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X-ray from a tube with a target A of ato...

X-ray from a tube with a target `A` of atomic number `Z` shows strong `K` lines for target `A` and weak`K` lines for impurities. The wavelength og `K_(alpha)` lines is `lambda_(z)` for target `A` and `lambda_(1) and lambda_(2)` for two impurities.
`(lambda_(z))/(lambda_(1)) = 4 and (lambda_(z))/(lambda_(2)) = (1)/(4)`
Assuming the screeining contant of `K_(alpha)` lines to be unity select the correct statement(s).

A

The atomic number of first impurity is `2 z - 1`.

B

The atomic number of first impurity is `2 z + 1`.

C

The atomic number of second impurity is ` ((z + 1))/(2)`.

D

The atomic number of second impurity is ` (z)/(2) + 1`.

Text Solution

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The correct Answer is:
To solve the problem, we will use Moseley's law, which relates the frequency of X-rays emitted by an atom to its atomic number. The law states that the frequency (ν) of the emitted X-rays is proportional to the square of the atomic number (Z) minus a screening constant (b): \[ \nu \propto (Z - b)^2 \] For K-alpha lines, we can assume the screening constant \( b \) is unity, so: \[ \nu \propto (Z - 1)^2 \] We also know that the wavelength (λ) is inversely proportional to the frequency: \[ \nu = \frac{c}{\lambda} \] This means: \[ \frac{1}{\lambda} \propto (Z - 1)^2 \] Thus, we can write: \[ \lambda \propto \frac{1}{(Z - 1)^2} \] ### Step 1: Analyze the given ratios We are given two ratios: 1. \(\frac{\lambda_z}{\lambda_1} = 4\) 2. \(\frac{\lambda_z}{\lambda_2} = \frac{1}{4}\) From these ratios, we can express the wavelengths in terms of \( \lambda_z \): - \( \lambda_1 = \frac{\lambda_z}{4} \) - \( \lambda_2 = 4\lambda_z \) ### Step 2: Set up equations using Moseley's law Using the relationship derived from Moseley's law, we can write: For the target \( A \): \[ \lambda_z \propto \frac{1}{(Z - 1)^2} \] For impurity 1 (with atomic number \( Z_1 \)): \[ \lambda_1 \propto \frac{1}{(Z_1 - 1)^2} \] For impurity 2 (with atomic number \( Z_2 \)): \[ \lambda_2 \propto \frac{1}{(Z_2 - 1)^2} \] ### Step 3: Substitute the wavelengths into the equations Substituting the expressions for \( \lambda_1 \) and \( \lambda_2 \): 1. From \( \lambda_z = 4\lambda_1 \): \[ \frac{1}{(Z - 1)^2} = 4 \cdot \frac{1}{(Z_1 - 1)^2} \] \[ (Z_1 - 1)^2 = 4(Z - 1)^2 \] Taking the square root: \[ Z_1 - 1 = 2(Z - 1) \] \[ Z_1 = 2Z - 1 \] 2. From \( \lambda_z = \frac{1}{4}\lambda_2 \): \[ \frac{1}{(Z - 1)^2} = \frac{1}{4} \cdot \frac{1}{(Z_2 - 1)^2} \] \[ (Z_2 - 1)^2 = 4(Z - 1)^2 \] Taking the square root: \[ Z_2 - 1 = \frac{1}{2}(Z - 1) \] \[ Z_2 = \frac{Z + 1}{2} \] ### Step 4: Final results and options From the calculations, we find: - The atomic number of the first impurity \( Z_1 = 2Z - 1 \) - The atomic number of the second impurity \( Z_2 = \frac{Z + 1}{2} \) Now, we can check the options: - Option A: Atomic number of first impurity is \( 2Z - 1 \) (Correct) - Option B: Atomic number of first impurity is \( 2Z + 1 \) (Incorrect) - Option C: Atomic number of second impurity is \( \frac{Z + 1}{2} \) (Correct) - Option D: Atomic number of second impurity is \( \frac{Z}{2} + 1 \) (Incorrect) ### Conclusion The correct statements are: - Option A: Atomic number of first impurity is \( 2Z - 1 \) - Option C: Atomic number of second impurity is \( \frac{Z + 1}{2} \)

To solve the problem, we will use Moseley's law, which relates the frequency of X-rays emitted by an atom to its atomic number. The law states that the frequency (ν) of the emitted X-rays is proportional to the square of the atomic number (Z) minus a screening constant (b): \[ \nu \propto (Z - b)^2 \] For K-alpha lines, we can assume the screening constant \( b \) is unity, so: \[ \nu \propto (Z - 1)^2 \] ...
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