Simple Harmonic Motion problem 1

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Homework Help Overview

The problem involves simple harmonic motion (SHM) and focuses on the displacement of a particle under specific initial conditions. Participants are analyzing the appropriate equations to describe the motion, particularly questioning the validity of using sine or cosine functions for displacement when the particle starts from rest.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants discuss the implications of using different equations for SHM, such as x = A sin(ωt) versus x = A cos(ωt), and question whether these forms accurately represent a particle starting from rest. They explore the relationship between displacement, velocity, and acceleration at t = 0.

Discussion Status

The discussion is ongoing, with participants offering alternative equations and reasoning about the conditions of the problem. Some have suggested that the equation Δx = A(1 - cos(ωt)) may be appropriate, while others are still seeking clarity on the initial conditions and the correct form of the displacement function.

Contextual Notes

There is a focus on the initial conditions of the problem, particularly the requirement that the particle starts from rest, which influences the choice of equations for SHM. Participants are also considering the implications of displacement at t = 0 and how it relates to the physical setup of the problem.

thunderhadron
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Hi friends the problem is -

https://fbcdn-sphotos-a-a.akamaihd.net/hphotos-ak-snc6/s480x480/6405_2656465868185_1414230035_n.jpg

Attempt -

As per the problem states,

For the first second equation of SHM, (using x = A sin ωt)

a = A sin ω

From here I get, sin ω = a/ A --------------(1)

Using it for the 2 seconds, total displacement would be a + b. So,

a + b = A sin 2ω

i.e. a + b = 2A sin ω. cos ω

i.e. a + b = 2A sin ω. √1-sin2ω ----------------(2)

Solving both the equations, I am getting the result,

A = 2a2/ √(3a2 - b2 - 2ab)

But the correct answer of this problem is option (A) as per the question.

Please friends help me in solving this Problem.

Thank you all in advance.
 
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Note that the particle starts from rest. Does the equation x = Asinωt describe a particle starting from rest? (Assuming "start" means t = 0)
 
TSny said:
Note that the particle starts from rest. Does the equation x = Asinωt describe a particle starting from rest? (Assuming "start" means t = 0)

No, thaks. I have taken the eqn in wrong manner.

Let the equation be x = A cosωt

Solving, a = A cos ω

i.e. cosω = a/A

And (a + b) = A cos 2ω

i.e. (a + b) = A √(2cos2ω -1)

Soving both we get A = √(a2 - b2 -2ab)

Yet answer is not achieved
 
The distance traveled can not be x=Acos(ωt), as the distance traveled would be A at zero time, (it should be zero) and the velocity would be negative...

If x(t) is the position at time t, the velocity is v=dx/dt. The particle travels in the positive x direction, and it is velocity is zero at t=0. What should be the form of the displacement as function of t?

ehild
 
Creating such kind of function is really giving me problem. Please help me out.
 
What about Δx=A(1-cosωt)?

ehild
 
ehild said:
What about Δx=A(1-cosωt)?

ehild

Yes this function is proper for the question. I appreciate your help. I will try to find answer with its help and get back to you soon.
 
ehild said:
What about Δx=A(1-cosωt)?

ehild

I am currently doing SHM, I am willing to know how you arrived at that equation. :)
 
Pranav-Arora said:
I am currently doing SHM, I am willing to know how you arrived at that equation. :)

I think its answer.

In my notion he thought that -
We are not allowed to use x = A sin ωt or x = A cos ωt here because these functions are not giving the appropriate conditions according to question. But the function which can give correct answer for v = 0 at t = 0 is is x = A cos ωt. But it it is giving some displacement at t = 0.
so what it giving the displacement at t = 0. That is A. Subtract it from A and the displacement as well as the velocity both will be zero at t = 0.

Even I am not sure that the function is correct or not right now. I will solve it and then again will discuss about it.
 
  • #10
ehild said:
The distance traveled can not be x=Acos(ωt), as the distance traveled would be A at zero time, (it should be zero) and the velocity would be negative...
ehild

ehild,

Please tell me that why are saying that the displacement of the particle should be zero at t = 0 ?

If I stretch a spring mass system fro it mean position and hold it for some time and then release. So there the particle would have some displacement at t = 0. Isn't it ?
 
  • #11
ehild said:
What about Δx=A(1-cosωt)?

ehild

Thank you very much ehild I go the correct answer. But Please clear the doubt which raised earlier.

The function is absolutely correct.
 
  • #12
Pranav: The shm along x in general is x=A cos (ωt+θ). The displacement from the position at zero time is Δx=x-x0=Acos(ωt+θ)-x0.

The particle starts from rest, so v=-Aωsinθ=0. That means θ=0 or π.
It starts to move in the positive x direction, v should increase, so the acceleration at t=0 is positive: -Aω2cosθ>0, that is θ=π.
cosθ=-1, but the displacement is zero if x0=Acosθ=-A.
So you can write up the displacement as Δx=Acos(ωt+π)+A=A(1-cosωt).ehild
 
  • #13
thunderhadron said:
ehild,

Please tell me that why are saying that the displacement of the particle should be zero at t = 0 ?

If I stretch a spring mass system fro it mean position and hold it for some time and then release. So there the particle would have some displacement at t = 0. Isn't it ?

Displacement is the change of position Δx=x(t)-x(0). Of course, it is zero at t=0. It is not meant as the change of length of a spring here.

We start measuring time when the particle has zero velocity. Assuming a general SHM x(t)=Acos(ωt+θ), we can get theta from the conditions given, that the initial velocity is zero, and the particle has positive velocity after. Read my previous post.

ehild
 
  • #14
ehild said:
Pranav: The shm along x in general is x=A cos (ωt+θ). The displacement from the position at zero time is Δx=x-x0=Acos(ωt+θ)-x0.

The particle starts from rest, so v=-Aωsinθ=0. That means θ=0 or π.
It starts to move in the positive x direction, v should increase, so the acceleration at t=0 is positive: -Aω2cosθ>0, that is θ=π.
cosθ=-1, but the displacement is zero if x0=Acosθ=-A.
So you can write up the displacement as Δx=Acos(ωt+π)+A=A(1-cosωt).


ehild

Thanks ehild! :smile:
 
  • #15
ehild said:
The shm along x in general is x=A cos (ωt+θ). The displacement from the position at zero time is Δx=x-x0=Acos(ωt+θ)-x0.

The particle starts from rest, so v=-Aωsinθ=0. That means θ=0 or π.
It starts to move in the positive x direction, v should increase, so the acceleration at t=0 is positive: -Aω2cosθ>0, that is θ=π.
cosθ=-1, but the displacement is zero if x0=Acosθ=-A.
So you can write up the displacement as Δx=Acos(ωt+π)+A=A(1-cosωt).


ehild

Very nice explanation.
 

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