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Calculate potential energy of a point charge –q placed along the axis due to a charge +Q uniformly distributed along a ring of radius R. Sketch P.E. as a function of axial distance z

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प्रश्न

Calculate potential energy of a point charge – q placed along the axis due to a charge +Q uniformly distributed along a ring of radius R. Sketch P.E. as a function of axial distance z from the centre of the ring. Looking at graph, can you see what would happen if – q is displaced slightly from the centre of the ring (along the axis)?

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उत्तर

The potential energy (U) of a point charge q placed at-potential V, U = qV In our case a negative charged particle is placed at the axis of a ring having charge Q. Let the ring has radius a, the electric potential at an axial distance z from the centre of the ring is 

`V = 1/(4piε_0) Q/sqrt(z^2 + a^2)`

Hence potential energy of a point charge – q is

`U = qV = (-q)[1/(4piε_0) Q/sqrt(z^2 + a^2)]`

⇒ `U = - 1/(4piε_0) (Qq)/sqrt(z^2 + a^2) = 1/(4piε_0) (-Qq)/sqrt(1 + (z/a)^2`

At z = 0, U = `- 1/(4piε_0) (Qq)/a`

At z → `oo`, U → 0

The variation of potential energy with z is shown in the figure. The charge – q displaced would perform oscillations. Nothing can be concluded just by looking at the graph.

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

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एनसीईआरटी एक्झांप्लर Physics Exemplar [English] Class 12
अध्याय 2 Electrostatic Potential And Capacitance
MCQ I | Q 2.22 | पृष्ठ १४

संबंधित प्रश्न

Find out the amount of the work done to separate the charges at infinite distance.


A point charge Q is placed at point 'O' as shown in the figure. Is the potential at point A, i.e. VA, greater, smaller or equal to potential, VB, at point B, when Q is (i) positive, and (ii) negative charge?


Figure shows the field lines due to a positive point charge. Give the sign of potential energy difference of a small negative charge between the points Q and P.


1 volt is equivalent to ______.


The work done in bringing a unit positive charge from infinite distance to a point at distance x from a positive charge Q is W. Then the potential at that point is ______.


  • Assertion (A): An electron has a high potential energy when it is at a location associated with a more negative value of potential, and a low potential energy when at a location associated with a more positive potential.
  • Reason (R): Electrons move from a region of higher potential to region of lower potential.

Select the most appropriate answer from the options given below:


In the circuit shown in figure initially, key K1 is closed and key K2 is open. Then K1 is opened and K2 is closed (order is important). [Take Q1′ and Q2′ as charges on C1 and C2 and V1 and V2 as voltage respectively.]

Then

  1. charge on C1 gets redistributed such that V1 = V2
  2. charge on C1 gets redistributed such that Q1′ = Q2′
  3. charge on C1 gets redistributed such that C1V1 + C2V2 = C1E
  4. charge on C1 gets redistributed such that Q1′ + Q2′ = Q

  1. In a quark model of elementary particles, a neutron is made of one up quarks [charge (2/3) e] and two down quarks [charges –(1/3) e]. Assume that they have a triangle configuration with side length of the order of 10–15 m. Calculate electrostatic potential energy of neutron and compare it with its mass 939 MeV.
  2. Repeat above exercise for a proton which is made of two up and one down quark.

  • Assertion (A): Work done in moving a charge around a closed path, in an electric field is always zero.
  • Reason (R): Electrostatic force is a conservative force.

Charges (+q) and (–q) are placed at points A and B respectively which are a distance 2L apart. C is the midpoint between A and B. What is the work done in moving a charge +Q along the semicircle CRD?

 


The electrostatic potential energy of a charge configuration is well-defined because the electrostatic force is a conservative force, which means:


If a system of like charges, assembled by doing work against their repulsive force, is released, the stored electrostatic potential energy:


For a system of unlike charges (attractive force), an external agent must do work to separate them because the system:


While assembling a system of charges, the work done in bringing the first charge \[q_1\] from infinity to its Position 1 is:


For a system of n charges, the total number of unique charge pairs whose potential energies must be summed is:


For n charges \[q_1, q_2, \ldots, q_n\] at positions \[r_1, r_2, \ldots, r_n\], where \[r_{ij}\] is the distance between charge i and charge j, the total electrostatic potential energy of the system is:


For a pair of like charges, the positive potential energy (U > 0) physically signifies that:


Four charges +q, -q, +q, -q are arranged alternately at corners A, B, C, D of a square of side d. With +q already at A, the work done in bringing -q from infinity to corner B is:


For the symmetrical arrangement of charges +q, -q, +q, -q at the corners of a square, the electric potential at the centre E due to the four charges is:


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