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The intensity of X–rays of wavelength 0....

The intensity of X–rays of wavelength 0.5Å reduces to one fourth on passing through 3.5 mm. Thickness of a metal foil. The coefficient of absorption of metal will be–

A

`0.2 mm^(-1)`

B

`0.4 mm^(-1)`

C

`0.6 mm^(-1)`

D

`0.8mm^(-1)`

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The correct Answer is:
To find the coefficient of absorption (μ) of the metal foil, we can use the formula related to the intensity of X-rays passing through a material: \[ I = I_0 e^{-\mu x} \] Where: - \( I \) is the final intensity after passing through the material, - \( I_0 \) is the initial intensity, - \( \mu \) is the coefficient of absorption, - \( x \) is the thickness of the material. Given that the intensity of X-rays reduces to one fourth, we can express this as: \[ I = \frac{I_0}{4} \] Now, substituting this into the equation: \[ \frac{I_0}{4} = I_0 e^{-\mu x} \] Dividing both sides by \( I_0 \): \[ \frac{1}{4} = e^{-\mu x} \] Taking the natural logarithm of both sides: \[ \ln\left(\frac{1}{4}\right) = -\mu x \] We can rewrite \( \frac{1}{4} \) as \( 4^{-1} \): \[ \ln(4^{-1}) = -\mu x \] Using the property of logarithms: \[ -\ln(4) = -\mu x \] Thus: \[ \mu x = \ln(4) \] Now, substituting \( x = 3.5 \, \text{mm} \): \[ \mu \cdot 3.5 = \ln(4) \] Now, we know that \( \ln(4) = 2 \ln(2) \). The value of \( \ln(2) \) is approximately \( 0.693 \): \[ \ln(4) = 2 \cdot 0.693 = 1.386 \] So we have: \[ \mu \cdot 3.5 = 1.386 \] Now, solving for \( \mu \): \[ \mu = \frac{1.386}{3.5} \] Calculating this gives: \[ \mu \approx 0.396 \, \text{mm}^{-1} \] Thus, the coefficient of absorption of the metal is approximately \( 0.396 \, \text{mm}^{-1} \). ### Final Answer: The coefficient of absorption of the metal is \( 0.396 \, \text{mm}^{-1} \). ---
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