Finding (C): Halfway Between Equilibrium and End Point

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Homework Help Overview

The discussion revolves around understanding the motion of an object in simple harmonic motion, specifically focusing on the time intervals between various points in its cycle. Participants are exploring the relationship between equilibrium and endpoint positions, as well as the time taken to traverse specific segments of the motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the concept of halfway points in motion and question the appropriateness of certain time intervals. There is an exploration of the symmetry in simple harmonic motion and how it relates to time calculations. Some participants suggest methods for determining specific time intervals based on the sine function.

Discussion Status

The discussion is active, with participants sharing different perspectives on the problem. Some have proposed methods for calculating time intervals, while others are questioning the assumptions and definitions related to the motion. There is no explicit consensus, but various approaches are being examined.

Contextual Notes

Participants are working within the constraints of homework guidelines, which may limit the information they can share or the methods they can use. The discussion includes assumptions about the nature of the motion and the mathematical representation of the system.

hidemi
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Homework Statement
A particle is in simple harmonic motion with period T. At time t = 0 it is halfway
between the equilibrium point and an end point of its motion, traveling toward the
end point. The next time it is at the same place is:
A. t =T
B. t =T/2
C. t =T/3
D. t = T/4
E. none of the above

The answer is C
Relevant Equations
X = A cos(wt+c)
I think (D) is correct since it is half way between the equilibrium point and and the end point of its motion, it is a quarter of the total distance. How to get (C)?
 
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I think t=T is ,though not least, the time it is in the same place. B to D are inappropriate because halfway means anywhere between the top and the bottom.
 
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can you find the angle between ##t_{1}## and ##t_{2}##
time.jpg
 
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Suppose the motion is between points A and B:

A P O Q B

The centre is O , the end points are A and B.
P is the midpoint of AO.
Q is the midpoint of OB.

Say we want the time for Q→B→Q.

The following times are equal:
##T_{OB} = T_{BO} = T_{OA} = T_{AO} = \frac T 4##
This a due to the inherent symmetry in a cycle of simple harmonic motion. It can be seen by looking at the shape of a sine curve.

But ##T_{AP}, T_{PO}##, etc. are not equal to any 'obvious' value (not ##\frac T 8## for example). Look at a sine curve carefully.

With O at x=0, taking x=0 when t=0 and assuming velocity at t=0 is positive, we can describe the motion by:$$x(t) = Asin \left[ \left( \frac {2\pi} T \right) t \right]$$(Using sine rather than cosine is most convenient here.)

Suppose we want ##T_{QB}##. (The required ‘return time' will be twice this.)

I think the simplest method to find ##T_{QB}## is first to find ##T_{OQ}## and then subtract it from ##T_{OB}## (since we already know that ##T_{OB} =\frac T 4##).

The position of Q is x = ##\frac A 2## which gives:$$\frac A 2 = Asin \left[ \left( \frac {2\pi} T \right) T_{OQ} \right]$$Solve for ##T_{OQ}##. And take it from there.

Someone might post a simpler method, but the above method is easier than it might initially appear!
 
Last edited:
Steve4Physics said:
Suppose the motion is between points A and B:

A P O Q B

The centre is O , the end points are A and B.
P is the midpoint of AO.
Q is the midpoint of OB.

Say we want the time for Q→B→Q.

The following times are equal:
##T_{OB} = T_{BO} = T_{OA} = T_{AO} = \frac T 4##
This a due to the inherent symmetry in a cycle of simple harmonic motion. It can be seen by looking at the shape of a sine curve.

But ##T_{AP}, T_{PO}##, etc. are not equal to any 'obvious' value (not ##\frac T 8## for example). Look at a sine curve carefully.

With O at x=0, taking x=0 when t=0 and assuming velocity at t=0 is positive, we can describe the motion by:$$x(t) = Asin \left[ \left( \frac {2\pi} T \right) t \right]$$(Using sine rather than cosine is most convenient here.)

Suppose we want ##T_{QB}##. (The required ‘return time' will be twice this.)

I think the simplest method to find ##T_{QB}## is first to find ##T_{OQ}## and then subtract it from ##T_{OB}## (since we already know that ##T_{OB} =\frac T 4##).

The position of Q is x = ##\frac A 2## which gives:$$\frac A 2 = Asin \left[ \left( \frac {2\pi} T \right) T_{OQ} \right]$$Solve for ##T_{OQ}##. And take it from there.

Someone might post a simpler method, but the above method is easier than it might initially appear!
I got it! Thanks so much!
 

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