Question bank/JEE Main/Physics

JEE MainPhysicsToughElectrostatics

Consider a sphere of radius R which carries a uniform charge
density
ρ\rho. If a sphere of radius R2\frac{R}{2}is carved out of it,
as shown, the ratio

∣E→AE→B∣|\frac{{\overset{\rightarrow}{E}}_{A}}{{\overset{\rightarrow}{E}}_{B}}|
of magnitude of electric field

E→A{\overset{\rightarrow}{E}}_{A}andE→B{\overset{\rightarrow}{E}}_{B},
respectively, at points A and B due to the remaining portion is

Show answer and solution
For a solid sphere
E=ρr3ε0E = \frac{\rho r}{3\varepsilon_{0}}
EA=−ρR2(3ε0)E_{A} = \frac{- \rho R}{2(3\varepsilon_{0})}
∣EA∣=ρR6ε0|E_{A}| = \frac{\rho R}{6\varepsilon_{0}}
Electric field at point
B=EB=E1A+E2AB = E_{B} = E_{1A} + E_{2A}
E1AE_{1A}Electric Field Due to solid sphere of radius R at point
B
=ρR3ε0= \frac{\rho R}{3\varepsilon_{0}}
E2AE_{2A}Electric Field Due to solid sphere of radius R/2R/2 (which having
charge density
−ρ- \rho)
=−ρR54ε0= - \frac{\rho R}{54\varepsilon_{0}}
EB=E1A+E2A=ρR3ε0−ρR54ε0=17ρR54ε0E_{B} = E_{1A} + E_{2A} = \frac{\rho R}{3\varepsilon_{0}} - \frac{\rho R}{54\varepsilon_{0}} = \frac{17\rho R}{54\varepsilon_{0}}
∣EA∣∣EB∣=917\frac{|E_{A}|}{|E_{B}|} = \frac{9}{17}

Source: Grass-G / P-19 Physics paper 28 Nov Fourth.docx

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