Sign in
12thPass logo
New chatPYQ LibraryDoubtsRank report
Sign in to see Recents

Your guest activity stays on this device

Sign in to save progress →
Sign in

Electrostatics question

2023 · 1 Feb · Shift 1 · Q44
Guest · filters and generic practice availableBrowsing as a guest · PYQ filters and generic practice are available. Sign in only for personalised features and saved progress.
  1. PYQ Library
  2. /JEE Main
  3. /Physics
  4. /Electrostatics
  5. /2023 · 1 Feb · Shift 1 · Q44

Electrostatics question

2023 · 1 Feb · Shift 1 · Q44

JEE MainPhysicsElectrostaticsMCQ+4 / −1
Let σ\sigmaσ be the uniform surface charge density of two infinite thin plane sheets shown in figure. Then the electric fields in three different region EI,EIIE_{I}, E_{I I}EI​,EII​ and EIIIE_{I I I}EIII​ are: JEE Main 2023 (Online) 1st February Morning Shift Physics - Electrostatics Question 102 English
  1. A
    E⃗I=0,E⃗II=σϵ0n^,EIII=0\vec{E}_{I}=0, \vec{E}_{I I}=\frac{\sigma}{\epsilon_{0}} \hat{n}, E_{I I I}=0EI​=0,EII​=ϵ0​σ​n^,EIII​=0
  2. B
    E⃗I=σ2ϵ0n^,E⃗II=0,E⃗III=σ2ϵ0n^\vec{E}_{I}=\frac{\sigma}{2 \epsilon_{0}} \hat{n}, \vec{E}_{I I}=0, \vec{E}_{I I I}=\frac{\sigma}{2 \epsilon_{0}} \hat{n}EI​=2ϵ0​σ​n^,EII​=0,EIII​=2ϵ0​σ​n^
  3. C
    E⃗I=−σϵ0n^,E⃗II=0,E⃗III=σϵ0n^\vec{E}_{I}=-\frac{\sigma}{\epsilon_{0}} \hat{n}, \vec{E}_{I I}=0, \vec{E}_{I I I}=\frac{\sigma}{\epsilon_{0}} \hat{n}EI​=−ϵ0​σ​n^,EII​=0,EIII​=ϵ0​σ​n^
  4. D
    E⃗I=2σϵ0n^,E⃗II=0,E⃗III=2σϵ0n^\vec{E}_{I}=\frac{2 \sigma}{\epsilon_{0}} \hat{n}, \vec{E}_{I I}=0, \vec{E}_{I I I}=\frac{2 \sigma}{\epsilon_{0}} \hat{n}EI​=ϵ0​2σ​n^,EII​=0,EIII​=ϵ0​2σ​n^
View written solutionFree

Correct answer: C

  1. Field due to one infinite charged sheet

For an infinite thin plane sheet with uniform surface charge density σ\sigmaσ, the magnitude of electric field on either side is

E=σ2ε0E=\frac{\sigma}{2\varepsilon_0}E=2ε0​σ​

Direction:

  • away from the sheet if σ>0\sigma>0σ>0
  • toward the sheet if σ<0\sigma<0σ<0
  1. Interpretation of the figure

Since the options indicate zero field in the middle region for the correct configuration, the two sheets must carry equal and opposite surface charge densities, +σ+\sigma+σ and −σ-\sigma−σ, with regions:

  • Region III: left of both sheets
  • Region IIIIII: between the sheets
  • Region IIIIIIIII: right of both sheets

Let n^\hat nn^ be the unit vector from left to right.

  1. Electric field in each region by superposition

Region III (left of both sheets)

  • Field due to left positively charged sheet: toward left, i.e. −σ2ε0n^-\dfrac{\sigma}{2\varepsilon_0}\hat n−2ε0​σ​n^
  • Field due to right negatively charged sheet: toward the negative sheet, i.e. toward right, so +σ2ε0n^+\dfrac{\sigma}{2\varepsilon_0}\hat n+2ε0​σ​n^

These cancel if the left sheet is +σ+\sigma+σ and right is −σ-\sigma−σ. But option C has nonzero outer regions and zero middle region, which corresponds to the actual figure being two sheets with same sign? Let us evaluate carefully.

If the two sheets have the same positive charge density σ\sigmaσ:

  • In Region III, both fields point left:
E⃗I=−σ2ε0n^−σ2ε0n^=−σε0n^\vec E_I=-\frac{\sigma}{2\varepsilon_0}\hat n-\frac{\sigma}{2\varepsilon_0}\hat n=-\frac{\sigma}{\varepsilon_0}\hat nEI​=−2ε0​σ​n^−2ε0​σ​n^=−ε0​σ​n^
  • In Region IIIIII, fields oppose and cancel:
E⃗II=0\vec E_{II}=0EII​=0
  • In Region IIIIIIIII, both fields point right:
E⃗III=σ2ε0n^+σ2ε0n^=σε0n^\vec E_{III}=\frac{\sigma}{2\varepsilon_0}\hat n+\frac{\sigma}{2\varepsilon_0}\hat n=\frac{\sigma}{\varepsilon_0}\hat nEIII​=2ε0​σ​n^+2ε0​σ​n^=ε0​σ​n^
  1. Match with options

This gives

E⃗I=−σε0n^,E⃗II=0,E⃗III=σε0n^\vec E_I=-\frac{\sigma}{\varepsilon_0}\hat n,\qquad \vec E_{II}=0,\qquad \vec E_{III}=\frac{\sigma}{\varepsilon_0}\hat nEI​=−ε0​σ​n^,EII​=0,EIII​=ε0​σ​n^

which matches Option C.

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

This means the two sheets in the figure must be identically charged, and the field cancels between them while adding outside.

PreviousNext

More from Electrostatics

  • Two equal positive point charges are separated by a distance 2a. The distance of a point from the centre of the line joining two charges on the equatorial line (perpendicular bisector) at which force experienced by a test charge q0​…2023 · Numerical
  • A cubical volume is bounded by the surfaces x=0,x=a,y=0,y=a,z=0,z=a. The electric field in the region is given by E=E0​xi^. Where E0​=4×104 NC−1 m−1…2023 · Numerical
  • For a uniformly charged thin spherical shell, the electric potential (V) radially away from the centre (O) of shell can be graphically represented as - Includes diagram2023 · MCQ
  • A dipole comprises of two charged particles of identical magnitude q and opposite in nature. The mass 'm' of the positive charged particle is half of the mass of the negative charged particle. The two charges are separated by a distance…2023 · MCQ
  • Graphical variation of electric field due to a uniformly charged insulating solid sphere of radius R, with distance r from the centre O is represented by: Includes diagram2023 · MCQ
  • An electric dipole of dipole moment is 6.0×10−6 Cm placed in a uniform electric field of 1.5×103 NC−1 in such a way that dipole moment is along electric field. The work done in rotating…2023 · Numerical
  • Electric potential at a point 'P' due to a point charge of 5×10−9C is 50 V. The distance of 'P' from the point charge is: (Assume, 4πε0​1​=9×10+9 Nm2C−2…2023 · MCQ
  • Three concentric spherical metallic shells X, Y and Z of radius a, b and c respectively [a < b < c] have surface charge densities σ,−σ and σ respectively. The shells X and Z are at same potential. If the radii of X…2023 · Numerical