Showing posts with label electrostatics. Show all posts
Showing posts with label electrostatics. Show all posts

Saturday, March 03, 2012

Electrostatics - Multiple Choice Questions on Electric Field and Potential

Today we will discuss a few simple, but interesting, multiple choice questions on electrostatics. Here are the questions:

(1) ABC is an equilateral triangle. When positive charges Q and 2Q are placed at points A and B, the electric potential at the mid point (O) of AB is found to be 180 V. What is the electric potential at the vertex C of the triangle under this condition?

(a) 60 V

(b) 90 V

(c) 120 V

(d) 180 V

(e) 240 V

The distance of the vertex C of the triangle from the charges is twice the distance from the point O. Since the electric potential due to a point charge is inversely proportional to the distance, the potential at the vertex C must be half the value at C. So the answer is 90 V.

[Mathematically, you will write (with usual notations)

(1/4πε0)(3Q/r) = 180 and

(1/4πε0)(3Q/2r) = x

This gives x = 90 V]

(2) Equal and opposite point charges + Q and Q are fixed at the corners A and B of an equilateral triangle (Fig.). If a negative point charge (– q) is placed at the vertex C of the triangle, the net force on this charge is directed

(a) towards right

(b) towards left

(c) towards A

(d) towards B

(e) towards the mid point of side AB

The force on the charge q due to the charge + Q is attractive and is directed along CA. The force due to the charge – Q is repulsive and is directed along BC. Since these forces have the same magnitude, their resultant acts parallel to BA. The net force on the charge – q is thus directed leftwards [Option (b)].

(3) A cube of side 4 cm has a constant electric potential of 2 volt on its surface. If there are no charges inside the cube, the potential at a distance of 1 cm from the centre of the cube is

(a) zero

(b) 0.25 V

(c) 0.5 V

(d) 1 V

(e) 2 V

Since the surface of the cube is an equipotential surface and there are no charges inside the cube, the electric field inside the cube must be zero. This means that the electric potential everywhere inside the cube is 2 V itself [Option (e)].

(4) A spherical conductor of radius R has a central cavity (Fig.) with a negative point charge (q) located at the centre of the cavity (without touching the surface of the cavity). The electric fiel at a point P distant r from the centre of the sphere is

(a) q/4πε0r2 directed towards the sphere

(b) q/4πε0r2 directed away from the sphere

(c) q/4πε0r2 directed upwards

(d) q/4πε0r2 directed downwards

(e) zero

The negative charge at the centre of the cavity will induce positive charge q on the surface of the cavity and negative charge –q on the outer surface of the sphere. The situation is similar to that of a spherical conductor carrying a charge –q so that the magnitude E of the electric field at the point P is given by

E = q/4πε0r2

Since the field is due to negative charge, the direction of the field is towards the centre of the sphere.

Sunday, October 02, 2011

Multiple Choice Questions on Unusual Combinations of Capacitors

"It is unwise to be too sure of one's own wisdom. It is healthy to be reminded that the strongest might weaken and the wisest might err."

– Mahatma Gandhi


Today we will consider a few questions on unconventional combinations of capacitors which occasionally find place in entrance examination question papers conducted for admitting students to medical, engineering and other degree courses.

(1) Four parallel metal plates are arranged in air as shown, with the same separation ‘d’ between neighbouring plates. If the area (of one surface) of each plates is A, the capacitance between the terminals T1 and T2 is

(a) 4ε0A/d

(b) ε0A/d

(c) 2ε0A/d

(d) 3ε0A/d

(e) ε0A/3d

Let us number the plates starting from the top as 1, 2, 3, and 4 respectively. The lower surface of plate No.1 and the upper surface of plate No.2 with air in between makes a capacitor of capacitance ε0A/d.

The lower surface of plate No.2 and the upper surface of plate No.3 with air in between makes another capacitor of capacitance ε0A/d.

The lower surface of plate No.3 and the upper surface of plate No.4 with air in between makes a third capacitor of capacitance ε0A/d.

This arrangement therefore makes three capacitors in parallel. The capacitance value of each capacitor is ε0A/d so that the parallel combined value which appears between the terminals T1 and T2 is 3ε0A/d [Option (d)].

(2) If the connection of metal plates in the above question is modified as shown in the adjoining figure, the capacitance between terminals T1 and T2 is

(a) ε0A/2d

(b) 3ε0A/2d

(c)0A/d

(d) 0A/d

(e) 0A/3d

In this case the capacitor at the centre (having capacitance ε0A/d) appears directly across the terminals T1 and T2. The upper and lower capacitors (each of value ε0A/d) are connected in series and this series combination having effective capacitance ε0A/2d also appears between the terminals T1 and T2. Therefore, the effective capacitance between T1 and T2 is ε0A/d + ε0A/2d = 3ε0A/2d [Option (b)].

(3) If a fifth plate is added to the combination shown in question No.1, as shown in the figure, what is the effective capacitance between T1 and T2?

(a) ε0A/4d

(b) ε0A/5d

(c) 0A/d

(d) 0A/5d

(e) 0A/d

Once you answer question No.1, this question becomes quite simple. You can easily see that there are four identical capacitors (each having capacitance ε0A/d) connected in parallel. Therefore, the effective capacitance between T1 and T2 is 4ε0A/d [Option (e)].

You can find a few more questions (with solution) in this section here.

Sunday, March 06, 2011

Multiple Choice Practice Questions on Electrostatics

“Live as if you were to die tomorrow. Learn as if you were to live for ever.”

Mahatma Gandhi


If you grasp the fundamental principles well, you will be able to answer multiple choice questions within the stipulated time. If you are confused about the fundamental principles, you will be tempted to waste your time while dealing with even simple questions just because of some simple distractions. See the following questions:

(1) A battery of emf 12 V is connected in series with two initially uncharged capacitors, each of value 100 μF (Fig.). The capacitors are fully charged. If the total energy spent by the battery for charging the capacitors is E joule, the energy of each capacitor is

(a) E

(b) E/2

(c) 2 E

(d) E/4

(e) E/8

If the total charge supplied by the battery is Q coulomb, the total energy E supplied by the capacitor is given by

E = VQ joule where V is the emf of the battery (which is 12 volt).

The two identical 100 μF capacitors in series is equivalent to a single capacitor of capacitance C = 50 μF. The energy of this charged capacitor combination is ½ CV2 joule = ½ VQ joule since Q = CV.

Therefore, the energy of the charged capacitor combination is ½ E.

Since there are two identical capacitors in the combination, the energy of each capacitor is E/4.

[So the capacitors have gained a total energy of E/2, even though the battery has delivered a total energy E. What happens to the other half of the energy? Well, it is irrecoverably lost as heat generated in the resistance of the circuit].

(2) Charges of equal magnitude are fixed at the diagonally opposite corners A and C of a non conducting square frame ABCD (Fig.). In case (i) the charges at A and C are positive and a third free negative charge q is moved from B to D. In case (ii) the charges at A and C are negative and a third free negative charge q is moved from B to D. In case (iii) the charges at A and C are of opposite sign and a third free negative charge q is moved from B to D. Pick out the correct statement regarding the work done for moving the charge q:

(a) In case (i) the work done is positive

(b) In case (ii) the work done is positive

(c) In case (i) the work done is negative

(d) In case (iii) the work done is positive

(e) In all cases the work done is zero

In case (i) the potentials at B and D are positive, but of equal value. In case (ii) the potentials at B and D are negative, but of equal value. In case (iii) the potentials at B and D are zero. Therefore, in all cases the potential difference between points B and D is zero so that the work done in moving the charge q from B to D is zero.

You will find some useful questions (MCQ) with solution here.

Tuesday, August 18, 2009

AIEEE 2009 Multiple Choice Questions (MCQ) with Solution on Electrostatics

The following four questions which appeared in the All India Engineering/Architecture Entrance Examination 2009 (AIEEE 2009) will be beneficial to most of the entrance test takers. Those who prepare for AP Physics C exam and physics GRE may take special note of question no.2. Here are the questions with solution:

(1) A charge Q is placed at each of the opposite corners of a square. A charge q is placed at each of the other two corners. If the net electric force on Q is zero, then Q/q equals

(1) – 1/√2

(2) – 2√2

(3) –1

(4) 1

The electric force FQQ (Fig.) on Q because of the charge Q at the opposite corner is repulsive and is given by

F1 = (1/4πε0)(Q2 /2a2) since the distance between the charges Q and Q is 2×a/√2 = a√2

The electric forces FQq and FQq (Fig.) on Q because of the charges q and q at the adjacent corners are perpendicular to each other. Each force has magnitude given by

FQq = (1/4πε0)(Qq/a2).

Their resultant F2 has magnitude √2 times the above value:

F2 = (1/4πε0)(√2 Qq/a2).

Since the net force on Q is zero, we have

F1 + F2 = 0

Therefore, (1/4πε0)(Q2 /2a2) + (1/4πε0)(√2 Qq/a2) = 0

This gives Q/q = – 2√2

[The charges Q and q must be of opposite sign so that the force between Q and q is attractive to ensure that F1 and F2 are opposite in directions and the net force on Q is zero as given in the question].

(2) Let P(r) = Qr/πR4 be the charge density distribution for a solid sphere of radius R and total charge Q. For a point ‘p’ inside the sphere at distance r1 from the centre of the sphere, the magnitude of electric field is

(1) Qr12 /3πε0 R4

(2) 0

(3) Q/4πε0 r12

(4) Qr12 /4πε0 R4

Charge dQ contained in the spherical shell of radius r and thickness dr is (Qr/πR4)(4πr2dr) = (4Q/R4) r3dr

Charge Q1 contained in the spherical volume of radius r1 is therefore given by

Q1 = 0r1 (4Q/R4) r3dr = (4Q/R4)(r14/4) = Qr14 /R4

If E is the electric field at distance r1 from the centre of the sphere, we have from Gauss theorem,

r12E = Qr14 /R4ε0 from which

E = Qr12 /4πε0 R4

[Remember that the charges distributed with spherical symmetry outside the point p will produce zero field at p and the field at p is indeed given correctly by the above expression].

(3) Two points P and Q are maintained at the potentials of 10 V and – 4 V, respectively. The work done in moving 100 electrons from P to Q is

(1) 2.24×10–16 J

(2) – 9.60×10–17 J

(3) 9.60×10–17 J

(4) – 2.24×10–16 J

This is a simple question. The potential difference ∆V between P and Q is 10 V – (– 4 V) = 14 V. Since the electrons are negatively charged, external work (positive work) has to be done to move them from the higher potential point P to the lower potential point Q.

The work done = q∆V = (100×1.6×10–19)×14 J = 2.24×10–16 J

(4) This question contains Statement-1 and statement-2. Of the four choices given after the statements, choose the one that best describes the two statements.

Statement 1 : For a charged particle moving from point P to point Q, the net work done by an electrostatic field on the particle is independent of the path connecting point P to point Q.

Statement 2 : The net work done by a conservative force on an object moving along a closed loop is zero.

(1) Statement-1 is true, Statement-2 is true; Statement-2 is the correct explanation of Statment-1.

(2) Statment-1 is true, Statement-2 is true; Statement-2 is not the correct explanation of Statement-1.

(3) Statement-1 is false, Statement-2 is true.

(4) Statement-1 is true, Statement-2 is false

Electrostatic field is conservative and the net work done by an electrostatic field on a charged particle is dependent only on the initial and final positions of the charged particle. (It is independent of the path connecting the initial and final positions).

The correct option is (1).

You will find some more useful multiple choice questions with solution from electrostatics at AP Physics Resources.

Wednesday, June 11, 2008

IIT-JEE 2008 Multiple Choice Questions on Electrostatics

The following two questions from Electrostatics were included under Straight Objective Type (Multiple choice, single answer type) in the IIT-JEE 2008 question paper:

(1) Consider a system of three charges q/3, q/3 and –2q/3 placed at points A, B and C respectively as shown in the figure. Take O to be the centre of the circle of radius R and angle CAB = 60º

(a) The electric field at point O is q/8πε0R2

(b) The potential energy of the system is zero

(c) The magnitude of the force between the charges at C and B is q2/54πε0R2

(d) The potential at point O is q/12πε0R

The electric field at O is due to the negative charge at C only since the equal positive charges situated at A and B will produce equal and opposite fields at O (and they will mutually cancel). The field at O is therefore negative and the option (a) is obviously wrong. Option (b) also is obviously wrong.

The magnitude of the force (F) between the charges at C and B is given by

F = (1/4πε0) [(2q/3)(q/3)/(2Rsin60º)2].

Thus F = q2/54πε0R2 as given in option (c).

(2) A parallel plate capacitor with plates of unit area and separation d is filled with a liquid of dielectric constant K = 2. The level of liquid is d/3 initially. Suppose the liquid level decreases at a constant speed V. The time constant as a function of time t is

(a) 6ε0R/(5d + 3Vt)

(b) (15d + 9Vt) ε0R/(2d2 – 3dVt – 9V2t2)

(c) 6ε0R/(5d 3Vt)

(d) (15d – 9Vt) ε0R/(2d2 + 3dVt – 9V2t2)

When a dielectric slab of thickness t1 and dielectric constant K is introduced in between the plates of a parallel plate air capacitor of plate area A and plate separation d, the effective capacitance changes from ε0A/d to ε0A/[dt1 + (t1/K)]

The effective capacitance C of a parallel plate capacitor with parallel dielectric slabs of thickness t1, t2, t3 etc. of dielectric constants K1, K2, K3 etc. respectively is given by the series combined value of capacitors with these dielectrics. Therefore,

1/C = 1/(K1ε0A/t1) + 1/(K2ε0A/t2) + 1/(K3ε0A/t3) + etc.

With a single slab of thickness t1 and dielectric constant K introduced between the plates, we have

1/C = 1/(Kε0A/t1) + 1/[ε0A/(d t1)] from which C = ε0A/[dt1 + (t1/K)]

In the present problem, the thickness of the layer of liquid (which serves as the dielectric slab) at the instant t is (d/3) V t and the thickness of the air space is (2d/3) + V t.

The effective capacitance is therefore given by

C = ε0A/[{(2d/3) + Vt} + {(d/3) Vt}/k)]

Substituting for A = 1 and K = 2, we obtain C = 6ε0/(5d + 3Vt).

The time constant of the circuit = RC = 6ε0R/(5d + 3Vt).

Reality is merely an illusion, albeit a very persistent one. 
Albert Einstein 

Sunday, April 06, 2008

Two Questions from Electrostatics-- Capacitor Combinations

Here are two multiple choice questions on effective capacitance of capacitor networks. [The first question was found to be some what difficult for the students (from their response)]:

(1) An unusual type of capacitor is made using four identical plates P1, P2, P3 and P4, each of area A arranged in air with the same separation d as shown in the figure. A thin wire outside the system of plates connects the plates P2 and P4. Wires soldered to the plates P1 and P3 serve as terminals T1 and T2 of the system. What is the effective capacitance between the terminals T1 and T2?

(a) (2ε0A)/3d

(b) (3ε0A)/2d

(c) (3ε0A)/d

(d) (ε0A)/d

(e) (ε0A)/2d

The arrangement contains 3 identlcal capacitors C1, C2 and C3 each of capacitance (ε0A)/d arranged as shown in the adjoining figure. Plate P2 is common for C1 and C2. Likewise, plates P3 is common for C2 and C3. The capacitors C2 and C3 are connected in parallel (to produce an effective value 2ε0A/d) and this parallel combination is connected in series with the capacitor C1 of value ε0A/d . The effective capacitance C between the terminals T1 and T2 is therfore given by

C = [(2ε0A/d) ×(ε0A/d)] / [(2ε0A/d) +(ε0A/d)].

Therefore, C = (2ε0A)/3d

(2) Four 2 μF capacitors and a 3 μF capacitor are connected as shown in the figure. The effective capacitance between the points A and B is
(a) 3 μF

(b) 2 μF

(c) 1.5 μF

(d) 1 μF

(e) 0.5 μF

This is a very simple question once you identify the circuit to be a balanced Wheatstone’s bridge. The 3 μF capacitor is connected between equipotential points and you can ignore it. Without the diagonal branch, there are four 2 μF capacitors only. The capacitors in the upper pair are in series and produce a value of 1 μF. The capacitors in the lower pair also produce a value of 1 μF. Since they are in parallel the effective capacitance between the points A and B is 2 μF.