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If the time period t of the oscillation ...

If the time period t of the oscillation of a drop of liquid of density d, radius r, vibrating under surface tension s is given by the formula `t=sqrt(t^(2b)s^(c)d^(a//2))`. It is observed that the time period is directly proportional to `sqrt((d)/(s)).` The value of b should therefore be:

A

`(3)/(4)`

B

`sqrt3`

C

`(3)/(2)`

D

`(2)/(3)`

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The correct Answer is:
To solve the problem, we need to analyze the given formula for the time period \( t \) of oscillation of a drop of liquid and determine the value of \( b \) based on the proportionality condition provided. ### Step-by-Step Solution: 1. **Understand the Given Formula**: The time period \( t \) is given by the formula: \[ t = \sqrt{r^{2b} s^{c} d^{\frac{a}{2}}} \] where \( r \) is the radius, \( s \) is the surface tension, and \( d \) is the density of the liquid. 2. **Identify the Proportionality Condition**: It is stated that the time period \( t \) is directly proportional to \( \sqrt{\frac{d}{s}} \): \[ t \propto \sqrt{\frac{d}{s}} \] This implies that: \[ t = k \sqrt{\frac{d}{s}} \] for some constant \( k \). 3. **Express the Proportionality in Terms of Dimensions**: From the proportionality, we can express: \[ t = k \sqrt{d} \cdot s^{-\frac{1}{2}} \] 4. **Equate the Two Expressions for Time Period**: Now, we can equate the two expressions for \( t \): \[ \sqrt{r^{2b} s^{c} d^{\frac{a}{2}}} = k \sqrt{d} \cdot s^{-\frac{1}{2}} \] 5. **Square Both Sides**: Squaring both sides gives: \[ r^{2b} s^{c} d^{\frac{a}{2}} = k^2 d \cdot s^{-1} \] 6. **Rearranging the Equation**: Rearranging the equation, we have: \[ r^{2b} s^{c + 1} d^{\frac{a}{2} - 1} = k^2 \] This indicates that the left-hand side must be dimensionless. 7. **Analyzing Dimensions**: We know the dimensions of each term: - Density \( d \): \( [M L^{-3}] \) - Surface tension \( s \): \( [M T^{-2} L^{-1}] \) - Radius \( r \): \( [L] \) We can express the dimensions of \( t \) as: \[ [T] = [L^{b} M^{0} T^{0}] [M^{1} T^{-2} L^{-1}]^{c} [M^{1} L^{-3}]^{\frac{a}{2}} \] 8. **Setting Up the Dimension Equation**: From the equation, we separate the dimensions of mass \( M \), length \( L \), and time \( T \): - For \( M \): \( 0 + c + \frac{a}{2} = 0 \) - For \( L \): \( b - c - \frac{3a}{2} = 0 \) - For \( T \): \( -2c = 1 \) 9. **Solving for \( c \)**: From \( -2c = 1 \), we find: \[ c = -\frac{1}{2} \] 10. **Substituting \( c \) into the Mass Equation**: Substituting \( c \) into the mass equation: \[ 0 - \frac{1}{2} + \frac{a}{2} = 0 \implies a = 1 \] 11. **Substituting \( a \) into the Length Equation**: Now substituting \( a = 1 \) into the length equation: \[ b + \frac{1}{2} - \frac{3}{2} = 0 \implies b = 1 \] ### Final Answer: The value of \( b \) is \( 1 \).
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