| | Physics 151 Lecture 2 - Static Electricity - The Electric Field |
 | | Since we have already seen how one point charge (the charge, say on an elementary particle) can exert a force on a second (see the previous lecture), we should state that the electric field produced by a positive (negative) point charge goes radially outward (inward) in all directions from (toward) the charge. |
 | | If we understand how charge is distributed over an object and if the object and its charge distribution have a high degree of symmetry, then we can easily calculate the electric field due to that object, and hence the force it can produce on other charged objects, by the usual techniques of integral calculus. |
 | | In other words, if h is big, then the point where we want to calculate the field is very far away from the segment and we expect that it will be difficult to tell the difference between the field due to a point charge and the field due to a small line segment. |
| dept.physics.upenn.edu /courses/gladney/phys151/lectures/lecture_jan_15_2003.shtml (1673 words) |