Summary
Highlights
When charges have unequal magnitudes, the number of electric field lines drawn should be proportional to their magnitudes. For example, if a +2 C charge has 6 lines, a -4 C charge should have 12 lines. The lines still flow from positive to negative, but the relative density reflects the differing magnitudes.
Electric field lines emanate away from positive charges and point towards negative charges. The direction indicates the type of charge, and the density of lines indicates the strength of the electric field. The equation E = kq/r^2 is used to calculate the magnitude of the electric field created by a point charge, where k is Coulomb's constant (9 x 10^9 N m^2/C^2), q is the magnitude of the charge in Coulombs, and r is the distance from the charge to the point of interest.
The density of electric field lines indicates the strength of the electric field; more dense lines imply a stronger field. For example, if two regions have three and six lines respectively, the region with six lines has twice the electric field strength. A crucial rule is that electric field lines never cross each other.
Given a reference charge (e.g., charge B = +4 C with 8 lines), the magnitude of other charges can be determined by comparing the number of field lines. For example, charge A with 4 lines (half of B's lines) would be +2 C, and charge C with 16 lines would be +8 C. The direction of the lines (outward or inward) indicates whether the charge is positive or negative. For instance, charge D with 4 inward lines would be -2 C.
When drawing electric field lines for two positive point charges, the lines will bend away from each other because positive charges repel. In the region directly between them, the electric field effectively cancels out, creating a null point. Understanding vector addition of electric fields at any point helps explain the curvature of the lines.
For a positive and a negative point charge, electric field lines emanate from the positive charge and terminate on the negative charge. The lines flow directly from positive to negative, creating curved paths around the charges. It's important to ensure lines flow correctly and don't incorrectly bend away if no other positive charge is present.
For parallel plates, one positively charged and one negatively charged, the electric field lines are mostly uniform and parallel in the interior of the plates, pointing from positive to negative. At the edges, the lines bulge outward slightly.
When a positive point charge is near a negatively charged plate, field lines emanate from the point charge and terminate perpendicularly on the plate. Lines close to the plate become relatively horizontal as they approach, demonstrating the attraction between the point charge and the opposite charge on the plate.