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Question: The minimum magnetic dipole moment of an electron in the hydrogen atom is A) \(\dfrac{{eh}}{{2\...

The minimum magnetic dipole moment of an electron in the hydrogen atom is

A) eh2πm\dfrac{{eh}}{{2\pi m}}
B) eh4πm\dfrac{{eh}}{{4\pi m}}
C) ehπm\dfrac{{eh}}{{\pi m}}
D) 00

Explanation

Solution

The electron revolving around the nucleus in an orbit of radius rr generates a current ii and a current carrying loop produces a magnetic dipole moment.

Formula Used:
1. Current ii generated by the revolving electron is given by, i=eTi = \dfrac{e}{T} where ee is the charge of the electron and T=2πωT = \dfrac{{2\pi }}{\omega } is the time period (ω\omega is the angular velocity).
2. Relation between linear velocity vv and angular velocityω\omega with rr as the radius is given by,

v=rωv = r\omega or ω=vr\omega = \dfrac{v}{r} .

3. Magnetic dipole moment is μ=iA\mu = iA ,where ii is the current flowing through a loop of area AA .
Angular momentum of an electron of mass mm moving with a velocity vvalong a circular orbit of radius rr is L=mvrL = mvr .
4. From Bohr’s postulate we have, mvr=nh2πmvr = \dfrac{{nh}}{{2\pi }} , nn is the principal quantum number and hh is the Planck's constant.

Complete step by step answer:
Step1: Sketch a schematic diagram of the electron in the hydrogen atom.

Step 2: Express the relation for the current generated by the revolving electron.

The electron revolving around the nucleus of the hydrogen atom is like the current flowing through a current carrying loop that encompasses an area AA.

So, the current generated by an electron of charge ee revolving around the orbit of radius rrfor a time TTwith angular velocity ω\omega is given by, i=eTi = \dfrac{e}{T} .

 Substitute $T = \dfrac{{2\pi }}{\omega }$ in the above equation to get, $i = \dfrac{{e\omega }}{{2\pi }}$ .  

Substituting for ω=vr\omega = \dfrac{v}{r} in the equation for current, we get i=ev2πri = \dfrac{{ev}}{{2\pi r}} .

Step 3: Express the relation for magnetic dipole moment of the electron in the hydrogen atom.
Magnetic dipole moment μ\mu of a current carrying loop of area AA is given by, μ=iA\mu = iA .

The area of the orbit (or loop) along which the electron revolves is given by, A=πr2A = \pi {r^2}as we assume the orbit to be circular.

Now substitute for i=ev2πri = \dfrac{{ev}}{{2\pi r}} and A=πr2A = \pi {r^2} to obtain the magnetic dipole moment μ\mu .

We have, μ=(ev2πr)πr2\mu = \left( {\dfrac{{ev}}{{2\pi r}}} \right)\pi {r^2} .

Simplifying we get,μ=evr2\mu = \dfrac{{evr}}{2} .

Step 4: Express the magnetic dipole moment μ\mu in terms of the angular momentum L=mvrL = mvr .

Angular momentum of a mass mm moving with a velocity vvalong a circular orbit of radius rr is L=mvrL = mvr .

i.e., vr=Lmvr = \dfrac{L}{m} .

Substituting the above relation in the equation μ\mu we get, μ=e2mL\mu = \dfrac{e}{{2m}}L .

Step 5: Use Bohr’s postulate about angular momentum to obtain the minimum magnetic dipole moment of the electron in the hydrogen atom.

According to Bohr’s atomic model, the angular momentum of the electron orbiting around the nucleus is quantized. The angular momentum of an electron is given by,

L=mvr=nh2πL = mvr = \dfrac{{nh}}{{2\pi }} .

Substitute L=nh2πL = \dfrac{{nh}}{{2\pi }} in the equation μ=e2mL\mu = \dfrac{e}{{2m}}L to obtain,

μ=e2m(nh2π)=neh4πm\mu = \dfrac{e}{{2m}}\left( {\dfrac{{nh}}{{2\pi }}} \right) = \dfrac{{neh}}{{4\pi m}} .

For minimum magnetic dipole moment, n=1n = 1 ,i.e., μ=eh4πm\mu = \dfrac{{eh}}{{4\pi m}} .

Therefore, the correct option is b) eh4πm\dfrac{{eh}}{{4\pi m}} .

Note: : It is important to evaluate the options in which quantities the final answer is expressed and hence then manipulate equations to reach to the final answer in the quantities displayed in the option.