Calculating Position in Simple Harmonic Motion with Given Amplitude and Velocity

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SUMMARY

The discussion focuses on calculating the position of a particle in simple harmonic motion (SHM) when its velocity is half of the maximum speed. The particle has an amplitude of 3 cm, and the maximum speed is derived using the formula vmax = ωA, where ω is the angular frequency. The total energy of the system is conserved, allowing for the calculation of position using energy equations. Ultimately, the position when the velocity is half the maximum speed is determined to be x = √(3/4) A.

PREREQUISITES
  • Understanding of simple harmonic motion (SHM)
  • Familiarity with energy conservation principles in physics
  • Knowledge of angular frequency (ω) and its relation to amplitude (A)
  • Ability to manipulate algebraic equations involving kinetic and potential energy
NEXT STEPS
  • Study the derivation of the equations for simple harmonic motion
  • Learn about energy conservation in oscillatory systems
  • Explore the relationship between amplitude, frequency, and maximum velocity in SHM
  • Investigate the effects of mass and spring constant on the motion of a mass-spring system
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillations, as well as educators teaching simple harmonic motion concepts.

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Homework Statement



A moving particle displays simple harmonic motion with an amplitude of 3 cm. What position will it be for it to have half of its maximum speed?


Homework Equations



vmax= omega*A

The Attempt at a Solution



I divided the amplitude by 2 but I believe that's an incorrect method. was i suppose to deriviate x(t)=omega*A*sin(omega*t+phi)
 
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I'm going to assume that the particle acts like a mass on a spring. Then, we can solve this problem using conservation of energy.

At the system's biggest displacement (3cm), there is no kinetic energy, so the total energy of the system is just the energy from the spring:

[tex]E_{tot} = \frac{1}{2} k A^2[/tex]​

At the equilibrium point, there is no spring energy. All of the energy is kinetic. Then, we can find the maximum velocity:

[tex]E_{tot} = \frac{1}{2} m v_{max}^2[/tex]

[tex]\frac{1}{2} k A^2 = \frac{1}{2} m v_{max}^2[/tex]

[tex]\sqrt{\frac{k}{m}} A = v_{max}[/tex]​

Note that [tex]\sqrt{k/m}[/tex] is usually called [tex]\omega[/tex], so this is simply the equation you gave us in your post.

Now, we want to find the position of the mass when the velocity is half max. At that point, there is both spring energy and kinetic energy.

[tex]E_{tot} = \frac{1}{2} k x^2 + \frac{1}{2} m \left( \frac{v_{max}}{2} \right)^2[/tex]

[tex]\frac{1}{2} k A^2 = \frac{1}{2} k x^2 + \frac{1}{2 \cdot 4} m \frac{k}{m} A^2[/tex]

[tex]A^2 = x^2 + \frac{1}{4} A^2[/tex]

[tex]\frac{3}{4} A^2 = x^2[/tex]

[tex]\sqrt{\frac{3}{4}} A = x[/tex]​

So, the position of the mass when it's traveling at half the maximum speed is [tex]x = \sqrt{\frac{3}{4}} A[/tex].
 

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