Deriving the Work-Energy Theorem: A Calculus Refresher

In summary, the chain rule states that if v is a function of x and x is a function of t, then the derivative of v with respect to t is equal to the derivative of v with respect to x times the derivative of x with respect to t. This can be helpful when trying to find the derivative of a function that is composed of multiple functions.
  • #1
nothing123
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0
It's been a while since I've taken calculus. I was going through the derivation of the work-energy theorem and came across this: dv/dt = (dv/dx)(dx/dt) which is supposed to be a result of the chain rule. Anyone care to explain and please simplify it as much as possible.

Thanks!
 
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  • #2
The chain rule is

f(g(x))' = f'(g(x))g'(x)

Now replace f with v, g with x, x with t,the first ' with d/dt, the second ' with d/dx (since f is a function of g aka x), and the third ' with d/dt and voila you have
dv/dt = (dv/dx)(dx/dt)
 
  • #3
Hi nothing123! :smile:

If v is a function of x only, and x is a function of t only, then if you increase t by a small amount ∆t, then x increases by a small amount ∆x = (dx/dt)∆t. (1)

But v also increases, by a small amount ∆v = (dv/dx)∆x. (2)

So, combining (1) and (2):
∆v = (dv/dx)∆x = (dv/dx)(dx/dt)∆t. :smile:
 
  • #4
Great, thanks for your help guys.
 

1. What is the Work-Energy Theorem and why is it important?

The Work-Energy Theorem states that the work done on an object is equal to the change in its kinetic energy. This means that the energy of a system can be conserved and transferred between different forms, allowing us to analyze and understand the behavior of objects in motion. It is an important concept in physics and engineering, as it helps us calculate the work required to move an object, the speed of an object after a certain amount of work is done, and the efficiency of various machines.

2. How is the Work-Energy Theorem derived using calculus?

The Work-Energy Theorem can be derived using the fundamental principles of calculus, specifically the concept of integration. By breaking down the work done on an object into smaller and smaller increments, we can use the integral of force over displacement to find the total work. Then, by applying the definition of work and the equations for kinetic energy, we can show that the work done on an object is equal to the change in its kinetic energy.

3. What are the assumptions and limitations of the Work-Energy Theorem?

The Work-Energy Theorem assumes that there are no external forces acting on the system, and that all work done is due to conservative forces. This means that friction, air resistance, and other non-conservative forces are not taken into account. Additionally, the theorem only applies to rigid bodies with constant mass and does not account for changes in potential energy or other forms of energy.

4. Can the Work-Energy Theorem be applied to non-conservative systems?

While the Work-Energy Theorem is typically used for conservative systems, it can also be applied to non-conservative systems by taking into account the work done by non-conservative forces. This can be done by adding an additional term to the equation for work, known as the work-energy principle, which accounts for the work done by non-conservative forces.

5. How is the Work-Energy Theorem used in real-world applications?

The Work-Energy Theorem has many practical applications in various fields, such as engineering, physics, and sports. It is used to analyze the efficiency of machines, such as engines and turbines, as well as to calculate the speed and trajectory of moving objects, such as projectiles. In sports, the theorem is used to understand the energy and work involved in different types of movements, such as running, throwing, and kicking. It is also used in designing roller coasters and other amusement park rides.

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