Infinite Sheet
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The maximum electric field strength E due to a uniformly charged ring of radius r, happens at a distance x, where value of x is (x is measured from the centre of the ring)
x = R
x=R2
x=R√2
x=√2R
Body 100 V/m
- 800 units
- 300 units
- 400 units
- 1500 units
(b) Draw the equipotential surfaces due to an electric dipole. Locate the points where the potential due to the dipole is zero.
If the dot product of two non-zero vectors is zero, then the vectors
- can have any orientation.
- are anti-parallel to each other.
- are parallel to each other.
- are perpendicular to each other.
A charged ball B hangs from a silk thread S, which makes an angle θ with a large charged conducting sheet P, as shown in the figure. The surface charge density σ of the sheet is proportional to
- sin θ
- tan θ
- cos θ
- cot θ
(b) Use Gauss's law to prove that electric field inside a uniformly charged spherical shell is zero.
- III→II→I→IV
- All tie
- II→I→III→IV
- I & II tie →III→IV
If E1(r0)=E2(r0)=E3(r0) at a given distance r0, then
- Q=4σπr20
- r0=λ2πσ
- Q=2σπr20
- r0=λπσ
- 98
- 43
- 32
- 89
[Assume x to be very small as compared to dimension of sheet]
A charge is distributed over three concentric spherical shells of radii such that their surface charge densities are equal to one another. The total potential at a point at distance from their common centre, where , would be :
- 1 m
- 2 m
- 3 m
- 4 m
- tanθ=σq2ϵ0mg
- tanθ=σq3ϵ0mg
- tanθ=2σqϵ0mg
- tanθ=3σqϵ0mg
- z=constant[x2y2]
- z=constant[xy2]
- z=constant[x4y2]
- None
Equipotential surfaces cannot ________.
- P
- P1
- P2
- P, P1 and P2
- T=2π√4qE5mL
- T=2π√5mL4qE
- T=2π√mL5qE
- T=2π√3mL2qE
- v=√2mgl+2q0×σ2ϵ0×Lm
- v=√2mgl+2q0×σ2ϵ0×Lm
- v=√2mgl+2q0×σ2ϵ0×Lm
- v=√2mgl2+2q0×σ2ϵ0×L2mL2
- 180∘, 14πϵ0Q2(2L)2
- 90∘, 14πϵ0Q2L2
- 180∘, 14πϵ0Q22L2
- 180∘, 14πϵ0Q2L2
A non-conducting square sheet of side 10 m is charged with a uniform surface charge density, σ=−60μCm2 . Find the magnitude and orientation of electric field vector due to the sheet at a point which is d = 0.02 mm away from the midpoint of the sheet.
3.39 x 106 N/C, away from the sheet
6.78 x 106 N/C, towards the sheet
3.39 x 106 N/C, towards the sheet
6.78 x 106 N/C, away from the sheet
- E/2
- E
- 2E
- 4E
- 0 N/C
- 2λπε0R N/C
- λπε0R N/C
- λ2πε0R N/C
- QωR2
- QωR22
- 23QωR2
- 54QωR2