Originally posted by Moose352
I don't understand how the derivative can be nonzero but the potential can be zero.
I am looking at it from a (perhaps overly) simplistic view. According to the book's answer, the eletric potential (and therefore the potential energy of a charge) at that point is zero.
yes, that is right
This, however, seems contradictory to the fact that a charge placed in the field will in fact gain a kinetic energy (a force is exerted on it), and therefore must have had potential energy. What am I missing here??
think of potential energy (and also electric potential) like a hill, that the charged particles roll up and down.
if the hill that we are rolling down looks like y=x
2, then when the ball is at the bottom and not moving then it will not feel any force. the derivative of this function is zero at the bottom.
but what if the function is like
[tex]y=\frac{x}{x^2-1}[/tex]
this function is pretty much what the potential looks like between two charges. notice that when x=0, y is also =0, so the potential right between the two charges is 0
on the other hand, the derivative of this function is nonzero at x=0. this corresponds to the fact that the force is nonzero, even though the potential is zero.
or, take a much simpler example: if the electric field is constant, like inside a capacitor, then the electric potential rises linearly, it looks like V=ax. this is zero at x=0, but still the force is not zero there.
think of the picture of a hill. the graph of y=ax just keeps falling off, there is lots of room to keep falling. it is the same with the potential between the two charges.
I am still not convinced with the scalar field. I can not believe that the direction of the potential can altogether be disregarded when calculating potential.
scalars don't have direction. i am not sure what you mean here.