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The voltage applied to the Coolidge X-ra...

The voltage applied to the Coolidge X-ray tube is increased by 25%. As a result the short wave limit of continuous X-ray spectrum shifts by `Delta lambda`. The initial voltage applied to the tube is

A

`(hc)/(4e Delta lambda)`

B

`(hc)/(5e Delta lambda)`

C

`(4hc)/(5e Delta lambda)`

D

`(5hc)/(4e Delta lambda)`

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AI Generated Solution

The correct Answer is:
To solve the problem, we need to analyze the relationship between the voltage applied to the Coolidge X-ray tube and the wavelength of the emitted X-rays. The key concept here is that the wavelength of the emitted X-rays is inversely proportional to the voltage applied. ### Step-by-Step Solution: 1. **Understanding the relationship**: The energy of the emitted X-rays is given by the equation: \[ E = \frac{hc}{\lambda} \] where \(E\) is the energy, \(h\) is Planck's constant, \(c\) is the speed of light, and \(\lambda\) is the wavelength. 2. **Relating energy to voltage**: The energy of the X-rays can also be expressed in terms of the voltage \(V\) applied to the tube: \[ E = eV \] where \(e\) is the charge of an electron. 3. **Setting up the equations**: For the initial voltage \(V_1\), we have: \[ \lambda_1 = \frac{hc}{eV_1} \] For the increased voltage \(V_2\), which is 25% more than \(V_1\): \[ V_2 = V_1 + 0.25V_1 = \frac{5}{4}V_1 \] Thus, the wavelength corresponding to \(V_2\) is: \[ \lambda_2 = \frac{hc}{eV_2} = \frac{hc}{e \cdot \frac{5}{4}V_1} = \frac{4hc}{5eV_1} \] 4. **Finding the change in wavelength**: The change in wavelength \(\Delta \lambda\) is given by: \[ \Delta \lambda = \lambda_1 - \lambda_2 \] Substituting the expressions for \(\lambda_1\) and \(\lambda_2\): \[ \Delta \lambda = \frac{hc}{eV_1} - \frac{4hc}{5eV_1} \] Simplifying this expression: \[ \Delta \lambda = \frac{hc}{eV_1} \left(1 - \frac{4}{5}\right) = \frac{hc}{eV_1} \cdot \frac{1}{5} = \frac{hc}{5eV_1} \] 5. **Solving for the initial voltage \(V_1\)**: Rearranging the equation gives: \[ V_1 = \frac{hc}{5e\Delta \lambda} \] ### Final Result: The initial voltage applied to the tube is: \[ V_1 = \frac{hc}{5e\Delta \lambda} \]
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