Finding motion where the acceleration depends on position and time

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SUMMARY

The discussion focuses on deriving the motion of a pendulum modeled as a spring, where the acceleration is defined as a function of both position and time: a(t) = -gj - k/m(|r(t)| - L_0) * r(t)/|r(t)|. The user seeks to create a differential equation using initial conditions, specifically initial velocity and position, while avoiding traditional equations of motion due to the variable nature of acceleration. Participants suggest using Hamilton's principle and resolving the motion component-wise, emphasizing the need for a clear understanding of vector components and the application of advanced physics concepts.

PREREQUISITES
  • Understanding of differential equations and their applications in physics.
  • Familiarity with vector calculus, specifically in resolving vector components.
  • Knowledge of simple harmonic motion and variable force problems.
  • Proficiency in using LaTeX for rendering mathematical equations.
NEXT STEPS
  • Study Hamilton's principle and its application in mechanics.
  • Learn how to resolve motion in terms of vector components, particularly in spring systems.
  • Research variable force problems and their solutions in classical mechanics.
  • Practice using LaTeX for writing and formatting complex equations.
USEFUL FOR

Students in advanced physics courses, particularly those studying mechanics, as well as educators and researchers interested in variable acceleration systems and differential equations.

simo22
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I have computed that the acceleration in my problem is
a(t) = -gj - k/m(|r(t)| - L_0) * r(t)/|r(t)|

Where a(t) is the acceleration vector, g is the gravitational acceleration, j is the unit vector in y-direction, k is the spring constant, m is the mass, r(t) is the position vector, |r(t)| is the length of r(t) and L_0 is the equilibrium length of a rope. I am asked in my problem to make a differential equation by using some initial values and the acceleration to compute the motion.

I was told by the teacher not to use the equations of motion because those require a constant acceleration, while the one we have here is dependent on the position. Is there a way for me to compute the motion given an initial velocity and position?
 
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Are you familiar with setting up and solving differential equations?
 
I'm somewhat familiar with it. I was thinking that since we know r(0), v(0) and a(t), I could simply compute
r(t) = r(0) + v(0)*t + ∫∫a(t)dtdt, but I do not know how to integrate a(t) when it depends on r(t)
 
simo22 said:
Summary:: Finding motion by making a differential equation using initial values and an acceleration that depends on position and time.

I have computed that the acceleration in my problem is
a(t) = -gj - k/m(|r(t)| - L_0) * r(t)/|r(t)|

Where a(t) is the acceleration vector, g is the gravitational acceleration, j is the unit vector in y-direction, k is the spring constant, m is the mass, r(t) is the position vector, |r(t)| is the length of r(t) and L_0 is the equilibrium length of a rope. I am asked in my problem to make a differential equation by using some initial values and the acceleration to compute the motion.

I was told by the teacher not to use the equations of motion because those require a constant acceleration, while the one we have here is dependent on the position. Is there a way for me to compute the motion given an initial velocity and position?

What physical scenario does this represent?
 
It is a pendulum where we think of the rope as a spring
 
simo22 said:
It is a pendulum where we think of the rope as a spring

Ah, ##r(t)## is a vector! You must write ##\vec r##. And the thing on the end is ##\hat r##. I guess you mean the bob is attached by a spring. It can't be a rope.

So, how are you going to resolve your vectors? ##\hat x, \hat y## or along the line of the spring and tangential to it?
 
Once more I'd rather suggest to use Hamilton's principle (which is adequate for an I-level thread, I hope).
 
Well, I have also computed the components of the acceleration, a_x and a_y, so I guess I could do it component-wise
 
simo22 said:
Well, I have also computed the components of the acceleration, a_x and a_y, so I guess I could do it component-wise

At this level, you may struggle without using Latex to render your equations:

https://www.physicsforums.com/help/latexhelp/

Another observation: this seems quite an advanced problem, so the comment about "not using equations of motion", by which you mean "not using SUVAT" looks strange. If you are looking at this problem, then the simplicity of SUVAT should be long ago! Have you not studied simple harmonic motion or other variable force problems before this?

In this case, perhaps resolving along the spring and tangential to it seems more natural. I haven't got time to analyse this myself, but my guess is that's a more promising approach.
 
  • #10
2nd derivative of distance with respect to time= acceleration. your title seems to have pointed to the definition of velocity, which is the 1st derivative of distance with respect to time. acceleration is the change of velocity with respect to time
 

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