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कर्नाटक बोर्ड पी.यू.सी.पीयूसी विज्ञान 2nd PUC Class 12

Find the equation of the equipotentials for an infinite cylinder of radius r0, carrying charge of linear density λ.

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प्रश्न

Find the equation of the equipotentials for an infinite cylinder of radius r0, carrying charge of linear density λ.

दीर्घउत्तर
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उत्तर

To find the potential at distance r from the line consider the electric field. We note that from symmetry the field lines must be radially outward. Draw a cylindrical Gaussian surface of radius r and length l. Then

`oint E.dS = 1/ε_0 λ1`

Or `E_r.2pirl = 1/ε_0 λ1`

⇒ `E_r = lambda/(2piε_0r)`

Hence, if r0 is the radius,

`V(r) - V(r_0) = - int_(r_0)^r E.dl = λ/(2piε_0)ln  r_0/r`

For a given V,

ln `r/r_0 = - (2piε_0)/λ [V(r) - V(r_0)]`

⇒ r = r0e –2πε0Vr0/λe + 2πε0V(r)/λ

The equipotential surfaces are cylinders of radius r = r0e –2πε0[V(r) – V(r0)]/λ

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पाठ 2: Electrostatic Potential And Capacitance - MCQ I [पृष्ठ १४]

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एनसीईआरटी एक्झांप्लर Physics Exemplar [English] Class 12
पाठ 2 Electrostatic Potential And Capacitance
MCQ I | Q 2.24 | पृष्ठ १४

संबंधित प्रश्‍न

A regular hexagon of side 10 cm has a charge 5 µC at each of its vertices. Calculate the potential at the centre of the hexagon.


Describe schematically the equipotential surfaces corresponding to

(a) a constant electric field in the z-direction,

(b) a field that uniformly increases in magnitude but remains in a constant (say, z) direction,

(c) a single positive charge at the origin, and

(d) a uniform grid consisting of long equally spaced parallel charged wires in a plane.


The discharging current in the atmosphere due to the small conductivity of air is known to be 1800 A on an average over the globe. Why then does the atmosphere not discharge itself completely in due course and become electrically neutral? In other words, what keeps the atmosphere charged?


What are the forms of energy into which the electrical energy of the atmosphere is dissipated during a lightning?
(Hint: The earth has an electric field of about 100 Vm−1 at its surface in the downward direction, corresponding to a surface charge density = −10−9 C m−2. Due to the slight conductivity of the atmosphere up to about 50 km (beyond which it is good conductor), about + 1800 C is pumped every second into the earth as a whole. The earth, however, does not get discharged since thunderstorms and lightning occurring continually all over the globe pump an equal amount of negative charge on the earth.)


Depict the equipotential surfaces for a system of two identical positive point charges placed a distance(d) apart?


Depict the equipotential surface due to
(i) an electric dipole,
(ii) two identical positive charges separated by a distance.


Statement - 1: For practical purpose, the earth is used as a reference at zero potential in electrical circuits.

Statement - 2: The electrical potential of a sphere of radius R with charge Q uniformly distributed on the surface is given by `Q/(4piepsilon_0R)`.


A particle of mass 'm' having charge 'q' is held at rest in uniform electric field of intensity 'E'. When it is released, the kinetic energy attained by it after covering a distance 'y' will be ______.


Which of the following statements is/are correct for equipotential surface?
  1. The potential at all the points on an equipotential surface is same.
  2. Equipotential surfaces never intersect each other.
  3. Work done in moving a charge from one point to other on an equipotential surface is zero.

Which of the following is NOT the property of equipotential surface?


Consider a uniform electric field in the ẑ direction. The potential is a constant ______.

  1. in all space.
  2. for any x for a given z.
  3. for any y for a given z.
  4. on the x-y plane for a given z.

Equipotential surfaces ______.

  1. are closer in regions of large electric fields compared to regions of lower electric fields.
  2. will be more crowded near sharp edges of a conductor.
  3. will be more crowded near regions of large charge densities.
  4. will always be equally spaced.

A curve connecting points that all have equal electric potential is best described as:


A charge \[q_0\] is moved from point A to point B on the same equipotential surface. If the potentials at A and B are \[V_A\] and \[V_B\] respectively, the work done is:


Equipotential surfaces are denser (closer together) in regions where:


What is the shape of the equipotential surfaces for a single point charge (+q)?


For an electric dipole (+q, −q), the equipotential surfaces are best described as:


The relation between the electric field \[\vec{E}\] and the potential gradient is expressed as:


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