Differential Equations in simple mechanics?

Click For Summary

Discussion Overview

The discussion revolves around the application of differential equations in solving mechanics problems, particularly in the context of tension in ropes. Participants explore how to use differential equations to derive information about forces in mechanical systems, with a focus on high school-level understanding.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant mentions encountering problems in a physics book that require finding tension in a rope using differential equations, seeking a technical explanation for application.
  • Another participant questions the specific scenario being discussed, noting that differential equations are not commonly encountered by high school students.
  • A participant expresses familiarity with differential equations but lacks knowledge on applying them to mechanical problems.
  • A technical example is provided, illustrating Newton's second law as a differential equation and discussing the relationship between force, mass, and acceleration.
  • Participants discuss the concept of tension in a rope, noting that tension is uniform in equilibrium and can be derived using trigonometry in certain configurations.
  • There is a suggestion that the tension in a partially slack rope is a more complex problem that may involve differential equations.
  • One participant emphasizes the need to define force in a mathematical context to solve differential equations, questioning the origin of force in physical terms.
  • Another participant illustrates a general example of a differential equation to clarify the concept of finding unknown functions based on their derivatives.
  • There is a distinction made between definitions and equations, highlighting the importance of understanding the context in which force is defined.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and application of differential equations in mechanics. While some agree on the basic principles, there is no consensus on specific applications or the complexity of certain problems, particularly regarding partially slack ropes.

Contextual Notes

Participants acknowledge the limitations of their discussions, particularly in defining force and its application in differential equations. The conversation reflects a range of experiences with differential equations, from basic understanding to more complex applications.

Timothy S
Messages
49
Reaction score
0
I came across a few problems in the Kleppner and Kolenkow book in which you must find the force of tension at specific lengths on a rope of mass m. They said you must use differential equations to solve these types of problems. How can you solve and use differential equations like this to get knew information? I would appreciate a technical explanation as i am only in high school.
 
Physics news on Phys.org
Is there a specific situation you have in mind? Not many high schoolers have experience with differential equations. Do you know what they are?
 
I know what differential equations are but i do not know to apply them mechanical problems.
 
Ok. I'm still not sure what type of problem you have in mind so I will give you a simple example of how differential equations are used straight from Newton's second law:
Suppose that a particle at rest is subject to a constant net force ##F##. Newton's second law tells us that (as you've probably seen it written) ##F=ma##. This is actually a differential equation which I'll write as ##F=m dv/dt##. The 'unknown' function in this case is the velocity function. All we have is information about its derivative

##dv/dt=F/m=constant##

So the job is to find the function who's derivative is a constant. In general, that is a linear equation. In this case the function is ##v(t)=F/m *t##.

As for modeling tension in a rope or chain you need to be more specific. Note that if the rope is in equilibrium then the tension is uniform throughout.
 
There's an introduction to Differential Equations at high-school level here:

http://www.examsolutions.net/maths-revision/syllabuses/Index/period-1/Further-Pure/module.php

Towards the bottom of the list of topics.
 
Last edited by a moderator:
Is F = m*a the F definition?
Then what you would substitute instead F in
dv/dt = F/m ?
 
mac_alleb said:
Then what you would substitute instead F in
dv/dt = F/m ?
The sum of the forces along a particular direction. In my post I called 'F' a constant force for simplicity.
 
The tension of a dangling rope (a rope in equilibrium) is simply the weight of whatever it is supporting.

Specifically, the force of tension on that rope goes in the direction of the rope. So if you have multiple ropes attached to a single object, you can derive using trigonometry.

I am guessing that instead of giving you initial values, it just gives you a differential equation describing the system.

If, in fact, you mean finding the tension on parts of a partially slack rope using differential equations... well, that's hard.
 
Simplicity is Ok, but what about the origin of F? Another formulae (which?), experiment or?
 
  • #10
F is just the name I gave to a constant force, the origin is unimportant. Think of it as the pull of a string or something.
 
  • Like
Likes   Reactions: ellipsis
  • #11
brainpushups said:
F is just the name I gave to a constant force, the origin is unimportant. Think of it as the pull of a string or something.
That's actually the best analogy I've heard for vector forces.
 
  • #12
Somehow somewhere isn't a case of differential equation. In order to solve it us must define F pure math. It could not be done from F = m*a, then? If you define F as constant, where to find the value of it?
 
  • #13
I think we are talking past each other here. Let me illustrate the example in a totally arbitrary way using different notation. Suppose I know that a differential equation is

##dx/dt=v##

where v is a constant; it does not need any physical meaning for the sake of this example, but it COULD stand for something physical... perhaps a constant velocity.

The goal of solving this equation is to find an unknown function x(t) knowing that its derivative is a constant value. This function is, of course

##x(t)=v*t+x0##

where x0 is the integration constant.

This problem is exactly the one that I explained above except the derivative physically represented acceleration (the derivative of velocity) and was equal to a constant net force.
 
  • #14
I could easily agree with you latest example. Us just wanted to underscore the difference between "definition" and "equation".
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 25 ·
Replies
25
Views
4K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 2 ·
Replies
2
Views
1K