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Question: The ratio of wavelength of deutron and proto accelerated through the same potential difference will ...

The ratio of wavelength of deutron and proto accelerated through the same potential difference will be -

A

12\frac{1}{\sqrt{2}}

B

21\sqrt{\frac{2}{1}}

C

12\frac{1}{2}

D

21\frac{2}{1}

Answer

(1) 12\frac{1}{\sqrt{2}}

Explanation

Solution

The de-Broglie wavelength (λ\lambda) for a charged particle of mass mm and charge qq accelerated through a potential difference VV is given by the formula:

λ=hp\lambda = \frac{h}{p}

where hh is Planck's constant and pp is the momentum of the particle. The kinetic energy (KK) gained by the particle is K=qVK = qV. Also, kinetic energy is related to momentum by K=p22mK = \frac{p^2}{2m}. Equating the two expressions for kinetic energy, we get:

qV=p22mqV = \frac{p^2}{2m}

p2=2mqVp^2 = 2mqV

p=2mqVp = \sqrt{2mqV}

Substituting this into the de-Broglie wavelength formula:

λ=h2mqV\lambda = \frac{h}{\sqrt{2mqV}}

Now, let's apply this formula to a proton (p) and a deuteron (d).

For a proton: Mass of proton (mpm_p) = mm (let's denote it as mm) Charge of proton (qpq_p) = ee (let's denote it as ee) Potential difference (VpV_p) = VV (given as same for both) The de-Broglie wavelength of the proton (λp\lambda_p) is:

λp=h2mpeV\lambda_p = \frac{h}{\sqrt{2m_p e V}}

For a deuteron: A deuteron is the nucleus of deuterium, consisting of one proton and one neutron. Mass of deuteron (mdm_d) \approx mass of proton + mass of neutron. Since the mass of a neutron is approximately equal to the mass of a proton, mdmp+mp=2mpm_d \approx m_p + m_p = 2m_p. Charge of deuteron (qdq_d) = charge of one proton = ee. Potential difference (VdV_d) = VV (given as same for both) The de-Broglie wavelength of the deuteron (λd\lambda_d) is:

λd=h2mdeV\lambda_d = \frac{h}{\sqrt{2m_d e V}}

We need to find the ratio of the wavelength of the deuteron to the proton, i.e., λdλp\frac{\lambda_d}{\lambda_p}.

λdλp=h2mdeVh2mpeV\frac{\lambda_d}{\lambda_p} = \frac{\frac{h}{\sqrt{2m_d e V}}}{\frac{h}{\sqrt{2m_p e V}}}

λdλp=2mpeV2mdeV\frac{\lambda_d}{\lambda_p} = \frac{\sqrt{2m_p e V}}{\sqrt{2m_d e V}}

λdλp=2mpeV2mdeV\frac{\lambda_d}{\lambda_p} = \sqrt{\frac{2m_p e V}{2m_d e V}}

λdλp=mpmd\frac{\lambda_d}{\lambda_p} = \sqrt{\frac{m_p}{m_d}}

Substitute md=2mpm_d = 2m_p:

λdλp=mp2mp\frac{\lambda_d}{\lambda_p} = \sqrt{\frac{m_p}{2m_p}}

λdλp=12\frac{\lambda_d}{\lambda_p} = \sqrt{\frac{1}{2}}

λdλp=12\frac{\lambda_d}{\lambda_p} = \frac{1}{\sqrt{2}}