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An alpha particle and a proton are accelerated from rest by a potential difference of 200 V. After this, their de Broglie wavelengths are `lambda_(alpha)` and `lambda_(p)` respectively. The ratio `(lambda_(p))/(lambda_(alpha))` is :

A

`3.8`

B

8

C

`7.8`

D

`2.8`

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The correct Answer is:
To find the ratio of the de Broglie wavelengths of an alpha particle and a proton after being accelerated through a potential difference of 200 V, we can follow these steps: ### Step 1: Understand the relationship between kinetic energy and potential difference When a charged particle is accelerated through a potential difference \( V \), the kinetic energy \( K \) gained by the particle is given by: \[ K = qV \] where \( q \) is the charge of the particle. ### Step 2: Determine the charges of the particles - The charge of a proton \( q_p = e \) (where \( e \) is the elementary charge). - The charge of an alpha particle \( q_{\alpha} = 2e \) (since it consists of 2 protons and 2 neutrons). ### Step 3: Calculate the kinetic energies Using the potential difference of 200 V: - For the proton: \[ K_p = q_p V = e \cdot 200 = 200e \text{ Joules} \] - For the alpha particle: \[ K_{\alpha} = q_{\alpha} V = 2e \cdot 200 = 400e \text{ Joules} \] ### Step 4: Relate kinetic energy to momentum The kinetic energy can also be expressed in terms of momentum \( p \): \[ K = \frac{p^2}{2m} \] From this, we can express momentum as: \[ p = \sqrt{2mK} \] ### Step 5: Calculate the momenta of the particles - For the proton: \[ p_p = \sqrt{2m_p K_p} = \sqrt{2m_p \cdot 200e} \] - For the alpha particle: \[ p_{\alpha} = \sqrt{2m_{\alpha} K_{\alpha}} = \sqrt{2m_{\alpha} \cdot 400e} \] ### Step 6: Calculate the de Broglie wavelengths The de Broglie wavelength \( \lambda \) is given by: \[ \lambda = \frac{h}{p} \] where \( h \) is Planck's constant. - For the proton: \[ \lambda_p = \frac{h}{p_p} = \frac{h}{\sqrt{2m_p \cdot 200e}} \] - For the alpha particle: \[ \lambda_{\alpha} = \frac{h}{p_{\alpha}} = \frac{h}{\sqrt{2m_{\alpha} \cdot 400e}} \] ### Step 7: Find the ratio of the wavelengths Now, we can find the ratio \( \frac{\lambda_p}{\lambda_{\alpha}} \): \[ \frac{\lambda_p}{\lambda_{\alpha}} = \frac{\frac{h}{\sqrt{2m_p \cdot 200e}}}{\frac{h}{\sqrt{2m_{\alpha} \cdot 400e}}} = \frac{\sqrt{2m_{\alpha} \cdot 400e}}{\sqrt{2m_p \cdot 200e}} \] This simplifies to: \[ \frac{\lambda_p}{\lambda_{\alpha}} = \frac{\sqrt{m_{\alpha} \cdot 400}}{\sqrt{m_p \cdot 200}} = \sqrt{\frac{m_{\alpha} \cdot 400}{m_p \cdot 200}} = \sqrt{2 \cdot \frac{m_{\alpha}}{m_p}} \] ### Step 8: Substitute the masses The mass of an alpha particle \( m_{\alpha} \) is approximately 4 times the mass of a proton \( m_p \): \[ \frac{m_{\alpha}}{m_p} \approx 4 \] Thus: \[ \frac{\lambda_p}{\lambda_{\alpha}} = \sqrt{2 \cdot 4} = \sqrt{8} = 2\sqrt{2} \] ### Final Answer The ratio \( \frac{\lambda_p}{\lambda_{\alpha}} \) is: \[ \frac{\lambda_p}{\lambda_{\alpha}} = 2\sqrt{2} \]
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