Lecture 30 - UMD Department of Physics - UMD Physics › courses › Phys260 › agashe › S08 ›...
Transcript of Lecture 30 - UMD Department of Physics - UMD Physics › courses › Phys260 › agashe › S08 ›...
Lecture 30
• applications of Gauss’s Law: cylindrical symmetry and conductors
• chapter 28 (Current and Conductivity): basic idea of electron current
Outline
Conductors in Electrostatic Equilibrium: at surface• if not, charges (free to move ) would...
• net charge outside
• If tangent to surface, charges move...
! E "= 0
!e = AEsurface for outside face+0 for inside face (Ein = 0)+0 for wall (E ! surface)!e = Qin
!0; Qin = !A "
Esurface =!
"!0
, ! to surface"
E
Ein = 0
Within conductor...
• excess charge on exterior surface
• inside hole ( inside conductor and no charge in hole): screening
• charge inside hole of neutral conductor polarizes...
E = 0 E = 0
Outline of Chapter 28 (Current and Conductivity)• motion of charges thru’ wire (current): due to electric field inside
wire (relation to charging/electrostatics)
• law of conservation of current
• relate current to conductivity
indicators of current
excess charge moves (current)
Electron Current• charge carriers (that move): electrons in metals
• no current : electrons moving rapidly, no net motion
• push on sea of electrons using : drift speed superposed on random thermal
vd
Ne = i!t
Ne = nV = nA!x = nAvd!t
E
Conservation of current• electron current same at A and B: can’t be created/destroyed/stored: lightbulb uses energy (work done to push electrons)
• wire full of electrons, don’t have to move from plate to plate (just shift/rearrange
Discharge of capacitor is instantaneous