Question:

For an application where the Reynolds number is to be kept constant, a liquid with a density of 1 g cm\(^-3\) and viscosity of 0.01 Poise results in a characteristic speed of 1 cm s\(^-1\). If this liquid is replaced by another with a density of 1.25 g cm\(^-3\) and viscosity of 0.015 Poise, the characteristic velocity will be ......... cm s\(^-1\) (rounded off to one decimal place).

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When maintaining constant Reynolds number, the characteristic velocity of a fluid is inversely proportional to the viscosity and directly proportional to the density. Use the Reynolds number equation to solve for velocity when changing fluid properties.
Updated On: Jan 30, 2026
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Correct Answer: 1.2

Solution and Explanation

The Reynolds number \( Re \) is a dimensionless quantity that helps predict flow patterns in different fluid flow situations. It is given by the equation: \[ Re = \frac{\rho u L}{\mu} \] Where: - \( \rho \) is the density of the fluid, - \( u \) is the characteristic velocity, - \( L \) is the characteristic length, - \( \mu \) is the dynamic viscosity. In this problem, we are asked to maintain the Reynolds number constant. Since the Reynolds number is constant, we can use a proportionality relationship between the two fluids. Let’s set up the following equation based on the given fluids: \[ \frac{\rho_1 u_1}{\mu_1} = \frac{\rho_2 u_2}{\mu_2} \] Where: - \( \rho_1 = 1 \, {g/cm}^3 \), - \( \mu_1 = 0.01 \, {Poise} \), - \( u_1 = 1 \, {cm/s} \) (characteristic velocity of the first fluid), - \( \rho_2 = 1.25 \, {g/cm}^3 \), - \( \mu_2 = 0.015 \, {Poise} \) (viscosity of the second fluid). Now, solving for the characteristic velocity \( u_2 \) of the second fluid: \[ u_2 = u_1 \frac{\rho_1}{\rho_2} \frac{\mu_2}{\mu_1} \] Substituting the known values: \[ u_2 = 1 \times \frac{1}{1.25} \times \frac{0.015}{0.01} = 1.2 \, {cm/s} \] Thus, the characteristic velocity of the second fluid is \( \mathbf{1.2 \, {cm/s}} \), which is slightly higher than that of the first fluid due to the increased viscosity and density of the second fluid.
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