Spring Force and Restoring Motion on XY Plane

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Homework Help Overview

The discussion revolves around a problem involving a small metal block constrained to move along a frictionless groove, attached to a spring. The block is displaced from the spring's equilibrium position and the participants are tasked with showing that the restoring force is proportional to x^3, indicating non-simple harmonic motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the components of the spring force and how they relate to the motion along the groove. There are questions about the total force in the spring and its components along the groove. Some participants express confusion about the importance of the y-component of the force and the implications of the spring's behavior.

Discussion Status

Participants are actively engaging with the problem, exploring different aspects of the spring force and its components. Some guidance has been offered regarding the relationship between the force and the displacement, and there is an ongoing examination of how to express the restoring force in terms of the displacement.

Contextual Notes

There are hints provided in the original problem statement that participants are encouraged to utilize, and some participants are questioning the assumptions made about the spring's behavior and the geometry involved in the problem.

yasar1967
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A small metal block of mass m is placed on a smooth horizontal table and constrained to move along a frictionless, rectilinear groove, The block is attached to one end of a spring (of spring constant k) whose other end is fastened to a pin P.
Let length L be the equilibrium length of the spring and the perpendicular distance to the groove, The spring is now pulled a distance Xo from the equilibrium position and released. Show that, if the displacement along the groove x « t. the restoring force on
the block is proportional to x ^3 , so the motion is not simple harmonic although it will still be periodic). [Hint: For x « L, x^2 + L^2 "" L + (x^2 /2L).]




General spring and harmonic , periodic motion formulas



I thought the cosine of the F force on the spring is the responsible force i.e. restoring force and sine of F has no importance, therefore Fcosineø = -k x .. but from there I get nowhere :(
 
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yasar1967 said:
Hint: For x « L, √(x^2 + L^2) ~ L + x^2/2L.

Hi yasar! :smile:

What diagram have you drawn?

What is the total force in the spring at distance x along the groove?

So what is the component along the groove?

(Hint: cosine ~ x/(L + x^2/2L).)
 
well, it's from "PHYSICS for Scientists... by Fishbane Gasiorowicz Thornton" Tim, but I don't know how to upload a picture or a diagram :(

If you could imagine it on a xy plane, x being the groove line and L is the distance from P point to the equilibrium at y axis, I fail to see the importance of y-component of F, if any.
 
ah - I hadn't realized the question provided you with a diagram!

ok - then back to my two questions:

What is the total force in the spring at distance x along the groove?

So what is the component along the groove? :smile:
 
>What is the total force in the spring at distance x along the groove?
Fx^2+Fy^2=F^2>So what is the component along the groove?
Fx= Fcosineø =F x/d = F x/seqroot(x^2+L^2)

..and the above should equal to (-kx)??
 
yasar1967 said:
>What is the total force in the spring at distance x along the groove?
Fx^2+Fy^2=F^2


>So what is the component along the groove?
Fx= Fcosineø =F x/d = F x/seqroot(x^2+L^2)

..and the above should equal to (-kx)??

No no no … F isn't a constant, is it? … so that doesn't get you anywhere. :frown:

The question wants you to assume that the spring has a coefficient, of µ, say, and to work out the force as a function of µ.

(When you work out proportionality later on, the µ won't matter).

So what is the total force in the spring at distance x along the groove, in terms of µ? :smile:
 
it should be -kx cosineø (or -µx cosineø)
then
cosineø being: x/d=x/seqroot(x^2+L^2)
so
F=-(kx^2)/(seqroot(x^2+L^2))??
 
yasar1967 said:
it should be -kx cosineø (or -µx cosineø)
then
cosineø being: x/d=x/seqroot(x^2+L^2)
so
F=-(kx^2)/(seqroot(x^2+L^2))??

oops … I didn't see the letter k in the question. :redface:

But shouldn't it be k times the increased length of the spring? You've used x, which is only the sideways displacement.

(and don't forget to use the hint formula in the question.)
 
first of all thank you for the help, I appreciate.
ok, the force on the spring is F=-k(ɅL) (as ɅL is the increased length and if ɅL is zero so the force)
and that force's cosine component makes the mass M moves along the x-axis on the groove:
F=-k(ɅL)cosineø=-k(ɅL)x/seqroot(x^2+L^2)

from here where do I go?
 
  • #10
Hi yasar1967! :smile:

(btw, what symbol did you intend to put before the L? It came out as a square on my iMac.)

Well, you were asked to show that the restoring force on the block is proportional to x^3.

So from now on, it's just algebra.

You have force = -k(ɅL)x/√(x^2+L^2)

So now you write ɅL in terms of L and x.

Then you use the hint formula in the question, and you get … ? :smile:
 
  • #11
that was meant to be Delta: Ʌ
:)

thanks again for the help
 
  • #12
You're very welcome! :smile:

oh, and I get Delta on my iMac by pressing alt-j

Can you read that? (copy it, if you like.)

∆∆∆∆∆∆ :wink:
 

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