An electron travels with a velocity of x `ms^(-1).` For a proton to have the same de-Broglie wavelength, the velocity will be approximately:
A
`(1840)/(x)`
B
`(x)/(1840)`
C
`1840 " x "`
D
x
Text Solution
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The correct Answer is:
To find the velocity of a proton that has the same de-Broglie wavelength as an electron traveling at a velocity of \( x \, \text{ms}^{-1} \), we can follow these steps:
### Step 1: Write the de-Broglie wavelength formula
The de-Broglie wavelength (\( \lambda \)) is given by the formula:
\[
\lambda = \frac{h}{mv}
\]
where \( h \) is Planck's constant, \( m \) is the mass of the particle, and \( v \) is its velocity.
### Step 2: Calculate the de-Broglie wavelength for the electron
For the electron, the de-Broglie wavelength (\( \lambda_e \)) can be expressed as:
\[
\lambda_e = \frac{h}{m_e \cdot x}
\]
where \( m_e \) is the mass of the electron and \( x \) is its velocity.
### Step 3: Write the de-Broglie wavelength for the proton
For the proton, the de-Broglie wavelength (\( \lambda_p \)) is:
\[
\lambda_p = \frac{h}{m_p \cdot v_p}
\]
where \( m_p \) is the mass of the proton and \( v_p \) is its velocity.
### Step 4: Set the wavelengths equal
Since we want the proton to have the same de-Broglie wavelength as the electron, we set \( \lambda_e = \lambda_p \):
\[
\frac{h}{m_e \cdot x} = \frac{h}{m_p \cdot v_p}
\]
### Step 5: Cancel out Planck's constant
We can cancel \( h \) from both sides:
\[
\frac{1}{m_e \cdot x} = \frac{1}{m_p \cdot v_p}
\]
### Step 6: Rearrange the equation
Rearranging gives us:
\[
m_e \cdot x = m_p \cdot v_p
\]
### Step 7: Substitute the mass of the proton
The mass of the proton (\( m_p \)) is approximately 1840 times the mass of the electron (\( m_e \)):
\[
m_e \cdot x = (1840 \cdot m_e) \cdot v_p
\]
### Step 8: Cancel the mass of the electron
Dividing both sides by \( m_e \):
\[
x = 1840 \cdot v_p
\]
### Step 9: Solve for the velocity of the proton
Now, we can solve for \( v_p \):
\[
v_p = \frac{x}{1840}
\]
### Conclusion
Thus, the velocity of the proton to have the same de-Broglie wavelength as the electron is:
\[
v_p \approx \frac{x}{1840}
\]
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