13. A small steel ball of radius r is allowed to fall under gravity through a column of a
viscous liquid of coefficient of viscosity n. After some time, the velocity of the body
attains a constant velocity v. The velocity depends on
(i) weight of the ball mg (ii) coefficient of viscosity n and (iii) radius of ball
r. Determine the relation for velocity, using the method of dimensions.

Answer :

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Answer:

To determine the relation for velocity using the method of dimensions, we'll consider the variables involved: weight of the ball \( mg \), coefficient of viscosity \( n \), and radius of the ball \( r \). We'll express the velocity \( v \) as a function of these variables.

Let's denote:

- \( v \) as velocity

- \( m \) as mass of the ball

- \( g \) as acceleration due to gravity

- \( \eta \) as coefficient of viscosity

- \( r \) as radius of the ball

We can express the velocity \( v \) as a function of these variables using dimensional analysis:

\[ v = k \cdot m^a \cdot g^b \cdot \eta^c \cdot r^d \]

where \( k \) is a dimensionless constant, and \( a, b, c, \) and \( d \) are the exponents to be determined.

Now, let's analyze the dimensions of each variable:

- Dimension of velocity \( [v] = [LT^{-1}] \) (where L represents length, and T represents time)

- Dimension of mass \( [m] = [M] \) (where M represents mass)

- Dimension of acceleration due to gravity \( [g] = [LT^{-2}] \)

- Dimension of coefficient of viscosity \( [\eta] = [ML^{-1}T^{-1}] \)

- Dimension of radius \( [r] = [L] \)

Now, let's substitute these dimensions into the equation:

\[ [LT^{-1}] = k \cdot [M]^a \cdot [LT^{-2}]^b \cdot [ML^{-1}T^{-1}]^c \cdot [L]^d \]

Equating dimensions on both sides, we get:

\[ L^1 T^{-1} = k \cdot M^a \cdot L^{b+c} T^{-2b-c} \]

Now, equating the powers of each dimension, we get:

For length dimension:

\[ 1 = b + c + d \]

For time dimension:

\[ -1 = -2b - c \]

For mass dimension:

\[ 0 = a + c \]

Solving these equations, we find:

\[ b = -\frac{1}{2}, \, c = \frac{1}{2}, \, d = 1 \]

Now, substituting these values back into the equation for velocity:

\[ v = k \cdot m^a \cdot g^b \cdot \eta^c \cdot r^d \]

\[ v = k \cdot m^a \cdot g^{-\frac{1}{2}} \cdot \eta^{\frac{1}{2}} \cdot r \]

As \( g \) is constant and \( a = 0 \) (since velocity does not depend on mass), we can rewrite the equation as:

\[ v = k \cdot \frac{\sqrt{\eta}}{\sqrt{g}} \cdot r \]

This is the relation for velocity in terms of the given variables.

Explanation:

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