Question:

To determine the composition of a bimetallic alloy, a sample is first weighed in air and then in water. These weights are found to be w1w_1 and w2w_2 respectively. If the densities of the two constituent metals are ρ1\rho_1 and ρ2\rho_2 respectively, then the weight of the first metal in the sample is (where ρw\rho_w is the density of water)

Updated On: Jun 17, 2022
  • ρ1ρw(ρ2ρ1)[w1(ρ2ρw)w2ρ2]\frac{\rho_{1}}{\rho_{w}\left(\rho_{2}-\rho_{1}\right)}\left[w_{1}\left(\rho_{2}-\rho_{w}\right)-w_{2}\rho_{2}\right]
  • ρ1ρw(ρ2+ρ1)[w1(ρ2ρw)+w2ρ2]\frac{\rho_{1}}{\rho_{w}\left(\rho_{2}+\rho_{1}\right)}\left[w_{1}\left(\rho_{2}-\rho_{w}\right)+w_{2}\rho_{2}\right]
  • ρ1ρw(ρ2ρ1)[w1(ρ2+ρw)w2ρ1]\frac{\rho_{1}}{\rho_{w}\left(\rho_{2}-\rho_{1}\right)}\left[w_{1}\left(\rho_{2}+\rho_{w}\right)-w_{2}\rho_{1}\right]
  • ρ1ρw(ρ2ρ1)[w1(ρ1+ρw)w2ρ1]\frac{\rho_{1}}{\rho_{w}\left(\rho_{2}-\rho_{1}\right)}\left[w_{1}\left(\rho_{1}+\rho_{w}\right)-w_{2}\rho_{1}\right]
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The Correct Option is A

Solution and Explanation

By Archimedes' Principle
F=vρwgF=v \rho_{w} g
(w1w2)g=vρwg\Rightarrow\left(w_{1}-w_{2}\right) g=v \rho_{w} g
Let, the total volume be vv and first metal weight be xx
w1w2=(v1+v2)ρww_{1}-w_{2}=\left(v_{1}+v_{2}\right) \rho_{w}
w1w2=v1ρw+v2ρw   (v=mρ)w_{1}-w_{2}=v_{1} \rho_{w}+v_{2} \rho_{w} \,\,\,\left(\because v=\frac{m}{\rho}\right)
w1w2=(xρ1ρw+w1xρ2ρw)w_{1}-w_{2}=\left(\frac{x}{\rho_{1}} \rho_{w}+\frac{w_{1}-x}{\rho_{2}} \rho_{w}\right)
w1w2=xρ2ρw+(w1x)ρwρ1ρ1ρ2w_{1}-w_{2}=\frac{x \rho_{2} \rho_{w}+\left(w_{1}-x\right) \rho_{w} \rho_{1}}{\rho_{1} \rho_{2}}
w1ρ1ρ2w2ρ1ρ2=xρ2ρw+w1ρwρ1xρwρ1w_{1}\, \rho_{1} \,\rho_{2}-w_{2} \,\rho_{1}\, \rho_{2}=x \rho_{2} \,\rho_{w}+w_{1} \,\rho_{w} \rho_{1}-x \rho_{w}\, \rho_{1}
x(ρ2ρ1)ρw=ρ1[w1(ρ2ρw)w2ρ2]x\left(\rho_{2}-\rho_{1}\right) \rho_{w}=\rho_{1}\left[w_{1}\left(\rho_{2}-\rho_{w}\right)-w_{2}\, \rho_{2}\right]
x=ρ1ρw(ρ2ρ1)[w1(ρ2ρw)w2ρ2]x=\frac{\rho_{1}}{\rho_{w}\left(\rho_{2}-\rho_{1}\right)}\left[w_{1}\left(\rho_{2}-\rho_{w}\right)-w_{2} \,\rho_{2}\right]
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Concepts Used:

Mechanical Properties of Fluid

The science of the mechanical properties of fluids is called Hydrostatics. A fluid is a substance that relents to the slightest pressure. Fluids are categorized into two classes famed by the names of liquids, and elastic fluids or gases, which later comprehend the air of the atmosphere and all the different kinds of air with which chemistry makes us acquainted.

Streamline Flow:

A streamline is a curve the tangent to which at any point provides the direction of the fluid velocity at that point. It is comparable to a line of force in an electric or magnetic field. In steady flow, the pattern of the streamline is motionless or static with time, and therefore, a streamline provides the actual path of a fluid particle.

Tube of Flow:

A tubular region of fluid enclosed by a boundary comprises streamlines is called a tube of flow. Fluid can never cross the boundaries of a tube of flow and therefore, a tube of flow acts as a pipe of the same shape.

Surface Tension and Viscosity:

The surface tension of a liquid is all the time a function of the solid or fluid with which the liquid is in contact. If a value for surface tension is provided in a table for oil, water, mercury, or whatever, and the contacting fluid is unspecified, it is safe to consider that the contacting fluid is air.