“The world is a dangerous place, not because of those who do evil, but because of those
who look on and do nothing.”
– Albert Einstein
“The world is a dangerous place, not because of those who do evil, but because of those
who look on and do nothing.”
– Albert Einstein
The following question appeared in Kerala Engineering Entrance 2007 question paper:
A simple pendulum is released from A as shown. If m and l represent the mass of the bob and the length of the pendulum, the gain in kinetic energy at B is
(a) mgl/2
(b) mgl/√2
(c) (mgl√3)/2
(d) 2mgl/√3
(e) mgl
From position A, the bob of the pendulum has fallen through a distance l cos 30º (fig.). Therefore, the loss of potential energy is mg l cos 30º = (mgl√3)/2.
Therefore, the gain in kinetic energy by the bob (by the law of conservation of energy) is (mgl√3)/2.
Here is another question which will be useful in the present context:
The bob of a simple pendulum has mass 0.2 kg. The bob is drawn aside so that the string is horizontal and is released. When it swings through 60º its kinetic energy is 0.5 J. The kinetic energy when the sting becomes vertical will be
(a) √3 J
(b) 1/√3 J
(c) √3/2 J
(d) 2/√3 J
(e) 1 J
You can use the figure used with the previous question for working out the present question as well since the angle turned is 60º. The loss of potential energy by the bob on swinging through 60º is mg l cos30º itself. [Or, you may take it as mg l sin60º].
Since the loss of potential energy is equal to the gain of kinetic energy, we have
mg l cos30º = 0.5 J
Or, (mgl√3)/2 = 0.5 J.
The kinetic energy when the string becomes vertical will be mgl since the bob falls through a distance l and loses its entire initial potential energy mgl.
From the above equation mgl = 1/√3 J [Option (b)].
[Note that the mass of the bob given in the question just serves as a distraction].
You will find some useful questions in this section here.
How strange is the lot of we mortals! Each of us is here for a brief sojourn; for what purpose we know not, though sometimes sense it. But we know from daily life that we exist for other people first of all for whose smiles and well-being our own happiness depends.
–Albert Einstein
Three questions from the section ‘work, energy & power’ were included in the AIPMT 2009 question paper. Here are those questions with solution:
(1) A block of mass M is attached to the lower end of a vertical spring. The spring is hung from the ceiling and has force constant value k. The mass is released from rest with the spring initially unstretched. The maximum extension produced in the length of the spring will be:
(1) 2 Mg/k
(2) 4 Mg/k
(3) Mg/2k
(4) Mg/k
If x is the maximum extension produced, we have
Mgx = ½ kx2, on equating the decrease in the gravitational potential energy of the mass M to the increase in the elastic potential energy of the spring.
Therefore, x = 2Mg/k
(2) A body of mass 1 kg is thrown upwards with a velocity 20 m/s. It momentarily comes to rest after attaining a height of 18 m. How much energy is lost due to air friction? (g = 10 ms–2)
(1) 30 J
(2) 40 J
(3) 10 J
(4) 20 J
The initial kinetic energy of the 1 kg mass is given by
½ mv2 = ½ ×1×202 = 200 J.
The gravitational potential energy of the 1 kg mass at its maximum height is given by
Mgh = 1×10×18 = 180 J.
The energy lost due to air friction is therefore equal to 200 – 180 = 20 J.
(3) An engine pumps water continuously through a hose. Water leaves the hose with a velocity v and m is the mass per unit length of the water jet. What is the rate at which kinetic energy is imparted to water?
(1) mv2
(2) ½ mv2
(3) ½ m2v2
(4) ½ mv3
Mas of water flowing out per second through the hose is mv. Therefore, kinetic energy imparted per second to the water is ½ ×(mv)×v2 = ½ mv3 [Option (3)].
Setting an example is not the main means of influencing others; it is the only means.
– Albert Einstein
Let us discuss a few multiple choice questions on work and energy.
(1) A small sphere of mass 20 g is projected vertically up with a velocity of 10 ms–1. If air resistance is negligible, what is the total work done by gravity during the upward trip of the sphere?
(a) 10 J
(b) –10 J
(c) – 1 J
(d) 1 J
(e) 9.8 J
When the sphere rises up its kinetic energy goes on decreasing because of the work done by the gravitational force against the motion of the sphere. (The gravitational potential energy of the sphere goes on increasing by an equal amount). The work done by gravity is evidently negative. When the sphere reaches the maximum height the entire kinetic energy gets converted into gravitational potential energy. The total work done by gravity during the the upward trip of the sphere is numerically equal to the initial kinetic energy (½ mv2) of the sphere but its sign is negative.
Therefore, the answer is – ½ mv2 = – ½ ×0.020×102 = –1 J.
(2) A world class athlete covers a distance of 100 m in 10 s. His kinetic energy can be estimated to be in the range
(a) 2 × 105 J to 5 × 105 J
(b) 2 × 104 J to 5 × 104 J
(c) 2 × 103 J to 5 × 103 J
(d) 200 J to 500 J
(e) 20 J to 50 J
This question has appeared in various entrance tests with slight differences in the wording and in the options. Last year it appeared in the All India Engineering Entrance Examination.
In the 100 m dash the velocity v is almost constant so that we have
v = 100 m/10 s = 10 ms–1
We may take the mass of the athlete to be 70 kg to 80 kg. Let us use 80 kg.
His kinetic energy will be ½ mv2 = ½ ×80×102 = 4000 J so that the correct option is (c).
Questions (3) and (4) appeared in Kerala Engineering Entrance Examination 2008 question paper.
(3) Two bodies A and B have masses 20 kg and 5 kg respectively. Each one is acted upon by a force of 4 kg wt. If they acquire the same kinetic energy in times tA and tB, then the ratio tA/ tB is
(a) ½
(b) 2
(c) 2/5
(d) 5/6
(e) 1/5
The concept of impulse will be very useful here. The impulse received by A and B in the times tA and tB are respectively F tA and F tB where F is the force acting on them (4 kg wt. here). But impulse is the change in momentum so that the momenta acquired by A and B are F tA and F tB.
Since the kinetic energy is p2/2m where p is the momentum, we have
(F tA)2/2mA = (F tB)2/2mB
Therefore, tA/ tB = √( mA/ mB) = √(20/5) = 2.
(4) A particle acted upon by constant forces 4i + j – 3k and 3i + j – k is displaced from the point i + 2j + 3k to the point 5i + 4j + k. The total work done by the forces in SI units is
(a) 20
(b) 40
(c) 50
(d) 30
(e) 35
The resutant force (F) on the particle is the sum of the forces given by
F = (4i + j – 3k) + (3i + j – k) = 7i + 2j – 4k.
The displacement (s) of the particle is given by
s = (5i + 4j + k) – (i + 2j + 3k) = (4i + 2j – 2k)
The work done (W) is given by
W = F.s = (7i + 2j – 4k) . (4i + 2j – 2k) = 28 + 4 + 8 = 40.