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Gauss’ Law for Cylinder Symmetry © Frits F.M. de Mul
Gauss’ Law for Cylinder Symmetry Question: Calculate  E- field in arbitrary points inside and outside cilinder Two cases: A: homogeneously  charged B: charged at surface walls only Available: Cilinder, radius  R,  infinitely long, carrying charge density  [C/m]
Gauss’ Law for Cylinder Symmetry ,[object Object],[object Object],[object Object],[object Object]
Analysis and Symmetry (1) 2.   Charge distribution:   C/m] ; homogeneous. 4.  Cylinder symmetry: 1.  Cylinder : infinitely long,  radius  R 3.  Coordinate axes: Z-axis = symm. axis Y X Z e z e r all points at  equal  r   are equivalent, even if  at  different  z  or   
Analysis and Symmetry (2) 5.  Consequences :  a point charge will not  move tangentially.  Y X Z 4.  Cylinder symmetry: e z e r all points at  equal  r   are equivalent, even if  at  different  z  or    E  directed radially everywhere. all planes  z = const.  are equivalent.
Approach to solution Choose Gauss-box  A. How to make optimum use of symmetry ?? ,[object Object], closed box needed !! Z Gauss’ Law: ,[object Object],dA ,[object Object],dA ==> pill box top lid bottom wall
Calculations (1) top and bottom lids do not  contribute ( E   dA ) wall contributes:  E. 2  rL charge enclosed:   L result:  E ( r ) =   2   r  Gauss’ Law: Z E L pill box: radius  r>R  ; height  L
Calculations (2) result:  E ( r ) =   2   r  but wait !! this holds for  r>R  ! A: homogeneously charged B: charged at surface only Gauss’ Law: Z L L for  r<R  :
Conclusions (1) field strength dependent of distance to cylinder => no homogeneous field A: homogeneously charged B: charged at surface only for infinite cylinder:
Conclusions (2) for infinite cylinder: A: homogeneously charged; B: surface charge only the end R 2 R r 0 E ( r ) A+B A B

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Gauss law for cylinders

  • 1. Gauss’ Law for Cylinder Symmetry © Frits F.M. de Mul
  • 2. Gauss’ Law for Cylinder Symmetry Question: Calculate E- field in arbitrary points inside and outside cilinder Two cases: A: homogeneously charged B: charged at surface walls only Available: Cilinder, radius R, infinitely long, carrying charge density  [C/m]
  • 3.
  • 4. Analysis and Symmetry (1) 2. Charge distribution:   C/m] ; homogeneous. 4. Cylinder symmetry: 1. Cylinder : infinitely long, radius R 3. Coordinate axes: Z-axis = symm. axis Y X Z e z e r all points at equal r are equivalent, even if at different z or  
  • 5. Analysis and Symmetry (2) 5. Consequences : a point charge will not move tangentially. Y X Z 4. Cylinder symmetry: e z e r all points at equal r are equivalent, even if at different z or   E directed radially everywhere. all planes z = const. are equivalent.
  • 6.
  • 7. Calculations (1) top and bottom lids do not contribute ( E  dA ) wall contributes: E. 2  rL charge enclosed:  L result: E ( r ) =  2   r  Gauss’ Law: Z E L pill box: radius r>R ; height L
  • 8. Calculations (2) result: E ( r ) =  2   r  but wait !! this holds for r>R ! A: homogeneously charged B: charged at surface only Gauss’ Law: Z L L for r<R :
  • 9. Conclusions (1) field strength dependent of distance to cylinder => no homogeneous field A: homogeneously charged B: charged at surface only for infinite cylinder:
  • 10. Conclusions (2) for infinite cylinder: A: homogeneously charged; B: surface charge only the end R 2 R r 0 E ( r ) A+B A B