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Question: A vertical column 50cm long at \({{50}^{o}}C\) balances \({{100}^{o}}C\) the coefficient of absolute...

A vertical column 50cm long at 50oC{{50}^{o}}C balances 100oC{{100}^{o}}C the coefficient of absolute expansion of the liquid is,
A. 0.005/oC B. 0.0005/oC C. 0.002/oC D. 0.0002/oC \begin{aligned} & A.\text{ }0.005{{/}^{o}}C \\\ & B.\text{ }0.0005{{/}^{o}}C \\\ & C.\text{ }0.002{{/}^{o}}C \\\ & D.\text{ }0.0002{{/}^{o}}C \\\ \end{aligned}

Explanation

Solution

Here in the question it is given that both vertical columns are balancing each other so we can say that their pressure will be equal by using this phenomena we can find the coefficient of absolute expansion of the liquid.

Formula used:
P=ρghP=\rho gh
ρ=ρo1+λT\rho =\dfrac{{{\rho }_{o}}}{1+\lambda T}

Complete step by step solution:
Now it is given that both vertical columns balance each other so we can say that pressure should be equal to both the vertical columns.
If P1 and P2{{P}_{1}}\text{ and }{{P}_{2}} be the pressure of the columns of respectively then,
P1=P2......(1){{P}_{1}}={{P}_{2}}......\left( 1 \right)

Now formula for the pressure is,
P=ρgh.....(2)P=\rho gh.....\left( 2 \right)
Where P = pressure
ρ\rho = gravity
g = acceleration due to gravity
h = height

Now given that,
Height of vertical column is h1=50cm{{h}_{1}}=50cm
Other column is h2=60cm{{h}_{2}}=60cm

Now from the equation (2) we can write equation (1) as
ρ1gh1=ρ2gh2....(3){{\rho }_{1}}g{{h}_{1}}={{\rho }_{2}}g{{h}_{2}}....\left( 3 \right)

Now if the λ\lambda be the coefficient of expansion of liquid then formula for the density for respective column is
ρ1=ρo(1+λT1)......(4) ρ2=ρo(1+λT2)......(5) \begin{aligned} & {{\rho }_{1}}=\dfrac{{{\rho }_{o}}}{\left( 1+\lambda {{T}_{1}} \right)}......\left( 4 \right) \\\ & {{\rho }_{2}}=\dfrac{{{\rho }_{o}}}{\left( 1+\lambda {{T}_{2}} \right)}......\left( 5 \right) \\\ \end{aligned}
Where, ρ\rho = density
ρo{{\rho }_{o}} = density 0oC{{0}^{o}}C
λ\lambda = the coefficient of absolute expansion of liquid.
T = temperature

Now put values of equation (4) and equation (5) into equation (3)
ρo(1+λT1)×g×h1=ρo(1+λT2)×g×h2 h1(1+λT2)=h2(1+λT1) \begin{aligned} & \Rightarrow \dfrac{{{\rho }_{o}}}{\left( 1+\lambda {{T}_{1}} \right)}\times g\times {{h}_{1}}=\dfrac{{{\rho }_{o}}}{\left( 1+\lambda {{T}_{2}} \right)}\times g\times {{h}_{2}} \\\ & \Rightarrow {{h}_{1}}\left( 1+\lambda {{T}_{2}} \right)={{h}_{2}}\left( 1+\lambda {{T}_{1}} \right) \\\ \end{aligned}

Here be careful while putting values,
50(1+λ×100)=60(1+λ×50) 50+5000λ=60+3000λ 5000λ3000λ=6050 2000λ=10 λ=0.005/oC \begin{aligned} & \Rightarrow 50\left( 1+\lambda \times 100 \right)=60\left( 1+\lambda \times 50 \right) \\\ & \Rightarrow 50+5000\lambda =60+3000\lambda \\\ & \Rightarrow 5000\lambda -3000\lambda =60-50 \\\ & \Rightarrow 2000\lambda =10 \\\ & \therefore \lambda =0.005{{/}^{o}}C \\\ \end{aligned}

Additional information:
Definition of The absolute coefficient of expansion,
The absolute coefficient of expansion of liquid is defined as the actual increase in the volume of liquid or we can say the sum of the apparent increase in the volume of liquid in a vessel and increase in the volume of the vessel per unit original volume of liquid per unit rise in temperature.

Note:
When we are putting values of the height and the temperature we have to be careful, because if any value from the given equation is replaced then it will lead us to an incorrect solution.