gracy said:
Ok.
As per my understanding
##Wnet##=##ΔKE##
(According to work energy theorem)
##Wconservative##= ##-ΔP.E##
##Wnon conservative##=##ΔP.E##+##ΔK.E##
Am I correct?
I don't know. Personally, I wouldn't look at it this way. I would let the math resolve the issue for me. Here's a one dimensional example. Suppose I have a charged particle of mass m and charge q in an electric field E (directed along the positive x axis), and I exert a force F along the x-axis to move the charge from x
1 to x
2. If a write a force balance on the system, I get:
$$m\frac{dv}{dt}=F+qE$$
Since an electric field is conservative, it can be represented as minus the derivative of the potential U. So, I have:
$$m\frac{dv}{dt}=F-q\frac{dU}{dx}$$
If I substitute dt=dx/v into this equation, I get
$$mv\frac{dv}{dx}=F-q\frac{dU}{dx}$$
Integrating this equation from x
1 to x
2 yields
$$\left(m\frac{v^2}{2}\right)_{x_2}-\left(m\frac{v^2}{2}\right)_{x_1}=\int_{x_1}^{x_2}Fdx-q(U(x_2)-U(x_1))$$
The terms on the left hand side of this equation is the change in kinetic energy. The first term on the right hand side is the external work done on the charge. The second term on the right hand side is minus the change in potential energy. So
$$Δ(KE)=W-Δ(PE)$$or
$$W=Δ(PE)+Δ(KE)$$
If the work is done in such a way that the change in kinetic energy is zero, then the work is equal to the change in potential energy.
Chet