If we did all things we are capable of, we would literally astound ourselves.

– Thomas A. Edison

Tuesday, October 06, 2009

Kerala Engineering Entrance 2009 Multiple Choice Questions on Work and Energy

In the KEAM (Engineering ) 2009 question paper three questions were included from the section ‘work, energy and power’. Here are those questions with solution:

(1) A particle is acted upon by a force F which varies with position x as shown in figure. If the particle at x = 0 has kinetic energy of 25 J, then the kinetic energy of the particle at x = 16 m is

(a) 45 J

(b) 30 J

(c) 70 J

(d) 135 J

(e) 20 J

The work done by a variable force acting along the direction of displacement can be found by drawing a force-displacement graph. The area under this graph gives the work done. Since the force has positive and negative values, the area also has positive (+50 units) and negative (– 30 units) values. The net area is +20 units and hence the gain in kinnetic energy during the movement from position x = 0 to the position x = 16 m is 20 J.

The particle has kinetic energy of 25 J at position x = 0. Therefore the kinetic energy at position x = 16 m is 25 + 20 = 45 J.

(2) Two springs P and Q of force constants kP and kQ [kQ = kP/2] are stretched by applying force of equal magnitude. If the energy stored in in Q is E, then the energy stored in P is

(a) E

(b) 2 E

(c) E/8

(d) E/4

(e) E/2

The potential energy (U) of a spring stretched (by a force F) through distance x is given by

U = ½ kx2 where k is the spring constant (force constant) given by k = F/x

This can be rewritten as

U = ½ (F2/k) since x = F/k

The nergy stored in P and Q are respectively given by UP = ½ (F2/kP) and UQ = ½ (F2/kQ).

Therefore, UP/UQ = kQ/kP = ½ as given in the question.

This gives UP = UQ/2 = E/2.

(3) A rod of mass m and length l is made to stand at an angle of 60º with the vertical. Potential energy of this rod in this position is

(a) mgl

(b) mgl/2

(c) mgl/3

(d) mgl/4

(e) mgl/√2

When the rod is kept inclined at an angle of 60º with the vertical, its centre of gravity is raised (from the ground level) by a height h = (l/2)cos 60º = l/4.

The gravitational potential energy of the rod in this position is mgh = mgl/4.

You will find many useful multiple choice questions on work, energy and power at physicsplus and at AP Physics Resources


Saturday, August 15, 2009

AIPMT 2009 - Multiple Choice Questions from Electrostatics

Three questions were included from electrostatics in the All India Pre-Medical/Pre-Dental 2009 Entrance Examination (Preliminary). They are given below with solution. The first question will appear to be a rather difficult and time consuming one. Those who are preparing for AP Physics Exam may make a special note of this question.
(1)
Three concentric spherical shells have radii a, b and c (a < b < c) and have surface charge densities σ, − σ and σ respectively. If VA, VB and VC denote the potentials of the three shells, then for c = a + b, we have

(1) VC = VBVA

(2) VCVBVA

(3) VC = VB = VA

(4) VC = VAVB

The potential V of a spherical shell of radius r having surface charge density σ is given by

V = (1/4πε0)(4πr2σ/r) = σr/ε0 where ε0 is the permittivity of free space.

Potential VA of the shell A is given by

VA = σa/ε0 – σb/ε0 + σc/ε0 = /ε0)[c – (b a)]

Potential VB of the shell B is given by

VB = – σb/ε0 + (1/4πε0)(4πa2σ/b) + σc/ε0

Or, VB = σ/ε0 [c – (b2 a2)/b]

Potential VC of the shell C is given by

VC = σc/ε0 – (1/4πε0)(4πb2σ/c) + (1/4πε0)(4πa2σ/c)

Or, VC = σ/ε0 [c – (b2 a2)/c] = σ/ε0 [c – (b + a)(b a)/c]

Since c = a + b we obtain

VC = σ/ε0 [c – (b a)]

The correct option therefore is VC = VAVB.

(2) Three capacitors each of capacitance C and of breakdown voltage V are joined in series. The capacitance and breakdown voltage of the combination will be

(1) 3 C, V/3

(2) C/3, 3 V

(3) 3 C, 3V

(4) C/3, V/3

This is a very simple question. The effective calacitance Ceff of the combination of three capacitors in series is given by the reciprocal relation,

1/Ceff = 1/C1 +1/C2 +1/C3

Here C1 = C2 = C3 = C so that Ceff = C/3

The breakdown voltage Veff for the series combination is the sum of the individual breakdown voltages:

Veff = 3V

(3) The electric potential at a point (x, y, z) is given by V = − x2y − xz3 + 4. The electric field E at that point is:

(1) E = i 2xy + j (x2 + y2) + k (3xz − y2)

(2) E = i z 3 + j xyz + k z2

(3) E = i (2xy − z3) + j xy2 + k 3z2x

(4) E = i (2xy + z3) + j x2 + k 3xz2

The electric field E is the negative gradient of potential:

E = − V/r = − (i V/∂x + j V/∂y + k V/∂z)

This gives E = i (2xy + z3) + j x2 + k 3xz2 as given in option (4).

You will find similar useful multiple choice questions (with solution) in electrostatics at aphysicsresources and at physicsplus

Tuesday, August 04, 2009

Kerala Medical Entrance (KEAM) 2009 Questions from Electrostatics

Keral Medical Entrance 2009 question paper contained three questions from electrostatics. They are simple except for the first one (given below) which will demand some three dimensional imagination.

(1) The total electric flux through a cube when a charge 8q is placed at one corner of the cube is

(a) ε0 q

(b) ε0 /q

(c) ε0 q

(d) q/ε0

(e) q/ε0

You should remember that the total electric flux originating from a charge q is q/ε0.

[You will definitely remember that the electric field E at a point distant r from a point charge is q/ε0r2. The electric field is equal to the electric flux through unit area held normal to the direction of the field. If you imagine a spherical surface with the charge q at the centre, the surface area of the sphere is 4πr2 and the total flux passing normally through the spherical surface is (q/ε0r2) ×4πr2 = q/ε0]

In the question the charge 8q is placed at one corner of the cube. The total electric flux originating from this charge is 8q/ε0. But only one-eigths of the flux passes through the cube. (You can place seven more cubes with their corners touching the charge to cover the entire volume around the charge).

The electric flux through a cube when a charge 8q is placed at one corner of the cube is therefore (1/8)×(8q/ε0) = q/ε0.

(2) A uniform electric field E exists along positive x-axis. The work done in moving a charge 0.5 C through a distance 2 m along a direction making an angle 60º with x-axis is 10 J. Then the magnitude of electric field is

(a) 5 Vm–1

(b) 2 Vm–1

(c) 5 Vm–1

(d) 40 Vm–1

(e) 20 Vm–1

The force (F) acting on charge q in electric field E is given by F = qE along the direction of the field (along the positive x-axis here). Since the displacement (d) of the charge is inclined at 60º with the x-axis, the work done (W) is given by

W = qEd cos 60

Therefore, 10 = 0.5×E×2×½, from which E = 20 Vm–1.

(3) A capacitor of capacitance C is charged to a potential V. If it carries charge Q, then the energy stored in it is

(a) ½ CV

(b) QV

(c) ½ QV2

(d) CV2

(e) ½ QV

The answer is ½ QV which you can obtain from ½ CV2 which is the form most of you will usually remember:

½ CV2 = ½ CV×V = ½ QV

[The capacitor is charged from zero potential to the potential V. The charge Q is therefore transferred to the capacitor at an average potential of (0+V)/2 = V/2. The work done is therefore QV/2.

To be more rigorous, if the charge on the capacitor at any instant of charging is q and the potential at the instant is v, the work done in transferring an additional charge dq is vdq= (q/C)dq. The total work done in transferring the entire charge Q is 0 Q(q/C)dq = Q2/2C = ½ ×Q×(Q/C) = ½ QV].

You will find more questions (with solution) of various entrance examinations at physicsplus.blogspot.com.

Friday, July 03, 2009

Thermodynamics – Two Multiple Choice Questions

Often simple questions on thermodynamics may cause unexpected confusion. The reason for the confusion is usually the lack of your understanding of the fundamentals. If you don’t have any confusion in respect of the following questions, well and good!

(1) A sample of an ideal gas initially having internal energy U1 and pressure P1 expands adiabatically and performs work W. Heat energy Q is then added to the gas at constant volume so that its pressure is increased to the initial value P1. As a result of the above processes, the internal energy of the gas

(a) decreases by Q W

(b) increases by Q W

(c) decreases by Q

(d) increases by Q

(e) remains unchanged

Since the gas expands adiabatically and outputs mechanical energy, the internal energy of the gas is decreased. [Remember that during adiabatic process there is no heat transfer between the gas and the surroundings]. On adding heat energy to the gas at constant volume the internal energy of the gas is increased. There is no work involved since the volume is constant (isochoric process).

Evidently the internal energy of the gas increases by Q W.

[You will obtain the answer from the mathematical statement of the 1st law of thermodynamics: ∆Q = ∆U + ∆W where ∆Q is the heat energy supplied to the system by the surroundings, ∆W is the work done by the system on the surroundings and ∆U is the increase in the internal energy of the system].

(2) In the given PV diagram, I is the initial state and F is the final state. The gas goes from I to F by (i) IAF (ii) IBF (iii) ICF. The heat absorbed by the gas is

(a) the same in all three processes

(b) the same in (i) and (ii)

(c) greater in (i) than in (ii)

(d) the same in (i) and (iii)

(e) greater in (iii) than in (ii)

This question appeared in Kerala engineering entrance 2009 question paper.

We have ∆Q = ∆U + ∆W

Since the same initial point (I) and the same final point (F) are given for all the three paths, the change in the internal energy (∆U) is the same for all the three processes. During the path IAF the net work done by the gas (∆W) is positive since the work done on the gas during the compression IA (given by the area under the line IA) is less than the work done by the gas during its expansion AF. No work is involved during the process IBF since the volume is constant (isochoric process). During the path ICF the net work done (∆W) by the gas is negative since the work done by the gas during its expansion IC is less than the work done on the gas during its compression CF.

Therefore, the heat absorbed by the gas (∆Q) is greater in (i) than in (ii).

You will find useful multiple choice questions with solution at apphysicsresources as well as at physicsplus.

Tuesday, June 09, 2009

Kerala Medical Entrance (KEAM) 2009 Questions on Optics

Physics questions in the Kerala Medical Entrance 2009 question paper were generally simple compared to those in the Kerala Engineering Entrance 2009 question paper. Today we will discuss the questions on optics included in the Medical Entrance question paper. Here are those three questions:

(1) A ray of light suffers minimum deviation in equilateral prism P. Additional prisms Q and R of identical shape and of same material as that of P are now combined as shown in figure. The ray will now suffer

(a) greater deviation

(b) no deviation

(c) same deviation as before

(d) total internal reflection

(e) smaller deviation

On combining additional prisms Q and R with P, we obtain a portion of an equilateral prism of the same material. Since the incident ray is such that the deviation produced by the prism P is minimum, the refracted ray will be parallel to the base of the prism P and hence it will pass parallel to the base of the combined prism, suffering the same deviation (minimum deviation) as before. The correct option is (c).

(2) When light is scattered by atmospheric atoms and molecules, the amount of scattering of light of wave length 440 nm is A. The amount of scattering for light of wave length 660 nm is

(a) (4/9) A

(b) 2.25 A

(c) 1.5 A

(d) 0.66 A

(e) A/5

The answer for this question is based on Rayleigh’s scattering formula which says that the amount of light scattered is inversely proportional to the fourth power of the wave length of light. Therefore, in the two cases we have respectively,

A α 1/4404 and

x α 1/6604 where x is the amount of scattering for light of wave length 660 nm.

Dividing, A/x = 6604/ 4404 = (3/2)4 = 81/16 = 5 nearly.

Therefore, x = A/5.

(3) In the measurement of the angle of a prism using a spectrometer, the reading of first reflected image are Vernier I: 320° 40' Vernier II: 140° 30' and those of the second reflected image are Vernier I: 80° 38'; Vernier II: 260° 24'. Then the angle of the prism is

(a) 59° 58'

(b) 59° 56'

(c) 60° 2'

(d) 60° 4'

(e) 60° 0'

When a parallel beam of light falls symmetrically on the two faces of the prism, the angle between the rays reflected from these faces is 2A where A is the angle of the prism. If you have a clear understanding of the experimental determination of the angle of the prism using this method, you will definitely be able to find the answer to the above question since you will know that the reading of Vernier I was first inecreased from 320° 40' to 360° on rotating the telescope to view the reflected image from the second face. The 360° mark is the same as 0° mark. So after reaching the zero reading the telescope has rotated through 80° 38'.

The difference between Vernier I readings is (360° - 320° 40') + 80° 38' = 39° 20'+ 80°' = 119° 58'. 38

The difference between Vernier II readings is 260° 24' - 140° 30' = 119° 54'.

The mean of the difference between the readings is 119° 56'.

Therefore, the angle of the prism is (119° 56')/2 = 59° 58'