Simple Harmonic Motion: Mass on a Spring Homework Solution

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SUMMARY

The discussion focuses on demonstrating that a mass attached to a spring executes simple harmonic motion (SHM) when displaced from its equilibrium position. The net force acting on the mass is expressed as F_net = -k(y - y_0) - mg, where k is the spring constant, y is the position of the mass, and g is the acceleration due to gravity. The relationship between force and displacement confirms that the motion is harmonic, and the period of oscillation can be derived in terms of y_0 and g. The final equation derived indicates the acceleration is proportional to the displacement from the equilibrium position, affirming the SHM characteristics.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with the concepts of force and equilibrium
  • Knowledge of simple harmonic motion (SHM) principles
  • Basic understanding of spring constants and oscillatory motion
NEXT STEPS
  • Study the derivation of the period of oscillation for a mass-spring system
  • Learn about the relationship between force and displacement in SHM
  • Explore the mathematical formulation of SHM, including angular frequency (ω)
  • Investigate real-world applications of SHM in mechanical systems
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and oscillatory motion, as well as educators seeking to explain the principles of simple harmonic motion in practical scenarios.

bmb2009
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Homework Statement


A massless spring hangs down from a support, with its lower end at y=0, where the y-axis is vertical and points downward (normal orientation of y). When a small unknown mass is attached to the spring, the lower end of the spring moves down to a position y_0 for the mass being in equilibrium

a.) Demonstrate that when the mass is pulled down to a position of y=y_0 + A and released from rest, it will execute a simple harmonic motion around y_0

b.) Express the period of oscillations of the mass in terms of y_0 and g.



Homework Equations





The Attempt at a Solution



Not really sure what/how to demonstrate that it executes s.h.m. I set up a force equation such that F_net= F_restoring - mg

F_net= -k(y-y_0) - mg
let Y be acceleration
mY= -k(y-y_0) - mg

mY=-kA-mg definfe ω^2 = k/m

Y=-(ω^2)A - g is the final equation i got... not sure how this proves anything and not really sure what to do.. any help? thanks
 
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bmb2009 said:
a.) Demonstrate that when the mass is pulled down to a position of y=y_0 + A and released from rest, it will execute a simple harmonic motion around y_0

b.) Express the period of oscillations of the mass in terms of y_0 and g.

Not really sure what/how to demonstrate that it executes s.h.m.
Start with the definition of SHM.
I set up a force equation such that F_net= F_restoring - mg

F_net= -k(y-y_0) - mg
Good start - how is the force related to displacement? Use words - and relate it to the definition of SHM.
 

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