Electric Dipole Potential: Direction of Electric Field at Theta=0,45,90,135,180

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SUMMARY

The electric dipole potential is defined by the equation V(r) = p cos(theta) / (4 * π * ε * r²). The electric field E at specific angles (0, 45, 90, 135, and 180 degrees) is derived from the equations Er = 2p cos(theta) / (4 * π * ε * r³) and E(theta) = p sin(theta) / (4 * π * ε * r³). At θ = 45 degrees, the relationship Er = 2 * E(theta) is established due to the equality of sin(45) and cos(45). The resultant angle of the electric field with respect to the dipole axis is determined to be 72 degrees through trigonometric analysis.

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Homework Statement


The potential due to an electric dipole is V(r)=pcos(theta)/(4*PI*epsilon*r^2)
Determine the direction of the electric field E at theta = 0 , 45, 90, 135 and 180 degrees?


Homework Equations


The field of an electric dipole is given by Er = 2pcos(theta)/(4*PI*epsilon*r^3)
and E(theta) = psin(theta)/(4*PI*epsilon*r^3)


The Attempt at a Solution


I am a bit confused when look at the solutions to this question. For theta = 45 degrees is says that

" Er = 2*E(theta) = sqrt(2)*p/(4*PI*epsilon*r^3) or alternatively
Ez=p/(8*PI*epsilon*r^3) and E(x/y) = 3p/(8*PI*epsilon*r^3)
so E = sqrt(5/2)*p/(4*PI*epsilon*r^3)
at an angle to the dipole axis of alpha=72 degrees where tan(alpha)=3 "

I am unsure why Er = 2*E(theta) and how that arrived at the direction of the dipole (especially how they determined it to be at an angle of 72 degrees?? )

Thanks
 
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captainjack2000 said:
I am unsure why Er = 2*E(theta)
Compare the formulas for Er and Eθ for θ = 45 degrees. Realize that sin(45) = cos(45).
and how that arrived at the direction of the dipole (especially how they determined it to be at an angle of 72 degrees?? )
The are asking for the direction of the field with respect to the dipole direction, not the direction of the dipole.

Given that Er = 2Eθ, first figure out (using a little trig) the angle the field makes with the radial direction (where θ = 45). The figure out its angle with respect to the dipole axis (which is where θ = 0).
 

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