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Electrostatics question

2013 · Shift 2 · Q41
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Electrostatics question

2013 · Shift 2 · Q41

JEE AdvancedPhysicsElectrostaticsMultiple correct+4 / −1
Two non-conducting spheres of radii R1{R_1}R1​ and R2{R_2}R2​ and carrying uniform volume charge densities +ρ+ \rho+ρ and −ρ,- \rho ,−ρ, respectively, are placed such that they partially overlap, as shown in the figure. At all points in the overlapping region JEE Advanced 2013 Paper 2 Offline Physics - Electrostatics Question 51 English
  1. A
    The electrostatic field is zero
  2. B
    The electrostatic potential is constant
  3. C
    The electrostatic field is constant in magnitude
  4. D
    The electrostatic field has same direction
View written solutionFree

Correct answer: D, C

  1. Field inside a uniformly charged non-conducting sphere

For a sphere with uniform volume charge density ρ\rhoρ, the electric field at an interior point whose position vector from the center is r⃗\vec rr is

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

For a sphere with charge density −ρ-\rho−ρ, the field becomes

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

This result is valid for all interior points.


  1. Set up vectors for the overlap region

Let the centers of the two spheres be O1O_1O1​ and O2O_2O2​.

Take any point PPP in the overlapping region.

Let

  • r⃗1=O1P→\vec r_1 = \overrightarrow{O_1P}r1​=O1​P​
  • r⃗2=O2P→\vec r_2 = \overrightarrow{O_2P}r2​=O2​P​

Since PPP lies inside both spheres, the field at PPP due to each sphere is given by the interior formula.

So,

  • due to the positively charged sphere: E⃗1=ρ3ε0r⃗1\vec E_1=\frac{\rho}{3\varepsilon_0}\vec r_1E1​=3ε0​ρ​r1​

  • due to the negatively charged sphere: E⃗2=−ρ3ε0r⃗2\vec E_2=-\frac{\rho}{3\varepsilon_0}\vec r_2E2​=−3ε0​ρ​r2​

Hence total field is

=\frac{\rho}{3\varepsilon_0}(\vec r_1-\vec r_2)$$ But $$\vec r_1-\vec r_2=\overrightarrow{O_1P}-\overrightarrow{O_2P}= \overrightarrow{O_1O_2}$$ which is a constant vector, independent of the point $P$. Therefore, $$\boxed{\vec E=\frac{\rho}{3\varepsilon_0}\overrightarrow{O_1O_2}}$$ So throughout the overlapping region, the electric field is **constant as a vector**. That means: - its **magnitude is constant** - its **direction is the same everywhere** Thus **C** and **D** are correct. --- 3. **Check whether the field is zero** Since $$\vec E=\frac{\rho}{3\varepsilon_0}\overrightarrow{O_1O_2}$$ this is zero only if the centers coincide, which is not the case for partial overlap. So **A is false**. --- 4. **Check whether potential is constant** Using $\vec E=-\nabla V$, if $V$ were constant in the overlap region, then $\vec E$ would have to be zero. But the field is nonzero constant. Hence the potential is **not constant**; instead it varies linearly with position. So **B is false**. --- 5. **Option-wise conclusion** - **A:** False - **B:** False - **C:** True - **D:** True Therefore the correct options are $$\boxed{C, D}$$
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