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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