Gauss's Law vs Coulomb's law problem

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SUMMARY

The discussion centers on determining the electric field at point P due to a thin sheet shaped as an annular semicircle with a positive surface charge density +σ. The consensus is to utilize Coulomb's Law rather than Gauss's Law, as the latter does not provide sufficient symmetry for effective application in this scenario. The total charge of the sheet is calculated by multiplying the surface charge density σ by its area, which is then used in Coulomb's equation to find the electric field. The symmetry of the problem allows for certain components of the electric field to cancel out, simplifying the calculations.

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  • Understanding of Gauss's Law and its mathematical formulation.
  • Familiarity with Coulomb's Law and its application in electrostatics.
  • Knowledge of electric field concepts and how to calculate it from charge distributions.
  • Basic proficiency in polar coordinates for integration purposes.
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  • Study the application of Coulomb's Law in non-uniform charge distributions.
  • Learn about the implications of symmetry in electrostatic problems.
  • Explore advanced techniques for integrating electric fields in polar coordinates.
  • Review examples of Gauss's Law applications to identify suitable scenarios.
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yeshuamo
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Homework Statement


A thin sheet in the shape of an annular semicircle has a positive surface charge density +σ as shown. What is the electric field at point P?

Here is an illustration of the problem:
http://postimg.org/image/630bpqwan/

Homework Equations


Gauss's Law:
φ=Qenclosed/ε0
φ=∫E⋅dA
Qenclosed=ε0*∫E⋅dA

Coulomb's Law:
E=(1/(4πε0))(Σq/(r2))

The Attempt at a Solution


If I draw a gaussian surface somewhere between the point P and the radius a, the charge enclosed would be zero. Can I assume that this would mean that the electric flux through that surface is zero, and, by extension, the electric field experienced at point P is zero, too?

If I'm wrong about the Gauss's law approach, should I instead use a Coulomb's law approach and integrate the electric field generated by the semicircular sheet, minus the electric field generated by the semicircular cavity?

Thank you.
 
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yeshuamo said:

Homework Statement


A thin sheet in the shape of an annular semicircle has a positive surface charge density +σ as shown. What is the electric field at point P?

Here is an illustration of the problem:
http://postimg.org/image/630bpqwan/

Homework Equations


Gauss's Law:
φ=Qenclosed/ε0
φ=∫E⋅dA
Qenclosed=ε0*∫E⋅dA

Coulomb's Law:
E=(1/(4πε0))(Σq/(r2))

The Attempt at a Solution


If I draw a gaussian surface somewhere between the point P and the radius a, the charge enclosed would be zero. Can I assume that this would mean that the electric flux through that surface is zero, and, by extension, the electric field experienced at point P is zero, too?

If I'm wrong about the Gauss's law approach, should I instead use a Coulomb's law approach and integrate the electric field generated by the semicircular sheet, minus the electric field generated by the semicircular cavity?

Thank you.
The short answer is to use Coulomb's Law.

The flux can be zero through some surface without the electric field being zero anywhere on that surface.
 
there is no symmetry that permits efficient use of gauss's law in this problem. the symmetry is much better suited for coulomb's law. you will have some components that cancel out due to the symmetry.
 
SammyS said:
The short answer is to use Coulomb's Law.

The flux can be zero through some surface without the electric field being zero anywhere on that surface.

cpsinkule said:
there is no symmetry that permits efficient use of gauss's law in this problem. the symmetry is much better suited for coulomb's law. you will have some components that cancel out due to the symmetry.

The symmetry factor makes this sensible. Thank you! I found the total charge of the thin sheet from the product of σ by its area, and used that total charge in the Coulomb's equation for electric field. And in polar coordinates, you were right, things canceled.

Thank you.
 

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