Regarding Energy and Work done in a Spring Mass System

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SUMMARY

The discussion focuses on analyzing a spring mass system where a displacement defined as u=sin(ωt) is applied instead of an external force. The key equations include the equation of motion m*a(t) + k*u(t) = F(u) and the total work done expressed as ∫[F(u)*du] over a time interval Δt. The user attempts to equate total work done with the changes in kinetic energy (KE) and potential energy (PE) but encounters discrepancies, indicating a misunderstanding in the relationship between work and energy in this context.

PREREQUISITES
  • Understanding of classical mechanics principles, particularly energy conservation.
  • Familiarity with spring dynamics and Hooke's Law.
  • Knowledge of calculus, specifically integration techniques.
  • Experience with differential equations related to motion.
NEXT STEPS
  • Review the principles of energy conservation in mechanical systems.
  • Study the derivation of the work-energy theorem in the context of spring systems.
  • Learn about the application of Fourier series in analyzing periodic functions like u=sin(ωt).
  • Explore numerical methods for solving differential equations related to spring mass systems.
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Students and educators in physics, mechanical engineers, and anyone interested in understanding the dynamics of spring mass systems and energy relationships in mechanical systems.

S S Gautam
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Homework Statement


I am trying to solve a spring mass system (mass m and constant spring stiffness k) where instead of applied force a displacement is applied as u=sin(ωt) where ω is the frequency and t is the time. I need to find the difference of the total work done and the energy (KE and PE) of the system. The spring constant is k and the mass of the spring is m. The spring is tied at one end and at the other end mass is attached to which the displacement u is applied.

Homework Equations



The equation of motion is m*a(t) + k *u(t) = F(u) where F(u) is the unknown force which depends on the displacement applied u.

The total work done during a time interval Δt is given by ∫[F(u)*du] with limits from t to t + Δt.

The total change in the KE (=ΔKE) and PE (=ΔPE) is (I think) given by ΔKE = 0.5*m*(V_t+Δt - V_t)^2 and ΔPE as 0.5*k*(u_t+Δt-u_t)^2.

The Attempt at a Solution


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Now, since there is no dissipation the total work done, W, from t to t + Δt should be equal to ΔKE+ΔPE i.e. change in KE and PE from t to t + Δt . I am calculating the work done as integral from t to t + Δt of F(u)*du where F(u) = m*a + k*u where a = double derivative of u. The change in KE and PE is computed from the formula ΔKE = 0.5*m*(V_t+Δt - V_t)^2 and ΔPE as 0.5*k*(u_t+Δt-u_t)^2. However, I do not get W = ΔKE+ΔPE. I have also tried getting the ΔKE and ΔPE using the integration from t to t+Δt. Can somebody suggest what is wrong that I am doing.

Your advice, suggestions is highly appreciated.

Thank you.
 
S S Gautam said:
I need to find the difference of the total work done and the energy (KE and PE) of the system.
What does this mean? Difference between what and what? Please quote the problem in its original.
 

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