Find the electric field from polarization

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SUMMARY

The discussion focuses on calculating the electric field from polarization using Gauss's law. The user derived the polarization charge density equations, specifically noting that for regions where 0 PREREQUISITES

  • Understanding of Gauss's Law in electromagnetism
  • Familiarity with polarization in dielectric materials
  • Knowledge of vector calculus
  • Basic principles of electrostatics
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  • Review the application of Gauss's Law for polarized materials
  • Study the concept of polarization charge density in dielectrics
  • Learn about the relationship between electric field and polarization vector
  • Examine examples of electric field calculations in spherical coordinates
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Students and professionals in physics, particularly those studying electromagnetism and electrostatics, as well as engineers working with dielectric materials and electric field calculations.

goohu
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Homework Statement
See picture.
Relevant Equations
Gauss law for polarizaton : ## -Q = \int P dA ## , dA = element of area
Untitled.png

Attempt at solution:
a) Since I need help with b) this section can be skipped. Results :
##ρ_{psa} = -Pa ##
##ρ_{psb} = Pb ##
##ρ_{p} = \frac {-1}{R^2} \frac {∂(R^2PR)}{∂R} = -3P ##

b) This is where I am unsure (first time using gauss law for P) so I need some confirmation here:
## \int E ⋅ ds = \frac {Q} {ε_0} = \frac {1} {ε_0} \int -P dA ##

This will become:
## E(R) 4πR^2 = -\frac {1} {ε_0} PR4πR^2 ##

For 0<R<a : E(R) = 0
For a<R<b : ## E(R) = -\frac {1} {ε_0} PR ##
For b<R : E(R) = 0

The problem here is the solution show : For a<R<b : ## E(R) = -\frac {1} {ε_0} P ##
Did I go wrong somewhere or is this a typo in the solutions?
 
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I agree with your result but depends what is that P that appears in the solution key. Is it the vector ##\mathbf{P}=PR\mathbf{a_R}## or the constant ##P##. I think the solution key means the vector ##\mathbf{P}##.
 
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