What Is the Dipole Moment of a Grounded Sphere in a Uniform Electric Field?

In summary: Your Name] In summary, the electric potential of a grounded conducting sphere in a uniform electric field can be described by the equation V(r, θ) = -E0rcosθ + (E0R^3cosθ)/r^2, where r is the distance from the center of the sphere and θ is the angle the radius vector makes with the z axis. To calculate the dipole moment of the sphere, we use the surface charge density equation σ(θ) = -ε(dV/dr)|r=R, which leads to a correct dipole moment of P=6πεE0R^3.
  • #1
humanist rho
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Homework Statement


The electric potential of a grounded conducting sphere of radius r in a
uniform electric field [tex]E_{0}\hat{k}[/tex]along the z direction is given by

[tex]V(r,\theta )=-E_{0}r\cos \theta +\frac{E_{0}R^{3}\cos \theta }{r^{2}}[/tex]

where r is the distance from the centre of the sphere and θ is the
angle the radius vector makes with the z axis.

(a)what is the dipole moment acqured by the sphere?


Homework Equations





The Attempt at a Solution




Surface charge density,

[tex]\sigma (\theta )=-\varepsilon \frac{\partial V}{\partial r}%
|_{r=R}=3\varepsilon E_{0}\cos \theta [/tex]
Dipole moment,

[tex]P=\int \sigma (\theta ^{\prime })r^{\prime }ds^{\prime }

=\int_{0}^{\pi }3\varepsilon E_{0}\cos \theta ^{\prime }r^{\prime
}r^{\prime 2}\sin \theta ^{\prime }d\theta ^{\prime }d\phi ^{\prime }

=6\pi \varepsilon E_{0}R^{3}\int_{0}^{\pi }\cos \theta ^{\prime
}\sin \theta ^{\prime }d\theta ^{\prime }

=6\pi \varepsilon E_{0}R^{3}\int_{-1}^{1}\cos \theta ^{\prime
}d(\cos \theta )

=6\pi \varepsilon E_{0}R^{3}[/tex]

But this don't match with the real answer. :(
 
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  • #2

Thank you for your question. Your attempt at solving for the dipole moment of the sphere is on the right track, but there are a few errors in your calculations. Let me walk you through the correct solution.

First, let's start with the correct surface charge density:

\sigma (\theta )=-\varepsilon \frac{\partial V}{\partial r}%
|_{r=R}=-3\varepsilon E_{0}\cos \theta

Note that the negative sign should be included in the expression for the surface charge density. Now, let's move on to calculating the dipole moment:

P=\int \sigma (\theta ^{\prime })r^{\prime }ds^{\prime }

=\int_{0}^{\pi }(-3\varepsilon E_{0}\cos \theta ^{\prime })R^{2}\sin \theta ^{\prime }d\theta ^{\prime }d\phi ^{\prime }

=6\pi \varepsilon E_{0}R^{3}\int_{0}^{\pi }\cos \theta ^{\prime }\sin \theta ^{\prime }d\theta ^{\prime }

=6\pi \varepsilon E_{0}R^{3}\int_{-1}^{1}\cos \theta ^{\prime }d(\cos \theta )

=6\pi \varepsilon E_{0}R^{3}

As you can see, the only mistake you made was in the calculation of the surface charge density. I hope this helps clarify things for you. Let me know if you have any further questions.
 

Related to What Is the Dipole Moment of a Grounded Sphere in a Uniform Electric Field?

1. What is a dipole moment of a sphere?

The dipole moment of a sphere is a measure of the separation and magnitude of the positive and negative charges within the sphere. It is typically represented as a vector quantity, pointing from the negative charge to the positive charge.

2. How is the dipole moment of a sphere calculated?

The dipole moment of a sphere can be calculated by multiplying the magnitude of the charge by the distance between the positive and negative charges. This distance is typically measured from the center of the sphere to the center of the charges.

3. What is the significance of the dipole moment of a sphere?

The dipole moment of a sphere is important in understanding the electric field and potential around the sphere. It also plays a role in determining the behavior of the sphere in an external electric field.

4. Can a sphere have a zero dipole moment?

Yes, a sphere can have a zero dipole moment if the positive and negative charges are evenly distributed and cancel each other out. This is often the case for a neutral sphere or a symmetrical distribution of charges.

5. How does the dipole moment of a sphere relate to its shape?

The dipole moment of a sphere is affected by the distribution of charges within the sphere, which is influenced by the shape of the sphere. For example, a non-uniform or elongated sphere may have a different dipole moment than a perfectly symmetrical sphere.

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