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

Consider a uniform electric field in the ẑ direction. The potential is a constant ______. in all space. for any x for a given z. for any y for a given z. on the x-y plane for a given z. - Physics

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प्रश्न

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.

पर्याय

  • a, b and c

  • a, c and d

  • b, c and d

  • c and d

MCQ
रिकाम्या जागा भरा
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उत्तर

b, c and d

Explanation:

We know, the electric field intensity E and electric potential V are E = `- (dV)/(dr)`

Electric potential decreases in the direction of the electric field. The direction of electric field is always perpendicular to one equipotential surface maintained at the high electrostatic potential to another equipotential surface maintained at low electrostatic potential.

The electric field in the z-direction suggests that equipotential surfaces are in the x-y plane. Therefore the potential is a constant for any x for a given z, for any y for a given z and on the x-y plane for a given z.

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Equipotential Surfaces
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पाठ 2: Electrostatic Potential And Capacitance - MCQ I [पृष्ठ १२]

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एनसीईआरटी एक्झांप्लर Physics [English] Class 12
पाठ 2 Electrostatic Potential And Capacitance
MCQ I | Q 2.07 | पृष्ठ १२

संबंधित प्रश्‍न

The top of the atmosphere is at about 400 kV with respect to the surface of the earth, corresponding to an electric field that decreases with altitude. Near the surface of the earth, the field is about 100 Vm−1. Why then do we not get an electric shock as we step out of our house into the open? (Assume the house to be a steel cage so there is no field inside!)


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.)


Draw the equipotential surfaces due to an electric dipole. Locate the points where the potential due to the dipole is zero.


Why is there no work done in moving a charge from one point to another on an equipotential surface?


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


Define equipotential surface. 


Two identical point charges, q each, are kept 2m apart in the air. A third point charge Q of unknown magnitude and sign is placed on the line joining the charges such that the system remains in equilibrium. Find the position and nature of Q.


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 ______.


Consider the following statements and select the correct statement(s).

  1. Electric field lines are always perpendicular to equipotential surface.
  2. No two equipotential surfaces can intersect each other.
  3. Electric field lines are in the direction of tangent to an equipotential surface.

The diagrams below show regions of equipotentials.

(i)
(ii)
(iii)
(iv)

A positive charge is moved from A to B in each diagram.


A unit charge moves on an equipotential surface from a point A to point B, then ______.

Equipotential surfaces ______.


Can two equipotential surfaces intersect each other? 


The work done to move a charge along an equipotential from A to B ______.

  1. cannot be defined as `- int_A^B E.dl`
  2. must be defined as `- int_A^B E.dl`
  3. is zero.
  4. can have a non-zero value.

Prove that a closed equipotential surface with no charge within itself must enclose an equipotential volume.


What is meant by an equipotential surface?


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