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An air bubble of radius 1 mm is allowed ...

An air bubble of radius 1 mm is allowed to rise through a long cylindrical column of a viscous liquid of radius 5 cm and travels at a steady rate of 2.1 cm per sec. if the density of the liquid is `1.47(g)/(c c)`. Its viscosity is nearly `(n)/(2)` poise. Then find the value of n. Assume `g=980(cm)/(sec^(2))` and neglect the density of air.

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To solve the problem, we will use the equation for terminal velocity derived from Stokes' law. The terminal velocity \( V \) of a small sphere moving through a viscous fluid is given by: \[ V = \frac{2}{9} \cdot \frac{r^2 \cdot (\rho - \sigma) \cdot g}{\eta} \] Where: - \( r \) = radius of the bubble - \( \rho \) = density of the liquid - \( \sigma \) = density of the bubble (air, which we neglect) - \( g \) = acceleration due to gravity - \( \eta \) = viscosity of the liquid ### Step 1: Identify the given values - Radius of the bubble \( r = 1 \, \text{mm} = 0.1 \, \text{cm} \) - Density of the liquid \( \rho = 1.47 \, \text{g/cm}^3 \) - Density of air \( \sigma \) is neglected - Terminal velocity \( V = 2.1 \, \text{cm/s} \) - Acceleration due to gravity \( g = 980 \, \text{cm/s}^2 \) - Viscosity \( \eta = \frac{n}{2} \, \text{poise} \) ### Step 2: Substitute the known values into the terminal velocity equation Since we are neglecting the density of air, we can simplify the equation: \[ V = \frac{2}{9} \cdot \frac{r^2 \cdot \rho \cdot g}{\eta} \] Substituting the known values: \[ 2.1 = \frac{2}{9} \cdot \frac{(0.1)^2 \cdot (1.47) \cdot (980)}{\frac{n}{2}} \] ### Step 3: Simplify the equation Calculating \( (0.1)^2 \): \[ (0.1)^2 = 0.01 \] Now substituting this back into the equation: \[ 2.1 = \frac{2}{9} \cdot \frac{0.01 \cdot 1.47 \cdot 980}{\frac{n}{2}} \] This can be rewritten as: \[ 2.1 = \frac{2 \cdot 0.01 \cdot 1.47 \cdot 980}{9 \cdot \frac{n}{2}} \] ### Step 4: Cross-multiply to solve for \( n \) Cross-multiplying gives: \[ 2.1 \cdot 9 \cdot \frac{n}{2} = 2 \cdot 0.01 \cdot 1.47 \cdot 980 \] This simplifies to: \[ 18.9 \cdot \frac{n}{2} = 2 \cdot 0.01 \cdot 1.47 \cdot 980 \] Calculating the right side: \[ 2 \cdot 0.01 \cdot 1.47 \cdot 980 = 28.836 \] So we have: \[ 18.9 \cdot \frac{n}{2} = 28.836 \] ### Step 5: Solve for \( n \) Multiply both sides by 2: \[ 18.9n = 57.672 \] Now divide by 18.9: \[ n = \frac{57.672}{18.9} \approx 3.05 \] ### Final Result The value of \( n \) is approximately \( 3 \).

To solve the problem, we will use the equation for terminal velocity derived from Stokes' law. The terminal velocity \( V \) of a small sphere moving through a viscous fluid is given by: \[ V = \frac{2}{9} \cdot \frac{r^2 \cdot (\rho - \sigma) \cdot g}{\eta} \] Where: - \( r \) = radius of the bubble ...
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