Jan 20 2009 Physics II Get Fuzzy: Jan 20, 2009.

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Jan 20 2009 Physics II Get Fuzzy: Jan 20, 2009

HITT Quiz Two identical conducting spheres A and B carry equal charge. They are separated by a distance much larger than their diameters. A third identical conducting sphere C is uncharged. Sphere C is first touched to A, then to B, and finally removed. As a result, the electrostatic force between A and B, which was originally F, becomes: A. F/2 B. F/4 C. 3F/8 D. F/16 E. 0 c

PHY 2049: Physics II Electric fields due to a point charge (Coulomb’s), a wire and a plane. Charge shells don’t act inside. In an insulator with uniformly distributed charge, only charge enclosed inside contributes to the field outside. Gauss’ theorem

PHY 2049: Physics II The electric field has been calculated along a line passing through the center of the ring. It is zero at the center of the ring, increases up to z ~ R and then decreases. It decreases as 1/R3 for large z. Looks like a spring. Problem 76 Calculus gift, sums replaced by integrals. Does an electron oscillate through the center fo the ring?

Wires, Rings etc.. Inside a uniformly charged ring, E = 0. Inside a uniformly charged spherical shell, E = 0. Electric field lines emerge from a positive charge. They end at a negative charge. Electric field lines do not cross.

Electric field vectors from a positive point charge Electric field vectors from a positive point charge. Field lines are not vector E.

Does not depend on the distance. C/L 2 dimensionally OK

PHY 2049: Physics II E = σ/εo inside

PHY 2049: Physics II Flux and Gauss’ theorem

PHY 2049: Physics II Gaussian (imaginary) surfaces Flux = Φ = ∑ E.dA E.dA for a cube is easy to visualize. Let calculus do it for a sphere or any other shape. Φc = qtotal /εo

S1: Φc = q/ εo S2: Φc = -q/ εo S3: Φc = 0 S4: Φc = 0

For a cylinder with axial field, no contribution to flux from the side walls. From the far top, >0 Near (bottom) , <0

PHY 2049: Physics II No force/field from the charge outside On inside circle E.4πr2=q/εo Coulomb’s law Very outside, E = k 5q/r2 P + + + + + +

PHY 2049: Physics II The electric field in a metal is zero Charge +q on inside surface. Because it is neutral, outside surface must be -q.

PHY 2049: Physics II Electric field is radial. E.A = 0 for the top and bottom surfaces. Sideways: E 2πrh = λh/ε0 E = λ/ 2πrε0

PHY 2049: Physics II Plane 2EA = σA/εo E = σ/2εo

Summary for today Electric Fields of a continuous charge distribution Field lines Electric flux and Gauss’ theorem Dipoles and Torques