Calculating Total Energy in Simple Harmonic Motion

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Homework Help Overview

The discussion revolves around calculating the total energy of a mass undergoing simple harmonic motion, specifically a 2kg mass with an amplitude of 1cm and a frequency of 16Hz.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the use of the general solution for position in simple harmonic motion and the differentiation to find velocity. There are discussions about the necessity of the phase angle and how to incorporate potential energy into the total energy calculation.

Discussion Status

Some participants have provided guidance on considering both kinetic and potential energy in the context of simple harmonic motion. There is an acknowledgment of the original poster's approach, with suggestions to simplify certain aspects, such as the phase angle.

Contextual Notes

There are discussions about the assumptions related to potential energy and the conditions under which kinetic and potential energy are maximized or minimized. The conversation reflects a lack of consensus on the exact approach but indicates a productive exploration of the topic.

Lavace
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Homework Statement


Calculate the total energy of a 2kg mass that is undergoing simple harmonic motion with an amplitude of 1cm and and frequency of 16Hz.


Homework Equations


ma = -w^2x

The Attempt at a Solution



The first thing I thought was using the general solution of x(t) = A cos(wt + psi), differentiating to find the velocity (after the phase angle, or is this even needed?), and then using the value in K.E = 1/2mv^2?

Please help!
 
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That might work, but you also need to calculate the potential energy stored in the spring. You may already know the formula or you can find it by integrating the spring force over displacement (work done by the spring is minus the potential energy stored in the spring)
 
The equation you've written
ma = -w^2x
should read a=-w2x right?

ma=-kx
a=-(k/m)x
a=-w2x
where w2=(k/m)

Following JaWiB, potential energy is equal to the negative line integral of the force. U=-\int F dl, which will come out to a familiar equation you've probably seen before. Since you're given the maximum displacement (amplitude), consider the energy of the particle at its maximum displacement and at the point of equilibrium (x=0). At what points is the energy of the particle purely kinetic or purely potential? Then consider conservation of energy.
 
No integrals are needed here. The OP was right on track:
Lavace said:

The Attempt at a Solution



The first thing I thought was using the general solution of x(t) = A cos(wt + psi), differentiating to find the velocity (after the phase angle, or is this even needed?), and then using the value in K.E = 1/2mv^2?
Don't worry about the phase angle, you may assume it's zero for simplicity.
The tricky part is what to do about the potential energy. At some point (value of x) the potential energy is zero, which simplifies the calculation of total energy.
 

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