Energy Integral Lemma-Differential Eq. HW

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SUMMARY

The discussion focuses on applying the energy integral lemma to demonstrate the behavior of free undamped mass-spring oscillators and pendulum motions. The key equation derived for the mass-spring system is m(y')² + ky² = constant, confirming that the total mechanical energy remains constant. The user successfully identifies the function f(y) as -k/m for the mass-spring system and -g/l sin(θ) for the pendulum, leading to the conclusion that both systems adhere to the energy conservation principle. The discussion emphasizes the importance of correctly applying the energy integral lemma in solving differential equations.

PREREQUISITES
  • Understanding of differential equations, specifically second-order linear ODEs.
  • Familiarity with the energy integral lemma and its application in mechanics.
  • Knowledge of mechanical systems, including mass-spring oscillators and pendulums.
  • Basic calculus, particularly integration and differentiation techniques.
NEXT STEPS
  • Study the derivation and application of the energy integral lemma in various mechanical systems.
  • Learn about the characteristics of simple harmonic motion and its mathematical representation.
  • Explore the relationship between potential and kinetic energy in oscillatory systems.
  • Investigate the stability and behavior of nonlinear pendulum systems using energy methods.
USEFUL FOR

Students and educators in physics or engineering, particularly those studying dynamics and mechanical systems, will benefit from this discussion. It is also valuable for anyone looking to deepen their understanding of energy conservation in oscillatory motion.

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Homework Statement


Use the energy integral lemma to show that motions of the free undamped mass-spring oscillator my"+ky=0 objey

m(y')^2 = ky^2=constant


Homework Equations



E(t)=1/2 y'(t)^2 - F (y(t))

The Attempt at a Solution


I am not sure how to even start this problem.I would like to know just what the problem is asking for.I do not have a problem doing the math to it.

Thank you
 
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If I remember correctly, the energy integral lemma says that the quantity E(t)=1/2 y'(t)^2 - F (y(t)) is a constant when y(t) satsifies the DE y''(t)=f(y) and f(y) has no explicit dependence on y' or t and F(y)=\int f(y)dy... So, I would start by placing your ODE in the form y''(t)=f(y)...what is f(y) in this case? Does it have any explicit dependence on y' or t? If not, then E(t)=1/2 y'(t)^2 - F (y(t)) is a constant.
 
so is my f(y)=-ky/m then i get the F(y) of that expression and plug into E(t)=
 
Yes, what does that give you?
 
1st of all i apologize since i don't know how to write equation symbol and such..

here is what i get

y=-ky/m

-k/m integral (y)= -k/m (y^2)/2

(1/2)y'^2 - k/m(y^2)/2=k

then i am trying to solve for y'^2 so
i end up with

my'^2 =2km +ky^2

and what i am suppose to get is m (y'^2) +ky^2 =constant.
 
so i realized i messed up my negative there since the original lemma has a negative and my f(y) has a negative so i end up with


my'^2 + ky^2 =2km

is it okay to re-write that expression as my'^2 + ky^2=constant since usually the values of k and m are #'s?

so it would be my'^2 + ky^2 = constant

??
 
Okay,I figured it out my question out.I don't know why i was adding an extra K.Thanks for guiding me through it.

I have another question if you could just help me with setting it up.
it involves the energy lemma .

the question is
Use the energy integral lemma to show that pendulum motions obey

(theta prime)^2 /2 - (g/l)cos(theta) = C

what is my f(y) in this case?
 
okay so i think i figured out this one too:

i did

(theta)"^2/2= [(g/l)cos(theta) ]'

(theta)"^2/2= -g/l sin(theta)

f(y)= -g/l sin(theta)

then after going through all the steps i ended up with

(theta)'^2 /2 - (g/l)cos(theta)=C which is the original DE.


let me know if this is okay.i am not sure if taking the 2nd derivative of the equation is allowed.
 

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