Simple Harmonic Motion: 5kg Particle Suspended by 500 N/m String

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SUMMARY

A 5 kg particle suspended by a light elastic string with a spring constant of 500 N/m exhibits simple harmonic motion (SHM) when displaced 20 cm from its equilibrium position. The equilibrium condition is established when the gravitational force (F_g = mg = 50 N) equals the elastic force (F_e = kΔy). The net force acting on the particle, when released, is proportional to its displacement from equilibrium, confirming SHM. The equation of motion derived is F_net = 500(y - 0.10), demonstrating the linear relationship required for SHM.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Knowledge of Hooke's Law and elastic forces
  • Familiarity with the concepts of equilibrium and net force
  • Basic proficiency in solving differential equations related to motion
NEXT STEPS
  • Study the derivation of the equations of motion for simple harmonic oscillators
  • Learn about the energy conservation principles in SHM
  • Explore the effects of damping on simple harmonic motion
  • Investigate real-world applications of SHM in engineering and physics
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Students of physics, mechanical engineers, and anyone interested in the principles of oscillatory motion and its applications in real-world scenarios.

markosheehan
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A particle of mass 5 kg is suspended from a fixed point by a light elastic string
which hangs vertically. The elastic constant of the string is 500 N/m.
The mass is pulled down a vertical distance of 20 cm from the equilibrium
position and is then released from rest.
(i) Show that the particle moves with simple harmonic motion.
 
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markosheehan said:
A particle of mass 5 kg is suspended from a fixed point by a light elastic string
which hangs vertically. The elastic constant of the string is 500 N/m.
The mass is pulled down a vertical distance of 20 cm from the equilibrium
position and is then released from rest.
(i) Show that the particle moves with simple harmonic motion.

Hi markosheehan! ;)

An elastic string provides a force that is linear with the displacement from the rest position.
As a consequence we have simple harmonic motion.
If we want to prove it, we have to set up the equation of motion and solve it.
Care to give it a try?

For the record, we expect some kind of attempt or explanation where you're stuck, if only to figure out how to help you best.
 
what i tryed to do was find the force down and the force up find the resultant force and let it equal to F=5a and then that would prove it but to do this when i am finding the force in the string i need the natural length of the string but it is not given in the question. to find the force up i use F=k(length-natural length)
 
markosheehan said:
what i tryed to do was find the force down and the force up find the resultant force and let it equal to F=5a and then that would prove it but to do this when i am finding the force in the string i need the natural length of the string but it is not given in the question. to find the force up i use F=k(length-natural length)

We don't need the natural length.
When the string has its natural length, the elastic force is zero.
The elastic force is proportional with the change in its natural length.

So let's start with the position in equilibrium.
Then the force of gravity is equal and opposite the elastic force.
That is:
$$F_g = F_e \quad\Rightarrow\quad mg = k\Delta y \quad\Rightarrow\quad 50 = 500 \Delta y\quad\Rightarrow\quad \Delta y = 0.10 \text{ m}$$

Now initially we pull the mass $20 \text{ cm}$ down and we let go.
Then we have:
$$F_{net} = F_e - F_g = ky-mg = 500y-50 = 500(y-0.10)$$

In other words, the net force is proportional to the distance from the equilibrium position.
 

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