrium point (let's call that x_0.

e) And using a similar approach to what we did for part a), you can calculate the net work done on the object at this point to give the max KE.
 
  • #11
OK, here is what I have now,
a) 1.2 m
b) 36 J
c) 36 J
d) .06 m
e) .09 J

explanations,
a) from dextercioby
b) work from the spring at 1.2 m is equal to -.5*-50*1.2^2, that comes out to 36 J
c) equal to part b)
d) solve formula F=-k*d for d, where the force = -3 N and k = -50, d = .06 m
e) work from the applied force - work from the spring (since the spring is "woking" the other way), work from the spring at .06 m is .09 J, and the work from the applied force = .18 J. that means a net work of .09 J for a kinetic energy of .09 J.

Am I wrong on something
 
  • #12
Use Newton's second law to find the equation of motion of the block.

<br /> ma = F - kx<br />

Then use the work-kinetic energy theorem, changing the integration variable to x&#039;.

<br /> \begin{align*}<br /> \Delta K &amp; = \int_{0}^{x}(F - kx&#039;)\, dx \\<br /> &amp; = Fx - \frac{1}{2}kx^{2}<br /> \end{align*}<br />

The block begins and ends at rest, so \Delta K = 0. Solving the equation gives
x = \frac{2F}{k} = 0.12 metres.
 
  • #13
Maximum kinetic energy corresponds to dK/dx = 0. This occurs when x = F/k = 0.06 metres. K = 3*0.06 - 0.5*50*0.06^2 = 0.09 joules.
 
  • #14
so then,
a) .12 m
b) .36 J
c) .36 J

I understand that explanation much better.

and the max distance from the wall is .12 m, which is double the distance of the location where net force = 0, which is what I eluded to in post #6.
 
  • #15
Yes, you got it. :smile:
 
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