Understand Hooke's Law and Spring Dynamics

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SUMMARY

This discussion focuses on Hooke's Law and the dynamics of springs, particularly in scenarios involving kinetic energy and gravitational potential energy. When an object with a velocity of 4 m/s compresses a spring with a spring constant (k) of 2, the time taken for compression can be determined using simple harmonic motion (SHM) principles. The compression differs based on whether the object is moving vertically or horizontally due to the influence of gravity, which adds potential energy to the system. The derived formula for the time to maximum compression is t = (π/2)√(m/k), indicating that it solely depends on the mass of the object and the spring constant, independent of the initial velocity.

PREREQUISITES
  • Understanding of Hooke's Law and spring dynamics
  • Basic principles of kinetic and potential energy
  • Knowledge of simple harmonic motion (SHM)
  • Familiarity with differential equations and their solutions
NEXT STEPS
  • Study the principles of simple harmonic motion (SHM) in detail
  • Learn about the energy conservation in spring systems
  • Explore the effects of gravitational potential energy on spring dynamics
  • Investigate differential equations related to oscillatory motion
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in understanding the dynamics of springs and oscillatory motion in various contexts.

daveed
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allright, here is something i haven't been able to understand with just hooke's law

if i have an object traveling at velocity v, let's say, 4m/s , and hits a spring at, i don't know, k=2? so then we know how far the spring compresses and all because you just need to set the work done and kinetic energy equal, but what i have not been able to get is how long does it take for it to compress? because with a changing force(and so a changing acceleration), i don't understand how to find the time it takes to stop the thing

also, when your talking about a ball bouncing up and hitting a spring, the compression would not be the same as if it had happened on a horizontal surface, because gravity would also be doing work on the ball too, right?
 
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if the object comes and hits the spring again(after being pulled down by gravity) and hits the spring out of phase, will you still need to take the work done by the spring? also, what if it- let's take this with a spring vibrating up and down now- hits the spring above the equillibrium point, where the force on the end of the spring is downwards? how does the object behave then?
 
daveed said:
also, when your talking about a ball bouncing up and hitting a spring, the compression would not be the same as if it had happened on a horizontal surface, because gravity would also be doing work on the ball too, right?

YES, of course the compression will be diffrent because of the gravity's force...
In this situation you don't only have kinetic energy but you have the gravity potential energy as well. The equation will be this then .5kx^2=.5mV2+mgh (in the vertical bouncing)...
but if it ball is traveling a horizontal distance you don't have gravity's potential energy hence the x would be less...

I hope I realized your question correctly..
 
daveed said:
allright, here is something i haven't been able to understand with just hooke's law

if i have an object traveling at velocity v, let's say, 4m/s , and hits a spring at, i don't know, k=2? so then we know how far the spring compresses and all because you just need to set the work done and kinetic energy equal, but what i have not been able to get is how long does it take for it to compress? because with a changing force(and so a changing acceleration), i don't understand how to find the time it takes to stop the thing

also, when your talking about a ball bouncing up and hitting a spring, the compression would not be the same as if it had happened on a horizontal surface, because gravity would also be doing work on the ball too, right?

F=-kx(t)=m\frac{d^2x(t)}{dt^2} (Newtons second law F=ma)

This is a differential equation with the general solution:
x(t)=Asin(\omega t)+Bcos(\omega t)

With \omega=\sqrt{k/m}[/tex]. Applying initial conditions; say x(t=0)=0<br /> x(t)=Asin(\omega t)<br /> <br /> The spring is totally compressed when:<br /> sin(\omega t)=1 so t=\frac{\pi}{2 \omega}=\frac{\pi}{2} \sqrt{m/k}<br /> <br /> And thus depends only on the mass of the object and the spring constant and not on the initial velocity of the object!
 

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