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When the voltage applied to an X-ray tub...

When the voltage applied to an X-ray tube increased from `V_(1)=15.5kV` to `V_(2)=31kV` the wavelength interval between the `K_(alpha)` line and the cut-off wavelength of te continuous X-ray spectrum increases by a factor of `1.3`. If te atomic number of the element of the target is z. Then the value of `(z)/(13)` will be: (take `hc=1240eVnm` and `R=1xx(10^(7))/(m))`

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To solve the problem, we will follow these steps: ### Step 1: Calculate the cut-off wavelength at V1 The cut-off wavelength (λ2) for the X-ray spectrum can be calculated using the formula: \[ \lambda_2 = \frac{hc}{eV_1} \] Where: - \( h \) is Planck's constant (given as \( hc = 1240 \, \text{eV nm} \)) - \( e \) is the charge of an electron (1 eV = 1.6 x \( 10^{-19} \) J) - \( V_1 = 15.5 \, \text{kV} = 15.5 \times 10^3 \, \text{V} \) Substituting the values: \[ \lambda_2 = \frac{1240 \, \text{eV nm}}{(1.6 \times 10^{-19} \, \text{C})(15.5 \times 10^3 \, \text{V})} \] Calculating this gives: \[ \lambda_2 \approx 0.08 \, \text{nm} \] ### Step 2: Determine the new cut-off wavelength at V2 When the voltage is increased to \( V_2 = 31 \, \text{kV} \), the new cut-off wavelength (λ2') can be calculated as: \[ \lambda_2' = \frac{hc}{eV_2} \] Substituting \( V_2 = 31 \, \text{kV} = 31 \times 10^3 \, \text{V} \): \[ \lambda_2' = \frac{1240 \, \text{eV nm}}{(1.6 \times 10^{-19} \, \text{C})(31 \times 10^3 \, \text{V})} \] Calculating this gives: \[ \lambda_2' \approx 0.04 \, \text{nm} \] ### Step 3: Calculate the change in wavelength The problem states that the wavelength interval between the K-alpha line and the cut-off wavelength increases by a factor of 1.3. Let \( \lambda_1 \) be the wavelength of the K-alpha line. The initial difference is: \[ \Delta \lambda = \lambda_1 - \lambda_2 \] After the voltage increase, the new difference is: \[ \Delta \lambda' = \lambda_1 - \lambda_2' = 1.3 \Delta \lambda \] ### Step 4: Set up the equation From the above, we have: \[ \lambda_1 - \lambda_2' = 1.3(\lambda_1 - \lambda_2) \] Substituting \( \lambda_2' = 0.04 \, \text{nm} \) and \( \lambda_2 = 0.08 \, \text{nm} \): \[ \lambda_1 - 0.04 = 1.3(\lambda_1 - 0.08) \] ### Step 5: Solve for λ1 Expanding the equation: \[ \lambda_1 - 0.04 = 1.3\lambda_1 - 1.04 \] Rearranging gives: \[ 1.3\lambda_1 - \lambda_1 = 1.04 - 0.04 \] \[ 0.3\lambda_1 = 1.0 \] \[ \lambda_1 = \frac{1.0}{0.3} \approx 3.33 \, \text{nm} \] ### Step 6: Relate λ1 to atomic number Z Using the formula for the K-alpha line: \[ \frac{1}{\lambda_1} = R(Z - 1)^2 \] Where \( R = 1 \times 10^7 \, \text{m}^{-1} \) or \( R = 1 \times 10^{9} \, \text{nm}^{-1} \). Substituting \( \lambda_1 \): \[ \frac{1}{3.33} = R(Z - 1)^2 \] Calculating gives: \[ Z - 1 = \sqrt{\frac{1}{3.33 \times 10^9}} \] Calculating \( Z \): \[ Z \approx 26 \] ### Step 7: Calculate \( \frac{Z}{13} \) Finally, we find: \[ \frac{Z}{13} = \frac{26}{13} = 2 \] ### Final Answer Thus, the value of \( \frac{Z}{13} \) is: \[ \boxed{2} \]

To solve the problem, we will follow these steps: ### Step 1: Calculate the cut-off wavelength at V1 The cut-off wavelength (λ2) for the X-ray spectrum can be calculated using the formula: \[ \lambda_2 = \frac{hc}{eV_1} \] Where: ...
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