Electric Fields.

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Presentation transcript:

Electric Fields

Two charges q = + 1 μC and Q = +10 μC are placed near each other as shown in the figure. Which of the following diagrams best describes the forces acting on the charges: +10 μC +1 μC a) b) c) This is an example of Newton’s third law:

The Electric Field r F º E q The net Coulomb force on a given charge is always proportional to the strength of that charge. Vector sum! F2 F1 F = + q1 F1 F The direction of the field is the direction of the force on a positive test charge. q F2 q2 positive test charge We can now define a quantity, the electric field, which is independent of the test charge, q, and depends only on position in space: q F E r º Electric Field Applet

The Electric Field Electric field is the force per unit positive charge at a point in space. The SI units of electric field are: N/C The magnitude of the electric field due to a point charge Q

Ways to Visualize the E Field Consider the E-field of a positive point charge at the origin + chg vector map + + + chg field lines

Rules for Vector Maps Direction of arrow indicates direction of field + chg + Direction of arrow indicates direction of field Length of arrows  local magnitude of E

Rules for Field Lines + - Lines leave (+) charges and return to (-) charges Number of lines leaving/entering charge  amount of charge Tangent of line = direction of E Local density of field lines  local magnitude of E Field at two white dots differs by a factor of 4 since r differs by a factor of 2 Local density of field lines also differs by a factor of 4 (in 3D)

Field Lines From Two Like Charges There is a zero halfway between the two charges r >> a: looks like the field of point charge (+2q) at origin

Field Lines from 2 Opposite Charges Grass seed suspended in oil lines up along the electric field.