Calculating Energy in Simple Harmonic Motion: Mass-Spring System

AI Thread Summary
The discussion revolves around calculating the total energy of a mass-spring system in simple harmonic motion, where a mass is attached to a spring and oscillates after being displaced from its equilibrium position. The key equation to prove is that the total energy is (1/2)k{Delta L^2 + A^2} + mgh, incorporating gravitational potential energy and elastic potential energy. Participants highlight the importance of understanding the energy transformations at various points in the oscillation, particularly at equilibrium and the extreme positions. The challenge lies in integrating Delta L into the energy calculations and proving the total energy remains constant throughout the motion. Ultimately, the discussion emphasizes the need for a clear understanding of kinetic, elastic potential, and gravitational potential energies in the context of harmonic motion.
doc1388
Messages
2
Reaction score
0

Homework Statement


A mass "m" is attached to the free end of a light vertical spring (unstretched length L) of spring contant "k" and suspended from a ceiling. The spring streches by Delta L under the load and comes to equilibrium at a height "h" above the ground level (y=0). The mass is pushed up vertically by "A" from its equilibrium position and released from rest. The mass-spring executes vertical oscillations. Assuming that gravitational potential energy of the mass "m" is zero at the ground level, show that the total energy of the spring-mass system is (1/2)k{Delta L^2 + A^2} + mgh.


Homework Equations


x(t)= Asin(Omega t + phi)
v(t)= wAcos(Omega t +phi)
Total Energy = 1/2 k A^2
Delta L k = mg

Hint: Draw four sketches of the vertical free spring, spring-mass in equilibrium, and the two extreme positions of oscillation of the mass. Below each of the above sketches (except free spring) write equations for Kinetic Energy, Elastic Potential Energy, Gravitational Potential Energy and Total Energy using symbols k, Delta L, m, A, g, h and v_m_

The Attempt at a Solution


I am struggling trying to find where Delta L fits into this equation. I understand the change in energies at the top and bottom are both full PE and GravPE and while it passes through equilibrium the KE is max because velocity is max. I just don't know how to even go about this problem I guess. I've labeled my drawing with the differences in h where at equilibrium y=h and the top y=h+A and at the bottom y=h-A. I'm lost. HELP please. Thank you in advance.
 
Physics news on Phys.org
I have attempted a bit more to this and I believe at equilibrium the total energy of the system is split up into three parts: Kinetic Energy is 1/2 m v_max_^2 + Elastic Potential Energy which is 1/2 k Delta L^2 + mgh

This is the answer if I sub in Omega and such and cancel masses I end up with the answer. But this is only the answer for equilibrium and I can't prove it is true at the extrema.

Any ideas?
 
I multiplied the values first without the error limit. Got 19.38. rounded it off to 2 significant figures since the given data has 2 significant figures. So = 19. For error I used the above formula. It comes out about 1.48. Now my question is. Should I write the answer as 19±1.5 (rounding 1.48 to 2 significant figures) OR should I write it as 19±1. So in short, should the error have same number of significant figures as the mean value or should it have the same number of decimal places as...
Thread 'A cylinder connected to a hanging mass'
Let's declare that for the cylinder, mass = M = 10 kg Radius = R = 4 m For the wall and the floor, Friction coeff = ##\mu## = 0.5 For the hanging mass, mass = m = 11 kg First, we divide the force according to their respective plane (x and y thing, correct me if I'm wrong) and according to which, cylinder or the hanging mass, they're working on. Force on the hanging mass $$mg - T = ma$$ Force(Cylinder) on y $$N_f + f_w - Mg = 0$$ Force(Cylinder) on x $$T + f_f - N_w = Ma$$ There's also...
Back
Top