2. Darryl Michael/GE CRD Fields and Waves Lesson 3.4 ELECTROSTATICS - MATERIALS

3. CONDUCTORS and DIELECTRICS ConductorsDielectrics High conductivities;  (for Copper) ~ 5.8x10 7 S/m Low conductivities;  (for Rubber) ~ 1x10 -15 S/m or 1/  -m Semiconductors (mid  ’s) Permittivities,  = 1-100   Note:  0 is the permittivity of free space/vacuum = 8.854 x 10 -12 F/m

4. CONDUCTORS Lattice of Nuclei Most electrons are stuck to the nucleus But, 1 or 2 electrons per atom are free to move This means that if you apply an external E- field, the free electrons will move

5. CONDUCTORS - - - - - - - - - - + + + + + + + + + + Apply external E-field, electrons conductor Force on electrons causes free electrons to move Charge displacement causes response E-field (opposite to applied external E-field)

6. CONDUCTORS The electrons keep moving until, This means that:, in a conductor Conductor is equipotential Do problem 1

7. DIELECTRICS + + electron cloud nucleus electron cloud centered on nucleus Cloud shifts to setup

8. DIELECTRICS Define: dipole moment Polarizationpartially cancels applied Field

9. DIELECTRICS Define: Displacement Flux Density ( C/m 2 ) Electric Field (V/m) subtracts out bound charge is due to bound/dielectric charge and free charge is due to bound/dielectric charge only and opposite sign is due to free charge only

10. FREE CHARGES Examples of free charges:  s on conductor electron beam doped region of semi-conductor Gauss’ Law uses just free charge Most general form

11. DIELECTRICS Don’t need to know about bound charges to findMany materials have Define, where Typically, Do Problem 2

12. DIELECTRIC BREAKDOWN - part d of problem Example: Arc in Air If E-field is too large, it will pull electrons off from atom These electrons are accelerated by the E-field These accelerated electrons then collide with more atoms that knock off more electrons This is an AVALANCHE PROCESS BREAKDOWN OCCURS if Damages materials - there is a Voltage limit on components, cables in air : = 30 kV/cm

13. BOUNDARY CONDITIONS - Normal Components all derived from Maxwell’s equations NORMAL COMPONENT h a Gaussian Surface Material 1 Material 2 Take h << a (a thin disc) TOP BOTTOM

14. Case 1: REGION 2 is a CONDUCTOR, D 2 = E 2 =0 Case 2: REGIONS 1 & 2 are DIELECTRICS with  s = 0 Can only really get  s with conductors BOUNDARY CONDITIONS - Normal Components

15. BOUNDARY CONDITIONS - Tangential Components Material 1 Material 2 w h h << w If region 2 is a conductor E 1t = 0 Note: Outside conductor E and D are normal to the surface