Simple harmonic motion (finding omega)

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SUMMARY

A particle executing simple harmonic motion with an amplitude of 2.51 cm reaches a speed equal to half of its maximum speed at a specific positive displacement from the midpoint. The maximum speed is defined as v_{max} = Aw, where A is the amplitude and w is the angular frequency. The energy conservation equation (1/2)kA^2 - (1/2)kx^2 = (1/2)mv^2 can be utilized to find the displacement x without needing to calculate w or k directly. The solution confirms that not all constants are necessary to determine the displacement at which the velocity is half its maximum value.

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  • Understanding of simple harmonic motion principles
  • Familiarity with the equations of motion for harmonic oscillators
  • Knowledge of energy conservation in mechanical systems
  • Basic algebra for manipulating equations
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  • Study the derivation of the energy conservation equation in simple harmonic motion
  • Learn about angular frequency w and its relation to spring constant k and mass m
  • Explore the relationship between displacement and velocity in harmonic motion
  • Investigate the effects of varying amplitude on the motion of oscillating systems
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Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators seeking to clarify concepts related to simple harmonic motion.

SteroidalPsyc
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Homework Statement


A particle executes simple harmonic motion with an amplitude of 2.51cm. At what positive displacement from the midpoint of its motion does its speed equal one half of its max speed?


Homework Equations


A=2.51 cm
x(t) = Acos(wt)
v(t) = -Awsin(wt)
vmax = |-Aw|


The Attempt at a Solution


I just want to know how to find w so I can plug it into the vmax equation.
 
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SteroidalPsyc said:

Homework Statement


A particle executes simple harmonic motion with an amplitude of 2.51cm. At what positive displacement from the midpoint of its motion does its speed equal one half of its max speed?

Homework Equations


A=2.51 cm
x(t) = Acos(wt)
v(t) = -Awsin(wt)
vmax = |-Aw|

The Attempt at a Solution


I just want to know how to find w so I can plug it into the vmax equation.

You actually don't need to plug it in. If v_{max} = Aw then \frac{v_{max}}{2} = \frac{Aw}{2}

Just use the energy equation

\frac{1}{2}kA^2 - \frac{1}{2}kx^2 = \frac{1}{2}mv^2

where v= \frac{Aw}{2}, and remember to sub \frac{k}{m} for w^2.
 
Last edited:
novop said:
You actually don't need to plug it in. If v_{max} = Aw then \frac{v_{max}}{2} = \frac{Aw}{2}

Just use the energy equation

\frac{1}{2}kA^2 - \frac{1}{2}kx^2 = \frac{1}{2}mv^2

where v= \frac{Aw}{2}, and remember to sub \frac{k}{m} for w^2.

I don't know what k is though. How do I find k?
 
Divide both sides by k!
 
O ok haha sorry I'm really tired. Thanks for the help I solved it!
 
You don't need the velocity or the angular frequency in order to answer the question. You're only asked at what displacement the velocity has half its maximum value.

x=A\cos{(\omega t)}

v=-\omega A \sin{(\omega t)}

v=-\omega A \sqrt{(1-\cos ^2 {(\omega t))}}

v = -\omega \sqrt{(A^2-x^2)}

|v|=\tfrac{1}{2} v_{max}=\tfrac{1}{2}\omega A

\tfrac{1}{2}\omega A = \omega \sqrt{(A^2-x^2)}

You don't always need all the constants involved in a problem in order to solve for a particular value. :)
 

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