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In the relation: P=(alpha)/(beta)e^(-(al...

In the relation: `P=(alpha)/(beta)e^(-(alphaZ)/(ktheta)),P` is pressure `Z` is distance `k` is Boltzmann constant and `theta` ils the temperature. The dimensional formula of `beta` will bes

A

`[M^(0)L^(2)T^(0)]`

B

`[M^(1)L^(2)T^(-1)]`

C

`[M^(1)L^(0)T^(-1)]`

D

`[M^(0)L^(2)T^(-1)]`

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To find the dimensional formula of \( \beta \) in the relation \[ P = \frac{\alpha}{\beta} e^{-\frac{\alpha Z}{k \theta}} \] where \( P \) is pressure, \( Z \) is distance, \( k \) is the Boltzmann constant, and \( \theta \) is temperature, we can follow these steps: ### Step 1: Understand the Equation The equation states that pressure \( P \) is equal to \( \frac{\alpha}{\beta} \) multiplied by a dimensionless exponential term. For the entire expression to be dimensionally consistent, \( \frac{\alpha}{\beta} \) must have the same dimensions as pressure \( P \). ### Step 2: Identify the Dimensions of Pressure The dimensional formula for pressure \( P \) is given by: \[ [P] = \frac{\text{Force}}{\text{Area}} = \frac{M L T^{-2}}{L^2} = M L^{-1} T^{-2} \] ### Step 3: Identify the Dimensions of \( \alpha \) To find the dimensions of \( \beta \), we first need to determine the dimensions of \( \alpha \). The term \( e^{-\frac{\alpha Z}{k \theta}} \) is dimensionless, which means that \( \frac{\alpha Z}{k \theta} \) must also be dimensionless. ### Step 4: Write the Dimensions of Each Component - \( Z \) (distance) has dimensions: \( [Z] = L \) - \( k \) (Boltzmann constant) has dimensions: \[ [k] = M L^2 T^{-2} \Theta^{-1} \] where \( \Theta \) represents temperature. - \( \theta \) (temperature) has dimensions: \( [\theta] = \Theta \) ### Step 5: Set Up the Dimensionless Condition Since \( \frac{\alpha Z}{k \theta} \) is dimensionless, we can write: \[ [\alpha] \cdot [Z] = [k] \cdot [\theta] \] Substituting the dimensions we have: \[ [\alpha] \cdot L = (M L^2 T^{-2} \Theta^{-1}) \cdot \Theta \] This simplifies to: \[ [\alpha] \cdot L = M L^2 T^{-2} \] ### Step 6: Solve for the Dimensions of \( \alpha \) Rearranging gives: \[ [\alpha] = \frac{M L^2 T^{-2}}{L} = M L T^{-2} \] ### Step 7: Find the Dimensions of \( \beta \) Now, since \( \frac{\alpha}{\beta} \) must have the same dimensions as pressure \( P \): \[ \frac{[\alpha]}{[\beta]} = [P] \] Substituting the known dimensions: \[ \frac{M L T^{-2}}{[\beta]} = M L^{-1} T^{-2} \] ### Step 8: Solve for \( [\beta] \) Cross-multiplying gives: \[ [\beta] = \frac{M L T^{-2}}{M L^{-1} T^{-2}} = L^2 \] Thus, the dimensional formula for \( \beta \) is: \[ [\beta] = L^2 \] ### Final Answer The dimensional formula of \( \beta \) is \( L^2 \). ---

To find the dimensional formula of \( \beta \) in the relation \[ P = \frac{\alpha}{\beta} e^{-\frac{\alpha Z}{k \theta}} \] where \( P \) is pressure, \( Z \) is distance, \( k \) is the Boltzmann constant, and \( \theta \) is temperature, we can follow these steps: ...
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