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An electron is accelerated through a pot...

An electron is accelerated through a potential difference of V volt. It has a wavelength `lamda` associated must be accelerated so that its de Broglie wavelength is the same as the of a proton? Take mass of proton to be 1837 times larger than the mass of electron.

A

V volt

B

1837V volt

C

`(V)/(1837)` volt

D

`sqrt(1837) V` volt

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The correct Answer is:
To solve the problem, we need to find the potential difference \( V_p \) through which a proton must be accelerated so that its de Broglie wavelength is the same as that of an electron accelerated through a potential difference \( V \). ### Step-by-step Solution: 1. **Understand the de Broglie Wavelength Formula**: The de Broglie wavelength \( \lambda \) of a particle is given by the formula: \[ \lambda = \frac{h}{p} \] where \( h \) is Planck's constant and \( p \) is the momentum of the particle. 2. **Relate Momentum to Kinetic Energy**: The momentum \( p \) can be expressed in terms of kinetic energy \( KE \): \[ p = \sqrt{2m \cdot KE} \] For a charged particle accelerated through a potential difference \( V \), the kinetic energy is given by: \[ KE = qV \] where \( q \) is the charge of the particle. 3. **Write the de Broglie Wavelength for Electron**: For the electron, we have: \[ \lambda_e = \frac{h}{\sqrt{2m_e \cdot eV}} \] where \( m_e \) is the mass of the electron and \( e \) is the charge of the electron. 4. **Write the de Broglie Wavelength for Proton**: For the proton, we have: \[ \lambda_p = \frac{h}{\sqrt{2m_p \cdot eV_p}} \] where \( m_p \) is the mass of the proton and \( V_p \) is the potential difference through which the proton is accelerated. 5. **Set the Wavelengths Equal**: Since the de Broglie wavelengths are the same: \[ \lambda_e = \lambda_p \] Substituting the expressions for \( \lambda_e \) and \( \lambda_p \): \[ \frac{h}{\sqrt{2m_e \cdot eV}} = \frac{h}{\sqrt{2m_p \cdot eV_p}} \] 6. **Cancel \( h \) and Rearrange**: Canceling \( h \) from both sides and squaring gives: \[ \frac{1}{2m_e \cdot eV} = \frac{1}{2m_p \cdot eV_p} \] Rearranging this yields: \[ m_p \cdot eV_p = m_e \cdot eV \] 7. **Substitute the Mass of Proton**: Given that the mass of the proton \( m_p \) is 1837 times the mass of the electron \( m_e \): \[ 1837m_e \cdot V_p = m_e \cdot V \] 8. **Solve for \( V_p \)**: Dividing both sides by \( m_e \): \[ 1837V_p = V \] Thus, \[ V_p = \frac{V}{1837} \] ### Final Answer: The potential difference \( V_p \) through which the proton must be accelerated is: \[ V_p = \frac{V}{1837} \]

To solve the problem, we need to find the potential difference \( V_p \) through which a proton must be accelerated so that its de Broglie wavelength is the same as that of an electron accelerated through a potential difference \( V \). ### Step-by-step Solution: 1. **Understand the de Broglie Wavelength Formula**: The de Broglie wavelength \( \lambda \) of a particle is given by the formula: \[ \lambda = \frac{h}{p} ...
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