Work Done By A Nonconstant Force: Difference between revisions

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When calculating the force, if the magnitude of the force or direction of the force changes, it is not possible to calculate the work done by multiplying force by the displacement. Instead the non constant force is split into a path with small increments.
= Work Done By A Nonconstant Force =
'''Claimed by Matt McCrory – Spring 2025'''


==The Main Idea==
This page explains how to calculate work done when the force applied is not constant. It includes conceptual explanations, worked examples, mathematical and computational models, and embedded simulations to make this concept easier to understand.


State, in your own words, the main idea for this topic


== The Main Idea ==
Before we understand nonconstant force, let's review constant force.


===A Mathematical Model===
For constant force:
: '''Work = Force × Distance'''
: <math>W = F \cdot d</math>


<math> W=\int\limits_{1}^{3}\frac{e^3/x}{x^2}\, dx
[[File:ConstantForce.png|thumb|center|300px|Work as the area under a constant force graph]]


===A Computational Model===
In real-life, however, forces often vary over distance. In that case, we use:
: <math>W = \int_{x_1}^{x_2} F(x) \, dx</math>


How do we visualize or predict using this topic. Consider embedding some vpython code here [https://trinket.io/glowscript/31d0f9ad9e Teach hands-on with GlowScript]
This integral calculates the total work as the area under the curve on a Force vs. Distance graph.


==Examples==
== Mathematical Model ==
Work done by a varying force is found by breaking the motion into tiny intervals:


Be sure to show all steps in your solution and include diagrams whenever possible
: <math>W = \sum \vec{F}_i \cdot \Delta \vec{r}_i</math>


===Simple===
As the interval becomes very small, it becomes a definite integral:
===Middling===
: <math>W = \int \vec{F} \cdot d\vec{r}</math>
===Difficult===


==Connectedness==
=== Spring Example ===
#How is this topic connected to something that you are interested in?
If <math>F = kx</math>, we derive:
#How is it connected to your major?
: <math>W = \int_0^x kx \, dx = \frac{1}{2}kx^2</math>
#Is there an interesting industrial application?


==History==
[[File:WorkIntegral.png|thumb|center|300px|Work done by a spring force]]


Put this idea in historical context. Give the reader the Who, What, When, Where, and Why.
== Computational Model ==
Computational models can approximate work using many tiny time steps. Below is Python code modeling a vertical spring in VPython:


== See also ==
<syntaxhighlight lang="python">
#initialize conditions
L = ball.pos - spring.pos
Lhat = norm(L)
s = mag(L) - L0
Fspring = -(ks * s) * Lhat


Are there related topics or categories in this wiki resource for the curious reader to explore?  How does this topic fit into that context?
#momentum principle
ball.p = ball.p + (Fspring + Fgravity) * deltat
</syntaxhighlight>


===Further reading===


Books, Articles or other print media on this topic
== Interactive Model ==
Try out this Trinket simulation of spring motion: 
[https://trinket.io/glowscript/49f7c0f35f View the simulation on Trinket]


===External links===
== Examples ==
[http://www.scientificamerican.com/article/bring-science-home-reaction-time/]
=== Simple ===
'''Question:''' 
A box is pushed 10 m east by a 40 N force, then 8 m north by a 60 N force.
'''Solution:''' 
: <math>W = 40 \cdot 10 + 60 \cdot 8 = 880 \, J</math>


=== Middling ===
'''Question:''' 
A spring with <math>k = 70 \, N/m</math> is stretched 10 cm. 
[[File:Middle1.JPG|thumb|center|200px|Spring stretching setup]]


==References==
'''Solution:''' 
: <math>W = \frac{1}{2} k x^2 = \frac{1}{2}(70)(0.1)^2 = 0.35 \, J</math>


This section contains the the references you used while writing this page
=== Difficult ===
'''Question:''' 
How much work is done by Earth’s gravity on an asteroid falling from distance <math>d</math> to radius <math>R</math>?


[[Category:Which Category did you place this in?]]
'''Solution:''' 
Start with Newton’s law of gravitation:
: <math>F = \frac{GMm}{r^2}</math>


Claimed By Justin V.
Then integrate:
: <math>W = \int_R^d \frac{GMm}{r^2} \, dr = GMm \left( \frac{1}{R} - \frac{1}{d} \right)</math>
 
== Connectedness ==
Understanding work by nonconstant forces is key in many fields:
 
* '''Springs''': Used in trampolines, shock absorbers, and mechanical pens 
* '''Engineering''': Fluid tanks fill unevenly, requiring nonconstant work 
* '''Energy''': Hydroelectric turbines rely on variable water flow 
* '''Space physics''': Rockets and satellites feel variable gravity
 
 
== History ==
Gaspard-Gustave de Coriolis was the first to define "work" as force over distance. Later physicists used calculus to model work by nonconstant forces.
 
== Further Reading & External Links ==
 
=== Book ===
* Chabay & Sherwood – ''Matter and Interactions'' (4th ed.)
 
=== Articles ===
* [https://phys.libretexts.org/Bookshelves/Classical_Mechanics/Classical_Mechanics_(Dourmashkin)/13%3A_Energy_Kinetic_Energy_and_Work/13.05%3A_Work_done_by_Non-Constant_Forces Nonconstant Force]
* [https://trinket.io/glowscript/49f7c0f35f Iterative Spring-Mass Simulation]
 
=== Simulations ===
* [https://trinket.io/glowscript/49f7c0f35f Spring-Mass Trinket Model]

Latest revision as of 22:24, 22 April 2025

Work Done By A Nonconstant Force

Claimed by Matt McCrory – Spring 2025

This page explains how to calculate work done when the force applied is not constant. It includes conceptual explanations, worked examples, mathematical and computational models, and embedded simulations to make this concept easier to understand.


The Main Idea

Before we understand nonconstant force, let's review constant force.

For constant force:

Work = Force × Distance
[math]\displaystyle{ W = F \cdot d }[/math]
Work as the area under a constant force graph

In real-life, however, forces often vary over distance. In that case, we use:

[math]\displaystyle{ W = \int_{x_1}^{x_2} F(x) \, dx }[/math]

This integral calculates the total work as the area under the curve on a Force vs. Distance graph.

Mathematical Model

Work done by a varying force is found by breaking the motion into tiny intervals:

[math]\displaystyle{ W = \sum \vec{F}_i \cdot \Delta \vec{r}_i }[/math]

As the interval becomes very small, it becomes a definite integral:

[math]\displaystyle{ W = \int \vec{F} \cdot d\vec{r} }[/math]

Spring Example

If [math]\displaystyle{ F = kx }[/math], we derive:

[math]\displaystyle{ W = \int_0^x kx \, dx = \frac{1}{2}kx^2 }[/math]
Work done by a spring force

Computational Model

Computational models can approximate work using many tiny time steps. Below is Python code modeling a vertical spring in VPython:

<syntaxhighlight lang="python">

  1. initialize conditions

L = ball.pos - spring.pos Lhat = norm(L) s = mag(L) - L0 Fspring = -(ks * s) * Lhat

  1. momentum principle

ball.p = ball.p + (Fspring + Fgravity) * deltat </syntaxhighlight>


Interactive Model

Try out this Trinket simulation of spring motion: View the simulation on Trinket

Examples

Simple

Question: A box is pushed 10 m east by a 40 N force, then 8 m north by a 60 N force. Solution:

[math]\displaystyle{ W = 40 \cdot 10 + 60 \cdot 8 = 880 \, J }[/math]

Middling

Question: A spring with [math]\displaystyle{ k = 70 \, N/m }[/math] is stretched 10 cm.

Spring stretching setup

Solution:

[math]\displaystyle{ W = \frac{1}{2} k x^2 = \frac{1}{2}(70)(0.1)^2 = 0.35 \, J }[/math]

Difficult

Question: How much work is done by Earth’s gravity on an asteroid falling from distance [math]\displaystyle{ d }[/math] to radius [math]\displaystyle{ R }[/math]?

Solution: Start with Newton’s law of gravitation:

[math]\displaystyle{ F = \frac{GMm}{r^2} }[/math]

Then integrate:

[math]\displaystyle{ W = \int_R^d \frac{GMm}{r^2} \, dr = GMm \left( \frac{1}{R} - \frac{1}{d} \right) }[/math]

Connectedness

Understanding work by nonconstant forces is key in many fields:

  • Springs: Used in trampolines, shock absorbers, and mechanical pens
  • Engineering: Fluid tanks fill unevenly, requiring nonconstant work
  • Energy: Hydroelectric turbines rely on variable water flow
  • Space physics: Rockets and satellites feel variable gravity


History

Gaspard-Gustave de Coriolis was the first to define "work" as force over distance. Later physicists used calculus to model work by nonconstant forces.

Further Reading & External Links

Book

  • Chabay & Sherwood – Matter and Interactions (4th ed.)

Articles

Simulations