2. Electrical dipoles on a thin long line Question: Calculate E- field in arbitrary points around the line Available: Thin line, infinitely long, homogeneously filled with dipoles, each with dipole moment p [Cm]
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4. Analysis and Symmetry (1) all points at equal r are equivalent, even if at different z or 1. Cylinder : infinitely long and thin 2. Distribution of dipoles: n dipoles / meter; homogeneous; all directions uniform each: dipole moment p [Cm] 3. Coordinate axes: X,Y,Z Z-axis = symm. axis Y X Z e z 4. Cylinder symmetry: e r
5. Analysis and Symmetry (2) Assume: field components of dipole field at some distance in point P àre known. p Dipole : r P e r e E r E
6. Analysis and Symmetry (3) Possible directions of the dipoles: X Z e z e r Y X Y X Z e z e r Y Y X Z e z e r Z
7. Approach to solution Use symmetry: dp = n p dz n = dipole density (per meter) Z Y P y P Choose : Point P at distance y P from axis. r + r - Dipole elements at + z and - z will contribute symmetrically dp in dz at + z dp in dz at - z +z -z O
8. Calculations (1): Dipoles // X-axis P dp in dz at + z dp in dz at - z Z +z -z y P r + r - O Y X Case 1: all dipoles // +X-axis dE d ==> E // -X-axis E result = 90 0 ==> e + =e
9. Calculations (2a): Dipoles // Y-axis resulting vector : ==> E // Y-axis Find directions of the field contributions dE dp in dz at - z P dp in dz at + z Z +z -z O Y X Case 2: all dipoles // +Y-axis e + e r+ e - e r- dE r cos dE sin dipole + z - z >0 d r >0 d r dE >0 d >0 E result
10. Calculations (2b): Dipoles // Y-axis Y-components: P Z +z -z O Y X dE d e - e + e r- e r+ d r d r E result r dp = n.p.dz ; dE r+ and dE r- : each: dE + and dE - : each:
11. Calculations (3a): Dipoles // Z-axis resulting vector : ==> E // Z-axis P dp in dz at + z dp in dz at - z Z +z -z O Y X Case 3: all dipoles // +Z-axis e + e r+ e - e r- dE r cos dE sin dipool + - <0 d r >0 d r dE >0 d >0 dE result
12. Calculations (3b) Z-components: P Z +z -z O Y X dE d e - e + e r- e r+ d r d r dE result r r dp = n p dz dE r+ and dE r- : each: dE + and dE - : each:
13. Conclusions dipole direction: dE - contributions: and r are measured from dipole to P ) the end X Z e z e r Y X Y Z