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Electrostatics question

2015 · Shift 2 · Q41
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Electrostatics question

2015 · Shift 2 · Q41

JEE AdvancedPhysicsElectrostaticsMultiple correct+4 / −2
Consider a uniform spherical charge distribution of radius R1{R_1}R1​ centred at the origin O.O.O. In this distribution, a spherical cavity of radius R2,{R_2},R2​, centred at PPP with distance OP=a=R1−R2OP=a = {R_1} - {R_2}OP=a=R1​−R2​(see figure) is made. If the electric field inside the cavity at position r→\overrightarrow rr is E→(r)→,\overrightarrow E \overrightarrow {\left( r \right)} ,E(r)​, then the correct statement(s) is (are) JEE Advanced 2015 Paper 2 Offline Physics - Electrostatics Question 49 English
  1. A
    E→\overrightarrow EE is uniform, its magnitude is independent of R2{R_2}R2​ but its direction depends on r→.\overrightarrow r .r.
  2. B
    E→\overrightarrow EE is uniform, its magnitude depends on R2{R_2}R2​ and its direction depends on r→.\overrightarrow r .r.
  3. C
    E→\overrightarrow EE is uniform, its magnitude is independent of a but its direction depends on a→\overrightarrow aa
  4. D
    E→\overrightarrow EE is uniform and both its magnitude and direction depend on a→\overrightarrow aa
View written solutionFree

Correct answer: D

  1. Use superposition

A spherical cavity inside a uniformly charged solid sphere can be treated as:

  • a full uniformly charged sphere of charge density ρ\rhoρ, centered at OOO, plus
  • a negative uniformly charged sphere of charge density −ρ-\rho−ρ, centered at PPP.

So the electric field inside the cavity is

E⃗(r⃗)=E⃗1(r⃗)+E⃗2(r⃗).\vec E(\vec r)=\vec E_1(\vec r)+\vec E_2(\vec r).E(r)=E1​(r)+E2​(r).
  1. Field inside a uniformly charged sphere

For a uniformly charged sphere of volume charge density ρ\rhoρ, the electric field at an internal point with position vector r⃗\vec rr measured from its center is

E⃗=ρ3ε0 r⃗.\vec E=\frac{\rho}{3\varepsilon_0}\,\vec r.E=3ε0​ρ​r.

Therefore:

  • For the big sphere centered at OOO,

    E⃗1(r⃗)=ρ3ε0 r⃗.\vec E_1(\vec r)=\frac{\rho}{3\varepsilon_0}\,\vec r.E1​(r)=3ε0​ρ​r.
  • For the cavity, represented as a sphere of charge density −ρ-\rho−ρ centered at PPP, the position vector relative to PPP is

    r⃗−a⃗,\vec r-\vec a,r−a,

    where a⃗=OP→\vec a=\overrightarrow{OP}a=OP. Hence

    E⃗2(r⃗)=−ρ3ε0(r⃗−a⃗).\vec E_2(\vec r)=\frac{-\rho}{3\varepsilon_0}(\vec r-\vec a).E2​(r)=3ε0​−ρ​(r−a).

  1. Add the two fields
E⃗(r⃗)=ρ3ε0r⃗−ρ3ε0(r⃗−a⃗)\vec E(\vec r)=\frac{\rho}{3\varepsilon_0}\vec r-\frac{\rho}{3\varepsilon_0}(\vec r-\vec a)E(r)=3ε0​ρ​r−3ε0​ρ​(r−a) E⃗(r⃗)=ρ3ε0[r⃗−r⃗+a⃗]\vec E(\vec r)=\frac{\rho}{3\varepsilon_0}\left[\vec r-\vec r+\vec a\right]E(r)=3ε0​ρ​[r−r+a] E⃗(r⃗)=ρ3ε0 a⃗\boxed{\vec E(\vec r)=\frac{\rho}{3\varepsilon_0}\,\vec a}E(r)=3ε0​ρ​a​
  1. Interpretation

This result shows:

  • The field is uniform inside the cavity, since it does not depend on r⃗\vec rr.
  • Its magnitude is E=ρa3ε0,E=\frac{\rho a}{3\varepsilon_0},E=3ε0​ρa​, so it depends on aaa.
  • Its direction is along a⃗\vec aa.

Since a=R1−R2a=R_1-R_2a=R1​−R2​, the magnitude also indirectly depends on R2R_2R2​, but the most direct statement among the options is dependence on a⃗\vec aa.


  1. Check each option
  • A: Says field is uniform, magnitude independent of R2R_2R2​, but direction depends on r⃗\vec rr.
    Wrong, because direction does not depend on r⃗\vec rr; field is constant.

  • B: Says field is uniform, magnitude depends on R2R_2R2​, but direction depends on r⃗\vec rr.
    Wrong, again direction does not depend on r⃗\vec rr.

  • C: Says field is uniform, magnitude independent of aaa, but direction depends on a⃗\vec aa.
    Wrong, magnitude is proportional to aaa.

  • D: Says field is uniform and both magnitude and direction depend on a⃗\vec aa.
    Correct.


  1. Final answer
Option D\boxed{\text{Option D}}Option D​
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