2:1
1:1
The de-Broglie wavelength (\( \lambda \)) of a particle is given by the equation:
\[ \lambda = \frac{h}{p} \]
Where: - \( h \) is Planck's constant, - \( p \) is the momentum of the particle.
We are given that the momentum of the α-particle is half that of the proton. Let's denote the momentum of the proton as \( p_{\text{proton}} \) and the momentum of the α-particle as \( p_{\alpha} = \frac{1}{2} p_{\text{proton}} \).
The de-Broglie wavelength for the proton is:
\[ \lambda_{\text{proton}} = \frac{h}{p_{\text{proton}}} \]
The de-Broglie wavelength for the α-particle is:
\[ \lambda_{\alpha} = \frac{h}{p_{\alpha}} = \frac{h}{\frac{1}{2} p_{\text{proton}}} = \frac{2h}{p_{\text{proton}}} \]
Thus, the ratio of the wavelengths of the de-Broglie waves of the α-particle and the proton is:
\[ \frac{\lambda_{\alpha}}{\lambda_{\text{proton}}} = \frac{\frac{2h}{p_{\text{proton}}}}{\frac{h}{p_{\text{proton}}}} = 2 \]
Correct Answer: (D) 2:1
Given:
Momentum of α-particle = \( \frac{1}{2} \) × momentum of proton
Step 1: Use de-Broglie wavelength formula: \[ \lambda = \frac{h}{p} \] where \( h \) is Planck’s constant and \( p \) is momentum.
Let \( p_p \) be momentum of proton and \( p_\alpha = \frac{1}{2}p_p \) Then the wavelengths are: \[ \lambda_p = \frac{h}{p_p}, \quad \lambda_\alpha = \frac{h}{p_\alpha} = \frac{h}{\frac{1}{2}p_p} = \frac{2h}{p_p} \]
Step 2: Take the ratio: \[ \frac{\lambda_\alpha}{\lambda_p} = \frac{2h/p_p}{h/p_p} = 2 \Rightarrow \lambda_\alpha : \lambda_p = 2 : 1 \]
Final Answer: \( \boxed{2:1} \)
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