Two Infinite Sheets
Trending Questions
- Q2
- Q4
- −Q2
- −Q4
What is the electric potential at their common centre ?
- σR/ϵ0
- σϵ0(R−r)
- σϵ0(R+r)
- None of these
- 6
- 7
- 15
- 20
[1 Mark]
- r−1
- r2
- r−32
- independent of r
- −(σ1+σ2)2ϵ0
- −(σ1 σ2)2ϵ0
- (σ1+σ2)2ϵ0
- (σ1−σ2)2ϵ0
- 10 N/C
- 20 N/C
- 30 N/C
- 40 N/C
- E1>E2
- E1<E2
- E1=E2
- can't be interpreted
- σ2ϵ0
- σϵ0
- Depends on the location of the point
- Zero
- Q
- Q2
- Q8
- Q4
- 10 N/C
- 20 N/C
- 30 N/C
- 40 N/C
- −4σϵ0^k
- −3σ2ε0^k
- 5σ2ε0^k
- −5σ2ε0^k
The infinite sheets of uniform charge density 10μCm2, −10μCm2and5μCm2 are placed in vacuum as shown. The direction of field intensity at points A and B are respectively?
Right, left
Left, Right
Right, Right
Left, Left
- Q4
- Q2
- Q
- Q8
- Ua=Ud
- Ua=kUd
- Ud=kUa
- Ua=(k−1)Ud
A uniformly charged spherical conductor has a radius of 1m and surface charge density 0.8Cm2. The electric field magnitude because of this at a point 1m radially away, from the surface of the sphere is
4.5×109NC
9×109NC
2.25×1010NC
7.2×109NC
The potential difference between two parallel plates is 104 volt. If the plates are separated by 0.5cm, the force on an electron between the plates is :
- 2×104N
- 3.2×10−13N
- 32×1012N
- 20N
- −(σ1+σ2)2ϵ0
- −(σ1 σ2)2ϵ0
- (σ1+σ2)2ϵ0
- (σ1−σ2)2ϵ0
- 6×107 V
- 3×107 V
- 4×107 V
- 2×107 V
- Aϵ02d , 2.5 qdϵ0A
- 2Aϵ0d , qd2ϵ0A
- Aϵ0d , 2.5qdϵ0A
- Aϵ0d , 5qdϵ0A
- σ/ϵ0 towards the positively charge plane
- σ/ϵ0 towards the negatively charged plane
- σ/(2ϵ0) towards the positively charged plane
- 0 and towards any direction
Two large conducting plates are placed parallel to each other with a separation of 2.00 cm between them. An electron starting from rest near one of the plates reaches the other plate in 2.00 microseconds. Find the surface charge density on the inner surfaces.
There identical metal plates with large surface areas are kept parallel to each other as shown in figure (30-E8). The leftmost plate is given a charge Q.the rightmost a charge -2Q and the middle one remains neutral. Find the charge appearing on the outer surface of the rightmost plate.
- −(σ1+σ2)2ϵ0
- −(σ1 σ2)2ϵ0
- (σ1+σ2)2ϵ0
- (σ1−σ2)2ϵ0
The electric field E is measured at a point P(0, 0, d) generated due to various charge distributions and the dependence of E on d is found to be different for different charge distributions. List - I contains different relations between E and d. List - II describes different electric charge distributions, along with their locations. Match the functions in List - I with the related charge distributions in List - II
List - I | List - II |
(P) E is independent of d | (1) A point charge Q at the origin |
(Q) E∝1d | (2) A small dipole with point charges Q at (0, 0, l) and - Q at (0, 0, −l). Take 2l<<d |
(R) E∝1d2 | (3) A infinite line charge coincident with the x-axis, with uniform linear charge density λ. |
(S) E∝1d3 | (4) Two infinite wires carrying uniform linear charge density parallel to the x-axis. The one along (y=0, z=l) has a charge density + λ and the one along (y=0, z=−l) has a charge density −λ. Take 2l<<d |
(5) Infinite plane charge coincident with the xy-plane with uniform surface charge density |
- P→5;Q→3, 4;R→1;S→2
- P→5;Q→3;R→1, 4;S→2
- P→5;Q→3;R→1, 2;S→4
- P→4;Q→2, 3;R→1;S→5
The infinite sheets of uniform charge density 10μCm2, −10μCm2and5μCm2 are placed in vacuum as shown. The direction of field intensity at points A and B are respectively?
Left, Left
Left, Right
Right, left
Right, Right