Electric field at center of charged hemispherical shell

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SUMMARY

The electric field at the center of a charged hemispherical shell is calculated using the formula \(E = \frac{\sigma}{4\epsilon_0}\), where \(\sigma\) is the surface charge density and \(\epsilon_0\) is the permittivity of free space. The integration process involves spherical coordinates, specifically using \(dA = R^2\sin\phi d\phi d\theta\). A common mistake is to incorrectly include a factor of two in the total electric field expression, which should be adjusted to avoid overcounting contributions from the azimuthal angle.

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  • Understanding of electric fields and Gauss's law
  • Familiarity with spherical coordinates and integration techniques
  • Knowledge of surface charge density (\(\sigma\)) and permittivity of free space (\(\epsilon_0\))
  • Basic proficiency in calculus, particularly double integrals
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  • Review the derivation of electric fields from charge distributions
  • Study the application of Gauss's law in various geometries
  • Learn about the properties of electric fields in spherical coordinates
  • Explore common mistakes in electric field calculations and how to avoid them
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Titan97
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Homework Statement


Find Electric field at center of charged hemispherical shell

Homework Equations


In spherical coordinates, $$dA=R^2\sin\phi d\phi d\theta$$

The Attempt at a Solution


Untitled.png

From the image, Enet=2dEy=2dEcosφ
$$dE=\frac{kdq}{R^2}E$$
$$dE=\frac{k\sigma dA}{R^2}$$
$$dE=\frac{k\sigma R^2\sin\phi d\phi d\theta }{R^2}$$
$$dE_{total}=2k\sigma\sin\phi\cos\phi d\phi d\theta$$
$$E=\int_0^{2\pi}\int_0^{\frac{\pi}{2}}2k\sigma\sin\phi\cos\phi d\phi d\theta$$
$$E=\frac{\sigma}{2\epsilon_0}$$
But given answer is $$E=\frac{\sigma}{4\epsilon_0}$$
 
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The integration over the azimuthal angle from 0 to ##2\pi## already takes the factor of two in your expression ##dE_{total}=2k\sigma\sin\phi\cos\phi d\phi d\theta## into account. So you should have removed it from ##dE_{total}##.
 
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Thank you.
 

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