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The Electric Field of a Dipole © Frits F.M. de Mul
The Electric Field of a Dipole Given: Electric Dipole,  situated in O,  with dipole moment  p  [Cm]  Question: Calculate  E- field in arbitrary points  P around the dipole P O p
The Electric Field of a Dipole ,[object Object],[object Object],[object Object],[object Object],[object Object]
Analysis and Symmetry All points at  equal  r  and   are equivalent, even if at  different   P O p Coordinate axes:  X,Y, Z Y-axis = dipolar axis X Z Y Symmetry:  cylindrical around Y-axis Cylindrical coordinates:  r,     and   perpendicular’ r  e r e  e r  e 
Approach to solution Several approaches possible: 1.  E  with “Coulomb”;  2.  E  from  V  with:  E  = - grad  V Choose option 2. Necessary: calculate  V(r,  )  first ! r  P O e r p e  e r X Y Z  e 
Intermezzo:  V(r,  )  -calculation Calculate :  Potential in  P  : (reference in inf.) If  a << r +  ,r -   ,  then Contributions to  V  from  +Q  and – Q  : P -Q + Q p=Qa a r + r -     P -Q + Q r - r +   r a a  cos  
Intermezzo:  V(r,  )  -calculation This approximation is called: Far-field approximation P -Q + Q r - r +   e r r a a  cos  
Calculation of  E  (1) Calculate  E  from  V  using : E =  -  grad  V In general : X Y Z U V W with  s u  ,s v   and  s w   line elements
Calculation of  E  (2) here  u=r, v=    ,w=  r  P O p e  e r X Y Z  e 
Calculation of  E  (3) here  u=r, v=    ,w=  r  P O p e  e r X Y Z  e 
Calculation of  E  (4) r  O p e  e r X Y Z  e  here  u=r, v=    ,w= 
Calculation of  E  (5) r  O e r p e  e r X Y Z e   E r E  E
Conclusions (1) r  O e r p e  e r X Y Z  e  E r E  E E r
Conclusions (2) E - directions   in the 4 quadrants:  r e r e  e r e  e r e  e r e  I II III IV I  II  III  IV cos  +  -  -  +  sin  +  +  -  - E r   and   E    -comp. E
Field lines in XY-plane (1) Field lines in  XY-plane : r  O p e  e r X Y
Field lines in XY-plane (2) Parameter: distance  a  between  -Q and +Q a  = 20 a  = 10 a  = 1 a  = 0.1 far field
Field lines in XY-plane (3) Parameter: distance  a  between  -Q and +Q a  = 20 a  = 10 a  = 1 a  = 0.1 far field
Field lines in XY-plane (4) Parameter: distance  a  between  -Q and +Q a  = 20 a  = 10 a  = 1 a  = 0.1 far field
Field lines in XY-plane (5) Parameter: distance  a  between  -Q and +Q a  = 20 a  = 10 a  = 1 a  = 0.1 far field
Field lines in XY-plane (6) Parameter: distance  a  between  -Q and +Q a  = 20 a  = 10 a  = 1 a  = 0.1 far field

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E field dipole

  • 1. The Electric Field of a Dipole © Frits F.M. de Mul
  • 2. The Electric Field of a Dipole Given: Electric Dipole, situated in O, with dipole moment p [Cm] Question: Calculate E- field in arbitrary points P around the dipole P O p
  • 3.
  • 4. Analysis and Symmetry All points at equal r and   are equivalent, even if at different  P O p Coordinate axes: X,Y, Z Y-axis = dipolar axis X Z Y Symmetry: cylindrical around Y-axis Cylindrical coordinates: r,  and   perpendicular’ r  e r e  e r  e 
  • 5. Approach to solution Several approaches possible: 1. E with “Coulomb”; 2. E from V with: E = - grad V Choose option 2. Necessary: calculate V(r,  ) first ! r  P O e r p e  e r X Y Z  e 
  • 6. Intermezzo: V(r,  ) -calculation Calculate : Potential in P : (reference in inf.) If a << r + ,r - , then Contributions to V from +Q and – Q : P -Q + Q p=Qa a r + r -     P -Q + Q r - r +   r a a cos 
  • 7. Intermezzo: V(r,  ) -calculation This approximation is called: Far-field approximation P -Q + Q r - r +   e r r a a cos 
  • 8. Calculation of E (1) Calculate E from V using : E = - grad V In general : X Y Z U V W with s u ,s v and s w line elements
  • 9. Calculation of E (2) here u=r, v=  ,w=  r  P O p e  e r X Y Z  e 
  • 10. Calculation of E (3) here u=r, v=  ,w=  r  P O p e  e r X Y Z  e 
  • 11. Calculation of E (4) r  O p e  e r X Y Z  e  here u=r, v=  ,w= 
  • 12. Calculation of E (5) r  O e r p e  e r X Y Z e   E r E  E
  • 13. Conclusions (1) r  O e r p e  e r X Y Z  e  E r E  E E r
  • 14. Conclusions (2) E - directions in the 4 quadrants:  r e r e  e r e  e r e  e r e  I II III IV I II III IV cos + - - + sin + + - - E r and E  -comp. E
  • 15. Field lines in XY-plane (1) Field lines in XY-plane : r  O p e  e r X Y
  • 16. Field lines in XY-plane (2) Parameter: distance a between -Q and +Q a = 20 a = 10 a = 1 a = 0.1 far field
  • 17. Field lines in XY-plane (3) Parameter: distance a between -Q and +Q a = 20 a = 10 a = 1 a = 0.1 far field
  • 18. Field lines in XY-plane (4) Parameter: distance a between -Q and +Q a = 20 a = 10 a = 1 a = 0.1 far field
  • 19. Field lines in XY-plane (5) Parameter: distance a between -Q and +Q a = 20 a = 10 a = 1 a = 0.1 far field
  • 20. Field lines in XY-plane (6) Parameter: distance a between -Q and +Q a = 20 a = 10 a = 1 a = 0.1 far field