Calculating Total Dipole Moment of Spherical Sheet

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The discussion centers on calculating the total dipole moment of a spherical sheet with a surface-charge density that varies with the polar angle. The initial calculation provided the z-component of the dipole moment, but confusion arose regarding the term "total" dipole moment, which refers to the complete vector form rather than just one component. The solution involves integrating over the full range of polar angles to account for the entire charge distribution. Clarification was provided that the x- and y-components of the dipole moment are zero due to symmetry. Understanding the full vector nature of the dipole moment is essential for solving the problem correctly.
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Homework Statement



A spherical sheet of radius a has surface-charge density which depends on the polar angle θ according to the formula

σ(θ)=σ0+σ1cos(θ)

Find the total dipole moment

Homework Equations


pz=∫(dQ)z
z=rcosθ


The Attempt at a Solution



I calculated the 1st dipole moment
pz=∫∫d∅dθσ0a^3sinθcos^2θ
pz=4/3pi*a^3σ0

I'm not understanding the question, "total" dipole moment?
 
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hansbahia said:
I'm not understanding the question, "total" dipole moment?

When you don't understand a term, the most logical thing to do is to look it up (first try looking in your textbook & notes, and if it isn't there, then try Google, and finally just ask your instructor for clarification).

Total dipole moment just means the electric dipole moment of the entire distribution (the full vector form, not just the z-component that you get from the 2 relevant equations you posted).
 
Thanks, I figured out. I had to integrate from 0 to pi
 
hansbahia said:
Thanks, I figured out. I had to integrate from 0 to pi

But do you see why the x- and y-components of the dipole moment are zero here? Getting the right answer is not the same as solving the problem.
 

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