An electron beam is acceleration by a potential difference V to hit a metallic target to produce X-rays. It produces continuous as well as characteristic X-rays. If `lambda_(min)` is the smallest possible wavelength of X-rays in the spectrum, the variation of `log lambda_(min)` with `log v` is correctly represented in
An electron beam is acceleration by a potential difference V to hit a metallic target to produce X-rays. It produces continuous as well as characteristic X-rays. If `lambda_(min)` is the smallest possible wavelength of X-rays in the spectrum, the variation of `log lambda_(min)` with `log v` is correctly represented in
A
Option1 Modulation index = 0.8, side frequency bands are at 1180 kHz and 1220 kHz
B
Option2 Modulation index = 0.8, side frequency bands are at 1180 kHz and 1220 kHz
C
Option3 Modulation index = 0.2, side frequency bands are at 1200 kHz and 1180 kHz
D
Option4 Modulation index = 5, side frequency bands are at 21/2 kHz and 18.8 kHz
Text Solution
AI Generated Solution
The correct Answer is:
To solve the problem, we need to analyze the relationship between the minimum wavelength of X-rays produced by an electron beam and the potential difference through which the electrons are accelerated. Let's break down the solution step by step.
### Step-by-Step Solution
1. **Understanding the Energy of the Electron Beam**:
The energy \( E \) of the electrons accelerated through a potential difference \( V \) is given by:
\[
E = eV
\]
where \( e \) is the charge of the electron.
2. **Relating Energy to Wavelength**:
The energy of a photon can also be expressed in terms of its wavelength \( \lambda \) using the equation:
\[
E = \frac{hc}{\lambda}
\]
where \( h \) is Planck's constant and \( c \) is the speed of light.
3. **Finding the Minimum Wavelength**:
The minimum wavelength \( \lambda_{\text{min}} \) corresponds to the maximum energy of the photon produced when the entire kinetic energy of the electron is converted into a photon. Thus, we can equate the two expressions for energy:
\[
eV = \frac{hc}{\lambda_{\text{min}}}
\]
Rearranging this gives:
\[
\lambda_{\text{min}} = \frac{hc}{eV}
\]
4. **Taking Logarithms**:
To analyze the relationship between \( \lambda_{\text{min}} \) and \( V \), we take the logarithm of both sides:
\[
\log \lambda_{\text{min}} = \log \left( \frac{hc}{eV} \right)
\]
This can be expanded using logarithmic properties:
\[
\log \lambda_{\text{min}} = \log(hc) - \log(e) - \log(V)
\]
5. **Rearranging the Equation**:
Rearranging gives:
\[
\log V = \log(hc) - \log(e) - \log \lambda_{\text{min}}
\]
This can be rewritten as:
\[
\log V = -\log \lambda_{\text{min}} + \text{constant}
\]
where the constant includes \( \log(hc) - \log(e) \).
6. **Identifying the Relationship**:
This equation shows that \( \log V \) is linearly related to \( -\log \lambda_{\text{min}} \). It indicates that as \( \lambda_{\text{min}} \) increases, \( V \) decreases, which means the slope is negative.
7. **Graphical Representation**:
When plotting \( \log V \) on the y-axis against \( \log \lambda_{\text{min}} \) on the x-axis, the graph will have a negative slope, indicating an inverse relationship.
### Conclusion
The variation of \( \log \lambda_{\text{min}} \) with \( \log V \) is represented by a straight line with a negative slope.
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