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Characteristic X-rays of frequency 4.2x...

Characteristic X-rays of frequency `4.2xx10^18` Hz are produced when transitions from L-shell to K-shell take place in a cartain target meterial. Use Mosley's law to determine the atoic number of the target matderial. Given Rydberg constant `R =1.1xx10^7 m^(-1)`.

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To determine the atomic number of the target material using Moseley's law, we can follow these steps: ### Step 1: Understand Moseley's Law Moseley's law states that the frequency of the X-rays emitted during electronic transitions can be expressed as: \[ \frac{1}{\lambda} = R \cdot (Z - 1)^2 \cdot \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \] Where: - \( \lambda \) is the wavelength of the emitted X-rays, - \( R \) is the Rydberg constant, - \( Z \) is the atomic number, - \( n_1 \) and \( n_2 \) are the principal quantum numbers of the initial and final energy levels. ### Step 2: Determine the Values In this case: - The frequency \( f = 4.2 \times 10^{18} \) Hz, - The Rydberg constant \( R = 1.1 \times 10^7 \, m^{-1} \), - The transition is from the L-shell (n=2) to the K-shell (n=1), so \( n_1 = 1 \) and \( n_2 = 2 \). ### Step 3: Convert Frequency to Wavelength Using the relationship between frequency and wavelength: \[ \lambda = \frac{c}{f} \] where \( c \) (the speed of light) is approximately \( 3 \times 10^8 \, m/s \). Calculating \( \lambda \): \[ \lambda = \frac{3 \times 10^8 \, m/s}{4.2 \times 10^{18} \, Hz} = \frac{3}{4.2} \times 10^{-10} \, m = 0.714 \times 10^{-10} \, m = 7.14 \times 10^{-11} \, m \] ### Step 4: Substitute into Moseley's Law Now we substitute \( \lambda \) into Moseley's law: \[ \frac{1}{\lambda} = R \cdot (Z - 1)^2 \cdot \left( \frac{1}{1^2} - \frac{1}{2^2} \right) \] Calculating \( \frac{1}{\lambda} \): \[ \frac{1}{\lambda} = \frac{1}{7.14 \times 10^{-11}} \approx 1.4 \times 10^{10} \, m^{-1} \] Now substituting into the equation: \[ 1.4 \times 10^{10} = 1.1 \times 10^7 \cdot (Z - 1)^2 \cdot \left( 1 - \frac{1}{4} \right) \] \[ 1.4 \times 10^{10} = 1.1 \times 10^7 \cdot (Z - 1)^2 \cdot \frac{3}{4} \] ### Step 5: Solve for \( Z \) Rearranging the equation: \[ (Z - 1)^2 = \frac{1.4 \times 10^{10}}{1.1 \times 10^7 \cdot \frac{3}{4}} \] Calculating the right side: \[ (Z - 1)^2 = \frac{1.4 \times 10^{10}}{8.25 \times 10^6} \approx 1.696 \times 10^3 \] Taking the square root: \[ Z - 1 \approx \sqrt{1.696 \times 10^3} \approx 41.2 \] Thus, \[ Z \approx 42.2 \] Since \( Z \) must be an integer, we round it to: \[ Z = 42 \] ### Final Answer The atomic number of the target material is \( Z = 42 \). ---

To determine the atomic number of the target material using Moseley's law, we can follow these steps: ### Step 1: Understand Moseley's Law Moseley's law states that the frequency of the X-rays emitted during electronic transitions can be expressed as: \[ \frac{1}{\lambda} = R \cdot (Z - 1)^2 \cdot \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right) \] Where: ...
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