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Question: A rectangular tube of uniform cross section has three liquids of densities \({{\rho }_{1}}\),\({{\rh...

A rectangular tube of uniform cross section has three liquids of densities ρ1{{\rho }_{1}},ρ2{{\rho }_{2}} and ρ3{{\rho }_{3}}. Each liquid column has length of sides of the equilateral triangle. Find the length x of the liquid of density ρ1{{\rho }_{1}} in the horizontal limb of the tube, if the triangular tube is kept in the vertical plane.

Explanation

Solution

The length of the tubes and the cross section are uniform so, the pressure at one end of the tube is equal to the other end at the base, so by equating pressure of both left and right side and by putting all the values of length, height of different liquids we will calculate our required answer.
Formula used:
Pressure P due to liquid is given by,
P=ρgh\Rightarrow P=\rho gh

Complete answer: :
When a liquid is placed in a column with some height at equilibrium it exerts a pressure due to force of gravity which is known as hydrostatic force.
The initial diagram according to the above problem statement is given by,

Now, by measuring heights and assuming length of liquid of density ρ1{{\rho }_{1}} at base be x and length of side of triangle be ll so,

Given, P1 =ρ1{{\rho }_{1}}(density of liquid one), P2=ρ2{{\rho }_{2}}(density of liquid two) and P3=ρ3{{\rho }_{3}} (density of liquid three) from the above diagram,
Now, pressure at point A will be,
P=ρgh\Rightarrow P=\rho gh
PA=ρ1gh1+ρ2gh2\Rightarrow {{P}_{A}}={{\rho }_{1}}g{{h}_{1}}+{{\rho }_{2}}g{{h}_{2}}
h1=xcos30\Rightarrow {{h}_{1}}=x\cos {{30}^{\circ }}
h2=(lx)cos30\Rightarrow {{h}_{2}}=(l-x)\cos {{30}^{\circ }}
PA=ρ1g(lx)cos30+ρ2gxcos30.......(1)\Rightarrow {{P}_{A}}={{\rho }_{1}}g(l-x)\cos {{30}^{\circ }}+{{\rho }_{2}}gx\cos {{30}^{\circ }}.......(1)
Similarly for pressure at point B will be,
PB=ρ2gh3+ρ3gh4\Rightarrow {{P}_{B}}={{\rho }_{2}}g{{h}_{3}}+{{\rho }_{3}}g{{h}_{4}}
h3=(lx)cos30\Rightarrow {{h}_{3}}=(l-x)\cos {{30}^{\circ }}
h4=xcos30\Rightarrow {{h}_{4}}=x\cos {{30}^{\circ }}
PB=ρ2g(lx)cos30+ρ3gxcos30........(2)\Rightarrow {{P}_{B}}={{\rho }_{2}}g(l-x)\cos {{30}^{\circ }}+{{\rho }_{3}}gx\cos {{30}^{\circ }}........(2)
Now by equating equation (1) and (2), we have
ρ1g(lx)cos30+ρ2gxcos30=ρ2g(lx)cos30+ρ3gxcos30\Rightarrow {{\rho }_{1}}g(l-x)\cos {{30}^{\circ }}+{{\rho }_{2}}gx\cos {{30}^{\circ }}={{\rho }_{2}}g(l-x)\cos {{30}^{\circ }}+{{\rho }_{3}}gx\cos {{30}^{\circ }}
Value of g and cos30\cos {{30}^{\circ }}will be cancel out from both side and the remaining equation is given by,
ρ1(lx)+ρ2x=ρ2(lx)+ρ3x\Rightarrow {{\rho }_{1}}(l-x)+{{\rho }_{2}}x={{\rho }_{2}}(l-x)+{{\rho }_{3}}x
xρ2xρ1+xρ2xρ3=lρ2lρ1\Rightarrow x{{\rho }_{2}}-x{{\rho }_{1}}+x{{\rho }_{2}}-x{{\rho }_{3}}=l{{\rho }_{2}}-l{{\rho }_{1}}
x(ρ2ρ1+ρ2ρ3)=l(ρ2ρ1)\Rightarrow x({{\rho }_{2}}-{{\rho }_{1}}+{{\rho }_{2}}-{{\rho }_{3}})=l({{\rho }_{2}}-{{\rho }_{1}})
x=l(ρ2ρ1)(2ρ2ρ1+ρ3)\Rightarrow x=\dfrac{l({{\rho }_{2}}-{{\rho }_{1}})}{(2{{\rho }_{2}}-{{\rho }_{1}}+-{{\rho }_{3}})}
\therefore The length of liquid of density ρ1{{\rho }_{1}}at the base of the equilateral triangular tube will be given by,
x=l(ρ2ρ1)(2ρ2ρ1+ρ3)\Rightarrow x=\dfrac{l({{\rho }_{2}}-{{\rho }_{1}})}{(2{{\rho }_{2}}-{{\rho }_{1}}+-{{\rho }_{3}})}

Note:
The pressure acting on a layer of fluid in bottom is directly proportional to the product of height and density of fluid and this pressure is mainly caused due to force of gravity. When density or height of fluid increases the pressure exerted at the bottom will increase. While increase in temperature of liquid will cause the molecules to separate and liquid will expand and density of liquid will decrease by which pressure exerted at bottom will decrease.