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Question: At a given place, a mercury barometer records a pressure of \(0.70\) m of Hg. What would be the heig...

At a given place, a mercury barometer records a pressure of 0.700.70 m of Hg. What would be the height of the water column if mercury in the barometer is replaced by water? Take the density of mercury to be 13.6×103kgm313.6 \times {10^3}\,kg\,{m^{ - 3}} .

Explanation

Solution

Barometer is a device which is used to record the pressure. Pressure exerted on any substance is given as ρgh\rho gh here, ρ\rho is the density of the substance used to record the pressure, gg is the acceleration due to gravity and hh is the height up to which the substance rises also known as barometric height.

Complete step by step solution: Barometer is used in the weather forecast to show the short term changes in the water.
The density of mercury is 13.613.6 times the density of water.
Let ρm{\rho _m} be the density of mercury,
The density of water is ρw{\rho _w} .
The barometric height of the mercury be hm{h_m}
Let the barometric height of the water column in the barometer be hw{h_w} .
The acceleration due to gravity is gg .
As pressure PP is given as:
P=ρghP = \rho gh
Therefore, for mercury the pressure will be given as:
P=ρmghmP = {\rho _m}g{h_m} --equation 11
Now, when the mercury is replaced by water the pressure remains the same but the barometric height changes. Thus, we can have the pressure as:
P=ρwghwP = {\rho _w}g{h_w} -- equation 22
As the pressure remains same, thus from equation 11 and equation 22 we have
ρwghw=ρmghm{\rho _w}g{h_w} = {\rho _m}g{h_m}
hw=ρmhmρw\Rightarrow {h_w} = \dfrac{{{\rho _m}{h_m}}}{{{\rho _w}}}
As, ρm=13.6×ρw{\rho _m} = 13.6 \times {\rho _w} , thus we have:
hw=(13.6ρw)hmρw{h_w} = \dfrac{{\left( {13.6{\rho _w}} \right){h_m}}}{{{\rho _w}}}
hw=(13.6)hm\Rightarrow {h_w} = \left( {13.6} \right){h_m}
We are given that hm=0.70m{h_m} = 0.70m , substituting this value, we get:
hm=13.6×0.70{h_m} = 13.6 \times 0.70
hm=9.52\Rightarrow {h_m} = 9.52

The height of the water column is 9.52m9.52m .

Note: The atmospheric pressure remains the same irrespective of the substance filled in the barometer as a result the substance rises to a height which is inversely proportional to its density. The density of mercury is 13.613.6 times the density of water. As a result, the rise in barometric height of water is also 13.613.6 times the rise in mercury.