Solving Harmonic Oscillator Equation w/ Initial Conditions

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Homework Help Overview

The discussion revolves around solving the harmonic oscillator equation for a mass-spring system with initial conditions. The original poster describes a scenario where a mass is placed on a spring connected to the ceiling, and the spring is released by cutting the wire at time t=0. The problem involves deriving the equation of motion and solving it under specified initial conditions.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants explore the application of Newton's second law to derive the motion equation. There are discussions about defining equilibrium points and the implications of initial conditions. Questions arise regarding the meaning of variables and the correct formulation of the differential equation in terms of the new variable y.

Discussion Status

Participants are actively engaging with the problem, questioning assumptions about equilibrium and the definitions of variables. Some guidance has been offered regarding rewriting the differential equation, but there is still uncertainty about the correct formulation and interpretation of the variables involved.

Contextual Notes

There is confusion regarding the variable 'c' and its role in the equilibrium condition. Participants are also grappling with how to correctly express the differential equation for the new variable y, which is defined in relation to x.

quas
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Homework Statement


a mass is placed on a loose spring and connected to the ceiling. the spring is connected to the floor in t=0 the wire is cut
a. find the equation of the motion
b. solve the equation under the initial conditions due to the question
שאלה לפורום.JPG

Homework Equations


## \sum F=ma
##
## x(t)=Asin(\omega t + \phi ) ##

The Attempt at a Solution


a. due to the 2 law of Newton: ## \sum F=ma_x
##
## mg-kx=ma ##
##
mg-kx=m\ddot{x}
\\
\ddot{x}=g-\frac{k}{m}x ##

b. first I'll find the point equilibrium
##
c-kx=ma
\\
c-kx=m\cdot 0
\\
x_0=\frac{c}{k}

##

then I'll define ## y=x-x_0 ##

How do I go from here?
thanks
 
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quas said:
##\ddot{x}=g-\frac{k}{m}x ##
OK

##x_0=\frac{c}{k}##
What does c stand for?

then I'll define ## y=x-x_0 ##

How do I go from here?
Rewrite the differential equation in terms of y instead of x.
 
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As TSny hints, you tripped finding x0. Think again what condition will be true at equilibrium and define x0 again. There won't be an unknown c.
 
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TSny said:
OK

What does c stand for?Rewrite the differential equation in terms of y instead of x.
sorry I meant ## x_0 = \frac{mg}{k}##
ok and then ## \ddot{y}=g-\frac{k}{m}y ## ?
 
Last edited:
##
\ddot{y}=g-\frac{k}{m}y## can't be right. Compare with ##
\ddot{x}=g-\frac{k}{m}x##
 
BvU said:
##
\ddot{y}=g-\frac{k}{m}y## can't be right. Compare with ##
\ddot{x}=g-\frac{k}{m}x##
I might have a barrier but I do not understand how to build a differential equation for y,,,,
I understand that ## \dot{x}=\frac{dx}{dt}=\frac{dy}{dt}=\dot{y} \\ a=\ddot{x}=\frac{d^2x}{dt^2}=\frac{d^2y}{dt^2}=\ddot{y} ##
 
BvU said:
##
\ddot{y}=g-\frac{k}{m}y## can't be right. Compare with ##
\ddot{x}=g-\frac{k}{m}x##
? I must be thick this morning, but if positive y is down that looks ok to me.
 
Cutter Ketch said:
? I must be thick this morning, but if positive y is down that looks ok to me.

Oh, good grief. It took me a minute!
 
quas said:
I might have a barrier but I do not understand how to build a differential equation for y,,,,
I understand that ## \dot{x}=\frac{dx}{dt}=\frac{dy}{dt}=\dot{y} \\ a=\ddot{x}=\frac{d^2x}{dt^2}=\frac{d^2y}{dt^2}=\ddot{y} ##

Much later after it stops oscillating and y is y0 what is the acceleration? g?
 
  • #10
quas said:
I might have a barrier but I do not understand how to build a differential equation for y,,,,
I understand that ## \dot{x}=\frac{dx}{dt}=\frac{dy}{dt}=\dot{y} \\ a=\ddot{x}=\frac{d^2x}{dt^2}=\frac{d^2y}{dt^2}=\ddot{y} ##
Simple: the second derivatives on the left are equal alright. But you need to substitute your expression for y in terms of x. Not just y = x, but: ...:rolleyes:
 

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