Electric Field Due to a Line of Charge Not on Its Axis
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Take
E0=5×103 N/C, l=2 cm,
a=1 cm, ε0=8.86×10−12 C2/Nm2
- 1.1×10−12 C
- 2.2×10−12 C
- 0.6×10−14 C
- None of the above
An infinitely long uniform line charge distribution of charge per unit length λ lies parallel to the y-axis in the y-z plane at z=√32a. If the magnitude of the flux of the electric field through the rectangular surface ABCD lying in the x-y plane with its centre at the origin is λLnε0 (ε0= permittivity of free space), then the value of n is
[K=14πε0]
- √2Kλd
- 2√2Kλd
- Kλ√2d
- 12√2Kλd
- 10√2
- 10
- 20√2
- 20
A long cylindrical wire carries a positive charge of linear density 2×10−8Cm−1 . An electron revolves around it in a circular path under the influence of the attractive electrostatic force. Find the kinetic energy of the electron . Note that it is independent of the radius.
- E0πR2
- 2E0πR2
- 2E0πR
- E02πR
- αl3
- 2αl3
- 3αl3
- 4αl3
- 5 N-m2/C
- 10 N-m2/C
- 15 N-m2/C
- Zero
- 0.15 N-m2/C
- 0.25 N-m2/C
- 0.35 N-m2/C
- 0.45 N-m2/C
Find the magnitude of the electric field at a point 4 cm away from a line charge od density 2×10−11 C m−1
- zero
- along the diagonal BD
- perpendicular to side AB
- along the diagonal AC
- increase
- decrease
- first increase and then decrease
- remains unchanged
Then, for the situation shown in figure at the Gaussian surface
- →E due to q2 would be zero
- →E due to both q1 and q2 would be non-zero
- ϕ due to both q1 and q2 would be non-zero
- ϕ due to q2 would be zero
A 10 -cm long rod carries a charge of +50μC distributed uniformly along its length. Find the magnitude of the electric field at a point 10 cm from from both the ends of the rod.
E∝rp (r<R) and E∝r−q (r>R)
where, r is the distance from the axis of the region. Find the value of p+q.
A uniformly charged rod (with total charge Q) and length l applies a force on other charge Q1placed on its axis (i.e. along the rod) at a distance 1000l from its centre can be approximated as KQQ1(1000l)2 The reason it came out to be so is because
For such large distances, the rod can be considered as a point charge
charges are conserved
charge is quantized
charges are invariant in nature
- 1×10−17 J
- 2×10−17 J
- 3×10−17 J
- 4×10−17 J
- 150 N/C
- 75 N/C
- 0.6 kN/C
- 4.8 kN/C
- λ4ϵ0
- 2ϵ0λ
- λ4ϵ0R
- 2πϵ0λ
Column-1 Column-2
(a) Current density | (p) is more at 1 |
(b) Electric field | (q) is more at 2 |
(c) Resistance per unit length | (r) is same at both sections 1 and 2 |
(d) Potential difference per unit length | (s) Data insufficient |
- a→p ; b→q ; c→r ; d→s
- a→p ; b→p ; c→q ; d→q
- a→p ; b→q ; c→r ; d→r
- a→p ; b→p ; c→p ; d→p
- 4 cm from the smaller charge and the point inside
- 4 cm from the smaller charge and the point outside
- 4 cm from the bigger charge towards the smaller charge
- 12 cm from both charges
रेखीय आवेश घनत्व λ वाले सीधे लम्बे तार के कारण बिंदु P पर नेट विद्युत क्षेत्र है
- λπε0r
- λ2πε0r
- Zero
शून्य - λ4πε0r
A charge Q is distributed uniformly along a rod of lengths L. The electric field at a distance ‘d’ along its axis from its closer end will be
None of these
- 1.6×10−13 N (towards west)
- 1.6×10−13 N (towards west)
- 1.6×10−10 N (towards east)
- 1.6×10−10 N (towards west)
[K=14πε0]
- √2Kλd
- 2√2Kλd
- Kλ√2d
- 12√2Kλd
- along vector →A
- along vector →B
- along vector →C
- zero
- 0.562×107
- 5.62×107
- 562×107
- 0.0562×107