The work energy theorem states:
$$W = \int_i^f \mathbf{F}net\cdot d\mathbf{l} = \frac{1}{2}mv_f^2 - \frac{1}{2} mv_i^2$$
This theorem is valid:
1. only for conservative forces.
2. only for non-conservative forces.
3. only for forces which are constant in time
4. only for forces which can be expressed as potential energies
5. for all forces.
Note:
* Correct Answer: E
A + and - charge are held a distance R apart and released.
The two particles accelerate toward each other as a result of the Coulomb attraction. As the particles approach each other, the energy contained in the electric field surrounding the two charges...
<img src="./images/two_charges_coming_together.png" align="center" style="width: 600px";/>
1. increases
2. decreases
3. stays the same
Note:
* Correct Answer: B