Graph of simple harmonic motion

AI Thread Summary
The discussion focuses on solving problems related to simple harmonic motion, specifically determining the time when the phase is pi/2, maximum velocity, maximum acceleration, and the time at which acceleration is maximized. Participants clarify that the period T does not equal 2pi, but rather relates to the radian frequency ω, where ω = 2π/T. To find the time for the phase of pi/2, the argument of the cosine function must equal pi/2, which leads to the conclusion that t is 1/4T. Additionally, maximum acceleration occurs when the argument of the cosine function equals 0 or pi. The conversation emphasizes the importance of understanding the mathematical relationships in simple harmonic motion to solve these problems effectively.
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Homework Statement



A particle moves with amplitude A and period T (see figure). Express the following in terms of A and T and numberical constants.
a) The time at which the phase is pi/2
b) maximum v
c) max a
d) time at which acceleration is a maximum

Homework Equations





The Attempt at a Solution


I got b and c, but I'm not sure about a and d.

For a, they ask for the time at which phase is pi/2. I know T = 2pi. For d, when acceleration is max, is time 0?

Can someone help me please?

THANKS
 

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T does not equal 2pi

\omega T = 2 \pi
and
\omega = \frac{2\pi}{T}
where omega is the radian frequency, because when you evaluate the sinusoid at t = T, the argument equals 2pi.

x(t) = cos(\omega t)
x(t) = cos(\frac{2\pi}{T}t)

Using this last equation, we can solve both a and d. For a, find a t that makes the argument pi/2. For d, differentiate twice to find acceleration and find the argument that maximizes acceleration.

you can use a more conceptual approach for both, however. For example, if you know how a cosine behaves, you can instantly know A just by looking at the graph.
 
xcvxcvvc said:
T does not equal 2pi

\omega T = 2 \pi
and
\omega = \frac{2\pi}{T}
where omega is the radian frequency, because when you evaluate the sinusoid at t = T, the argument equals 2pi.

x(t) = cos(\omega t)
x(t) = cos(\frac{2\pi}{T}t)

Using this last equation, we can solve both a and d. For a, find a t that makes the argument pi/2. For d, differentiate twice to find acceleration and find the argument that maximizes acceleration.

you can use a more conceptual approach for both, however. For example, if you know how a cosine behaves, you can instantly know A just by looking at the graph.

I'm not getting what you mean by finding a t that makes it pi/2. We don't have any values of t
 
for a, time has to be 1/4t.

is that right?
 
differentiating the equation twice gives acceleration = -A omega^2 cos (omega t)

amax = Aomega^2, so t has to be equal to 1?
 
mizzy said:
for a, time has to be 1/4t.

is that right?
no. the time at which a phase of pi/2 happens, t, will have T in it.
mizzy said:
differentiating the equation twice gives acceleration = -A omega^2 cos (omega t)

amax = Aomega^2, so t has to be equal to 1?

no. wt must equal 0 or pi for |a(t)| to be maximum.
 
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