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Question: The compensated pendulum of a clock consists of an isosceles triangular frame of base length \[{l_1}...

The compensated pendulum of a clock consists of an isosceles triangular frame of base length l1{l_1} and expansivity α1{\alpha _1} and slides of length l2{l_2} and expansivity α2{\alpha _2}. The pendulum is supported, as shown in Figure. Find the ratio l1l2\dfrac{{{l_1}}}{{{l_2}}} so that the length of the pendulum may remain unchanged at all temperatures.

A. l1l2=2a2a1\dfrac{{{l_1}}}{{{l_2}}} = 2\sqrt {\dfrac{{{a_2}}}{{{a_1}}}}
B. l1l2=a2a1\dfrac{{{l_1}}}{{{l_2}}} = \dfrac{{{a_2}}}{{{a_1}}}
C. l1l2=a22a1\dfrac{{{l_1}}}{{{l_2}}} = \dfrac{{{a_2}}}{{2{a_1}}}
D. l1l2=2a2a1\dfrac{{{l_1}}}{{{l_2}}} = \dfrac{{2{a_2}}}{{{a_1}}}

Explanation

Solution

Three basic thermal expansions are linear expansion, superficial expansion and cubical expansion. Here, in the question we need to determine the ratio l1l2\dfrac{{{l_1}}}{{{l_2}}} so that the length of the pendulum may remain unchanged at all temperatures. For this the amount a material expands or contracts per unit length due to a one-degree change in temperature.

Complete step by step answer:
Let C be the base of the triangle,
Now draw a perpendicular bisector on the side AB from the vertex C

Here cosθ=BMBC=12BMBC=l12l2\cos \theta = \dfrac{{BM}}{{BC}} = \dfrac{{\dfrac{1}{2}BM}}{{BC}} = \dfrac{{{l_1}}}{{2{l_2}}}
Now when the triangle expands,
Let A’B’C be the new triangle and draw a perpendicular AN from A to A’C

Here AA’=x increase in the length of AB=12l1α1t = \dfrac{1}{2}{l_1}{\alpha _1}t, where t is the increase in temperature and
A’N= increase in the length of AB=l2α2t = {l_2}{\alpha _2}t
Since the change in angle after the expansion is very small, hence we can write
BAC=BAC=θ\angle BAC = \angle B'A'C = \theta
Hence
cosθ=ANAA(i)\cos \theta = \dfrac{{A'N}}{{AA'}} - - (i)
Where cosθ=l12l2\cos \theta = \dfrac{{{l_1}}}{{2{l_2}}}
Hence substituting the value in equation (i), we get
l12l2=l2α2t12l1α1t\dfrac{{{l_1}}}{{2{l_2}}} = \dfrac{{{l_2}{\alpha _2}t}}{{\dfrac{1}{2}{l_1}{\alpha _1}t}}
By solving

l12l2=2l2α2l1α1 (l1l2)2=4α2α1 l1l2=4α2α1 =2α2α1  \dfrac{{{l_1}}}{{2{l_2}}} = \dfrac{{2{l_2}{\alpha _2}}}{{{l_1}{\alpha _1}}} \\\ {\left( {\dfrac{{{l_1}}}{{{l_2}}}} \right)^2} = 4\dfrac{{{\alpha _2}}}{{{\alpha _1}}} \\\ \dfrac{{{l_1}}}{{{l_2}}} = \sqrt {4\dfrac{{{\alpha _2}}}{{{\alpha _1}}}} \\\ = 2\sqrt {\dfrac{{{\alpha _2}}}{{{\alpha _1}}}} \\\

Hence the ratio l1l2\dfrac{{{l_1}}}{{{l_2}}}so that the length of the pendulum may remain unchanged at all temperatures =2α2α1= 2\sqrt {\dfrac{{{\alpha _2}}}{{{\alpha _1}}}}

So, the correct answer is “Option A”.

Note:
Expansion corresponds to change in length, area and volume of the substance where linear expansivity is the increase in the length of a substance for per unit length of the substance for one degree Celsius rise in temperature.