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Question: Consider an electron in the $n = 3$ orbit of a hydrogen-like atom with atomic number $Z$. At absolut...

Consider an electron in the n=3n = 3 orbit of a hydrogen-like atom with atomic number ZZ. At absolute temperature TT, a neutron having thermal energy kBTk_BT has the same de Broglie wavelength as that of this electron. If this temperature is given by T=Z2h2απ2a02mNkBT = \frac{Z^2h^2}{\alpha \pi^2 a_0^2 m_N k_B}, (where hh is the Planck's constant, kBk_B is the Boltzmann constant, mNm_N is the mass of the neutron and a0a_0 is the first Bohr radius of hydrogen atom) then the value of α\alpha is ______

Answer

72

Explanation

Solution

The de Broglie wavelength of an electron in the nn-th orbit of a hydrogen-like atom with atomic number ZZ is given by λe=2πrnn\lambda_e = \frac{2\pi r_n}{n}, where rnr_n is the radius of the nn-th orbit. The radius of the nn-th orbit is rn=n2a0Zr_n = \frac{n^2 a_0}{Z}, where a0a_0 is the first Bohr radius of hydrogen.

So, the de Broglie wavelength of the electron in the nn-th orbit is λe=2πn(n2a0Z)=2πna0Z\lambda_e = \frac{2\pi}{n} \left(\frac{n^2 a_0}{Z}\right) = \frac{2\pi n a_0}{Z}.

For n=3n=3, the de Broglie wavelength of the electron is λe=2π(3)a0Z=6πa0Z\lambda_e = \frac{2\pi (3) a_0}{Z} = \frac{6\pi a_0}{Z}.

The de Broglie wavelength of a particle with kinetic energy EE is given by λ=hp=h2mE\lambda = \frac{h}{p} = \frac{h}{\sqrt{2mE}}.

The neutron has thermal energy kBTk_BT. So, the kinetic energy of the neutron is EN=kBTE_N = k_BT.

The de Broglie wavelength of the neutron is λN=h2mNkBT\lambda_N = \frac{h}{\sqrt{2 m_N k_B T}}.

According to the problem statement, the de Broglie wavelengths are the same: λe=λN\lambda_e = \lambda_N.

6πa0Z=h2mNkBT\frac{6\pi a_0}{Z} = \frac{h}{\sqrt{2 m_N k_B T}}.

We are given the temperature T=Z2h2απ2a02mNkBT = \frac{Z^2h^2}{\alpha \pi^2 a_0^2 m_N k_B}. Substitute this expression for TT into the equation:

6πa0Z=h2mNkB(Z2h2απ2a02mNkB)\frac{6\pi a_0}{Z} = \frac{h}{\sqrt{2 m_N k_B \left(\frac{Z^2h^2}{\alpha \pi^2 a_0^2 m_N k_B}\right)}}.

The terms mNm_N and kBk_B cancel out in the denominator inside the square root:

6πa0Z=h2Z2h2απ2a02\frac{6\pi a_0}{Z} = \frac{h}{\sqrt{\frac{2 Z^2 h^2}{\alpha \pi^2 a_0^2}}}.

Simplify the square root in the denominator:

2Z2h2απ2a02=2αZ2h2π2a02=2αZhπa0\sqrt{\frac{2 Z^2 h^2}{\alpha \pi^2 a_0^2}} = \sqrt{\frac{2}{\alpha}} \sqrt{\frac{Z^2 h^2}{\pi^2 a_0^2}} = \frac{\sqrt{2}}{\sqrt{\alpha}} \frac{Z h}{\pi a_0}.

So, the equation becomes:

6πa0Z=h2αZhπa0\frac{6\pi a_0}{Z} = \frac{h}{\frac{\sqrt{2}}{\sqrt{\alpha}} \frac{Z h}{\pi a_0}}.

6πa0Z=hαπa02Zh\frac{6\pi a_0}{Z} = \frac{h \sqrt{\alpha} \pi a_0}{\sqrt{2} Z h}.

Cancel hh from the numerator and denominator on the right side:

6πa0Z=απa02Z\frac{6\pi a_0}{Z} = \frac{\sqrt{\alpha} \pi a_0}{\sqrt{2} Z}.

Cancel πa0Z\frac{\pi a_0}{Z} from both sides:

6=α26 = \frac{\sqrt{\alpha}}{\sqrt{2}}.

Multiply both sides by 2\sqrt{2}:

α=62\sqrt{\alpha} = 6\sqrt{2}.

Square both sides to find α\alpha:

α=(62)2=62×(2)2=36×2=72\alpha = (6\sqrt{2})^2 = 6^2 \times (\sqrt{2})^2 = 36 \times 2 = 72.

The value of α\alpha is 72.