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

– Thomas A. Edison

Wednesday, September 19, 2007

KEAM (Engineering) 2007 Questions on Elasticity

You will often find questions involving elastic potential energy in entrance examinations for admission to professional and other degree courses. Here is a question which appeared in Kerala Government Engineering Entrance 2007 test paper:

A wire of natural length L, Young’s modulus Y and area of cross section A is extended by x. Then the energy stored in the wire is given by

(a) (YA/2L)x2 (b) (YA/3L)x2 (c) (YL/2A)x2 (d) (YA/2L2)x2 (e) (A/2YL)x2

The elastic potential energy per unit volume is ½ stress×strain. Since the Young’s modulus Y = stress/strain, we can modify the above expression as (½)Y×strain2. The elastic potential energy stored in the entire wire is (½)Y×strain2 × volume of the wire = (½)Y×strain2 × AL = (½)Y×(x/L)2 × AL = (YA/2L)x2.

Here is another question which appeared in Kerala Government Engineering Entrane 2007 test paper:

The length of a rubber cord is l1 metre when the tension is 4N and l2 metre when the tension is 6N. The length when the tension is 9N is

(a) (2.5 l2 1.5 l1) m (b) (6 l2 1.5 l1) m (c) (3 l1 2 l2) m

(d) (3.5 l2 2.5 l1) m (e) (2.5 l2 + 1.5 l1) m

You can use Hooke’s law to solve this question. Since the increase in length is directly proportional to the force (tension) applied, in accordance with Hooke’s law, we have

l2 – l1 = K(6 – 4) where K is the constant of proportionality.

[Note that the increase in length from l1 to l2 is produced by the increase in tension from 4N to 6 N].

If the length of the rubber cord is l3 when the tension is 9 N, we have

l3 – l1 = K (9 – 4)

Dividing the first equation by the second, we obtain

(l2 – l1)/(l3 – l1) = 2/5, from which l3 = (2.5 l2 1.5 l1) metre.

You will find more questions on elasticity on clicking on the label ‘elasticity’ below this post or on the on the side of this page.

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