Energy Integral Lemma-Differential Eq. HW

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Homework Help Overview

The discussion revolves around the application of the energy integral lemma to demonstrate properties of motion in a free undamped mass-spring oscillator and a pendulum. Participants are exploring the relationships between energy expressions and differential equations in these contexts.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the formulation of the energy integral lemma and its application to the given differential equations. Questions arise regarding the identification of functions and constants within the equations, as well as the interpretation of results. There is an exploration of how to express energy conservation in terms of constants.

Discussion Status

Some participants have made progress in understanding the problem and have clarified their approaches. There is a recognition of the need to accurately identify functions and constants, with some guidance provided on how to set up the equations. Multiple interpretations of the energy lemma are being explored, particularly in relation to different physical systems.

Contextual Notes

Participants express uncertainty about the notation and the steps involved in deriving the energy expressions. There is an acknowledgment of potential errors in earlier calculations, which are being corrected as the discussion progresses.

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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 [itex]F(y)=\int f(y)dy[/itex]... 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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