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An electron of mass me and a proton of m...

An electron of mass `m_e` and a proton of mass `m_p` are accelerated through the same potential difference. The ratio of the de Broglie wavelength associated with an electron to that associated with proton is

A

1

B

`(m_(p))/(m_(e))`

C

`(m_(e))/(m_(p))`

D

`sqrt((m_(p))/(m_(e))`

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The correct Answer is:
To solve the problem of finding the ratio of the de Broglie wavelength associated with an electron to that associated with a proton when both are accelerated through the same potential difference, we can follow these steps: ### Step 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. The momentum \( p \) can also be expressed in terms of mass (\( m \)) and velocity (\( v \)): \[ p = mv \] Thus, the de Broglie wavelength can be rewritten as: \[ \lambda = \frac{h}{mv} \] ### Step 2: Calculate the kinetic energy of the particles When a charged particle is accelerated through a potential difference \( V \), its kinetic energy (\( KE \)) is given by: \[ KE = qV \] where \( q \) is the charge of the particle. For an electron and a proton, the charge \( q \) is the elementary charge \( e \). ### Step 3: Relate kinetic energy to velocity The kinetic energy can also be expressed in terms of mass and velocity: \[ KE = \frac{1}{2} mv^2 \] Setting the two expressions for kinetic energy equal gives: \[ qV = \frac{1}{2} mv^2 \] From this, we can solve for \( v \): \[ v = \sqrt{\frac{2qV}{m}} \] ### Step 4: Substitute velocity into the de Broglie wavelength formula Now, we can substitute the expression for \( v \) back into the de Broglie wavelength formula: \[ \lambda = \frac{h}{m \sqrt{\frac{2qV}{m}}} = \frac{h}{\sqrt{2mqV}} \] ### Step 5: Calculate the de Broglie wavelengths for the electron and proton For the electron: \[ \lambda_e = \frac{h}{\sqrt{2m_e e V}} \] For the proton: \[ \lambda_p = \frac{h}{\sqrt{2m_p e V}} \] ### Step 6: Find the ratio of the de Broglie wavelengths Now, we can find the ratio of the de Broglie wavelengths of the electron to that of the proton: \[ \frac{\lambda_e}{\lambda_p} = \frac{\frac{h}{\sqrt{2m_e e V}}}{\frac{h}{\sqrt{2m_p e V}}} = \frac{\sqrt{2m_p e V}}{\sqrt{2m_e e V}} = \sqrt{\frac{m_p}{m_e}} \] ### Final Result Thus, the ratio of the de Broglie wavelength associated with the electron to that associated with the proton is: \[ \frac{\lambda_e}{\lambda_p} = \sqrt{\frac{m_p}{m_e}} \]

To solve the problem of finding the ratio of the de Broglie wavelength associated with an electron to that associated with a proton when both are accelerated through the same potential difference, we can follow these steps: ### Step 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. The momentum \( p \) can also be expressed in terms of mass (\( m \)) and velocity (\( v \)): ...
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