Help With Intergration Dipole Homework Statement

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SUMMARY

The discussion focuses on solving a homework problem related to electric potential differences (\Delta V) in the context of a dipole. The participants explore two methods for calculating \Delta V: superposition of potentials from individual charges and integration of the electric field. The equations used include the potential formula V_q = (1/4\pi\epsilon_0)(+or-q/r) and the integral of the electric field, with specific attention to the correct application of integration techniques. The solutions for parts (a) and (b) highlight the importance of understanding both superposition and integration in electrostatics.

PREREQUISITES
  • Understanding of electric potential and electric fields
  • Familiarity with dipole theory in electrostatics
  • Knowledge of integration techniques in calculus
  • Proficiency in using the formula V_q = (1/4\pi\epsilon_0)(+or-q/r)
NEXT STEPS
  • Study the method of superposition in electrostatics
  • Learn about integration techniques for electric fields, specifically in the context of dipoles
  • Explore the implications of electric potential differences in various configurations of charges
  • Review the concept of electric field lines and their relation to potential
USEFUL FOR

Students studying electromagnetism, particularly those tackling problems involving electric dipoles and potential differences. This discussion is beneficial for anyone looking to deepen their understanding of electrostatic principles and integration methods.

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Homework Statement



We know the magnitude of the electric field at a location on the x-axis and at a location on the y axis, if we are far from the dipole.

(a) Find [tex]\Delta[/tex]V= V_p - V_a along a line perpendicular to the axis of a dipole. Do it two ways: from superposition of V due to the two charges and from the integral of the electric field.

(b) Find [tex]\Delta[/tex]V = V_c - V_d along the axis of the dipole. Include the correct signs. Do it two ways: from the superposition of V due to the two charges and from the integral of the electric field.


Homework Equations



V_q = (1/4[tex]\pi[/tex][tex]\epsilon[/tex]_0)(+or-q/r)
k= 1/4[tex]\pi[/tex][tex]\epsilon[/tex]_0

The Attempt at a Solution



(a)
superposition
[tex]\Delta[/tex]V= (1/4[tex]\pi[/tex][tex]\epsilon[/tex]_0)(+q/(d^2+(s^2)/4))^(1/2))-(1/4[tex]\pi[/tex][tex]\epsilon[/tex]_0)(-q/(d^2+(s^2)/4))^(1/2))

[tex]\Delta[/tex]V= 0

BUT
i don't kno how to do integral
i think its

integral from p to a : E times dd

how do i do it?

i thinks its...

int from a to b: kq/r^2

and i use formula:
int of 1 / x^2 + a^2 dx = (1/a)tan^-1 (x/a)

but I am not sure how to use it or show the answer


(b) superposition



[tex]\Delta[/tex]V = V_c - V_d
= (E_c)a - (E_d)b = 2kqsa/(a^3) -2kqsb/(b^3)
= ((sq)/(2[tex]\pi[/tex][tex]\epsilon[/tex]_0))(1/(a^2)-1(b^2))

but again

i don't kno how to do integration

i haven't got a clue for part B
 

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At the location on the y-axis
due to +q charge
E= k*q/r^2
E = -dV/dr
dV = - E*dr . V = - k*q* intg(1/r^2)*dr
Find the integration. Similarly find V due to - q. Then find net V.
Follow the same method to find V along x-axis.
 
wats the R for V_a?

wats the R for V_p?

are they different?

i think the R for V_a is ((s/2)^2 + d^2 ) )^ (1/2)

but for V_p...

is it just s/2?

if that's true i don't think i will get 0 for [tex]\Delta[/tex]V = V_p - V_A
 

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