What is the force on an electric dipole due to a line of charge?

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SUMMARY

The discussion focuses on the calculation of the force exerted by a line of charge density \(\lambda\) on an electric dipole, resulting in the formula \(F = \frac{2\lambda p}{4\pi\epsilon_{0}r^{2}}\). The analysis assumes that the distance \(r\) is significantly larger than the charge separation \(s\) in the dipole. Key equations include the relationship between the electric field \(E\) and the forces on the dipole charges, leading to the conclusion that the attractive force is dependent on the dipole moment \(p\) and the charge density \(\lambda\).

PREREQUISITES
  • Understanding of electric dipoles and dipole moments
  • Familiarity with Coulomb's law and electric fields
  • Knowledge of electrostatics, specifically line charge density
  • Basic calculus for manipulating equations involving limits
NEXT STEPS
  • Study the derivation of electric field due to a line charge
  • Learn about the concept of dipole moments in electrostatics
  • Explore the implications of the force on dipoles in varying electric fields
  • Investigate the role of \(\epsilon_{0}\) in electrostatic calculations
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Physics students, educators, and professionals in electromagnetism who are looking to deepen their understanding of electric dipoles and their interactions with electric fields generated by line charges.

KillerZ
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Homework Statement



Show that a line of charge density \lambda exerts an attractive force on an electric dipole with magnitude F = \frac{2\lambda p}{4\pi\epsilon_{0}r^{2}}. Assume that r is much larger than the charge separation in the dipole.

23ti1j5.png

Homework Equations



I need to show that the magnitude, F = \frac{2\lambda p}{4\pi\epsilon_{0}r^{2}}

p = qs => assume s is very small at end of calculations

F = Fon -q + Fon +q = 0

Fon -q = -qE
Fon +q = +qE

The Attempt at a Solution



I am not sure if I am doing this correct?

F = Fon -q + Fon +q
F = -qE + +qE

= \frac{pE}{s} + \frac{pE}{s}

= \frac{p}{s}\frac{1}{4\pi\epsilon_{0}}\frac{2\lambda}{r} + \frac{p}{s}\frac{1}{4\pi\epsilon_{0}}\frac{2\lambda}{r}
 
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KillerZ said:

Homework Statement



Show that a line of charge density \lambda exerts an attractive force on an electric dipole with magnitude F = \frac{2\lambda p}{4\pi\epsilon_{0}r^{2}}. Assume that r is much larger than the charge separation in the dipole.

23ti1j5.png

Homework Equations



I need to show that the magnitude, F = \frac{2\lambda p}{4\pi\epsilon_{0}r^{2}}

p = qs => assume s is very small at end of calculations

F = Fon -q + Fon +q = 0

Fon -q = -qE
Fon +q = +qE

The Attempt at a Solution



I am not sure if I am doing this correct?

F = Fon -q + Fon +q
F = -qE + +qE

= \frac{pE}{s} + \frac{pE}{s}

= \frac{p}{s}\frac{1}{4\pi\epsilon_{0}}\frac{2\lambda}{r} + \frac{p}{s}\frac{1}{4\pi\epsilon_{0}}\frac{2\lambda}{r}

There are 2 problems here:

  • A "-" sign got lost from the -qE term, when you went on to the next step.
  • The distance to the +q charge is not r.

Hope that helps. :smile:
 

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