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The intensity of gamma radiation from a ...

The intensity of gamma radiation from a given source is `I`
On passing through `36 mm` of lead , it is reduced to `(1)/(8)` . The thickness of lead which will reduce the intensity to `(1)/(2)` will be

A

6mm

B

9mm

C

18mm

D

12mm

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To solve the problem, we need to determine the thickness of lead that will reduce the intensity of gamma radiation from a given source to half its original value. We are given that the intensity is reduced to \( \frac{1}{8} \) after passing through \( 36 \, \text{mm} \) of lead. ### Step-by-Step Solution: 1. **Understanding the Intensity Reduction**: The intensity of gamma radiation decreases exponentially as it passes through a material. The relationship can be expressed as: \[ I = I_0 e^{-\mu d} \] where: - \( I \) is the final intensity, - \( I_0 \) is the initial intensity, - \( \mu \) is the linear attenuation coefficient, - \( d \) is the thickness of the material. 2. **Setting Up the Equation for Given Conditions**: From the problem, when \( d = 36 \, \text{mm} \), the intensity reduces to \( \frac{1}{8} I_0 \). Thus, we can write: \[ \frac{1}{8} I_0 = I_0 e^{-\mu \cdot 36} \] Dividing both sides by \( I_0 \) (assuming \( I_0 \neq 0 \)): \[ \frac{1}{8} = e^{-\mu \cdot 36} \] 3. **Taking the Natural Logarithm**: Taking the natural logarithm of both sides: \[ \ln\left(\frac{1}{8}\right) = -\mu \cdot 36 \] We know that \( \ln\left(\frac{1}{8}\right) = \ln(8^{-1}) = -\ln(8) \), so: \[ -\ln(8) = -\mu \cdot 36 \] This simplifies to: \[ \mu \cdot 36 = \ln(8) \] 4. **Finding the Thickness for Half Intensity**: Now, we need to find the thickness \( d \) that will reduce the intensity to half, i.e., \( I = \frac{1}{2} I_0 \): \[ \frac{1}{2} I_0 = I_0 e^{-\mu d} \] Dividing by \( I_0 \): \[ \frac{1}{2} = e^{-\mu d} \] Taking the natural logarithm: \[ \ln\left(\frac{1}{2}\right) = -\mu d \] This simplifies to: \[ -\ln(2) = -\mu d \quad \Rightarrow \quad \mu d = \ln(2) \] 5. **Relating the Two Equations**: From the first equation, we have: \[ \mu = \frac{\ln(8)}{36} \] Substituting this into the second equation: \[ \frac{\ln(8)}{36} d = \ln(2) \] 6. **Solving for \( d \)**: Rearranging gives: \[ d = \frac{36 \ln(2)}{\ln(8)} \] Since \( \ln(8) = 3 \ln(2) \): \[ d = \frac{36 \ln(2)}{3 \ln(2)} = \frac{36}{3} = 12 \, \text{mm} \] ### Final Answer: The thickness of lead which will reduce the intensity to \( \frac{1}{2} \) is \( 12 \, \text{mm} \).

To solve the problem, we need to determine the thickness of lead that will reduce the intensity of gamma radiation from a given source to half its original value. We are given that the intensity is reduced to \( \frac{1}{8} \) after passing through \( 36 \, \text{mm} \) of lead. ### Step-by-Step Solution: 1. **Understanding the Intensity Reduction**: The intensity of gamma radiation decreases exponentially as it passes through a material. The relationship can be expressed as: \[ I = I_0 e^{-\mu d} ...
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