If the electron were a classical solid sphere, with radius

rc=e24πO0˙mc2

(the so-called classical electron radius, obtained by assuming the electron's mass is attributable to energy stored in its electric field, via the Einstein formula E=mc2), and its angular momentum is (1/2)h then how fast (in m/sm/s) would a point on the "equator" be moving? Does this model make sense? (Actually, the radius of the electron is known experimentally to be much less than5.156×1010m/src, but this only makes matters worse).

Short Answer

Expert verified

The speed is ϑ=5.156×1010m/s. The quantum spin is totally different from the classical spin.

Step by step solution

01

Definition of quantum spin.

In practise, spin is computed as a dimensionless spin quantum number by dividing the spin angular momentum by the decreased Planck constant, which has the same dimensions as angular momentum.

02

Find the quantum spin

Angular momentum is L=.

where Iis the moment of inertia, and for a sphere, it is equal to 2/5mr2

role="math" localid="1655966871442" ωis the angular velocity, and it is equal to the linear velocity divided by the radius of the path J/r.

L=25mr2vr=25mrgr=re=e24πo0mc2andL=h/2h2=25me24πo0mc2θh=e-t5πo0C2

Thus, the expression of Plank’s constant is obtained.

03

Substitute the value of each one of constants

In this step substitute the given values in the expression of velocity,

ϑ=5πho'c2e2=5π1.055×10-348.85×10-123×10821.6×10-192=5.156×1010m/s.

If the quantum spin were the same as the classical spin, one of the postulates of special relativity would be violated (i.e.,ϑ>C), which couldn't be true because nothing could move faster than the speed of light, hence the quantum spin must be something altogether different.

As nothing can travel faster than the speed of light, quantum spin is distinct from classical spin.

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Most popular questions from this chapter

(a) Construct the wave function for hydrogen in the state n=4,I=3,m=3. Express your answer as a function of the spherical coordinates r,θandϕ.

(b) Find the expectation value of role="math" localid="1658391074946" rin this state. (As always, look up any nontrivial integrals.)

(c) If you could somehow measure the observable Lx2+Ly2on an atom in this state, what value (or values) could you get, and what is the probability of each?

An electron is in the spin state

χ=A3i4

(a) Determine the normalization constant .

(b) Find the expectation values of Sx,Sy , and Sz.

(c) Find the "uncertainties" ,σSx , σSyandσSz . (Note: These sigmas are standard deviations, not Pauli matrices!)

(d) Confirm that your results are consistent with all three uncertainty principles (Equation 4.100 and its cyclic permutations - only with in place ofL, of course).

[Refer to Problem 4.59 for background.] In classical electrodynamics the potentials Aandφare not uniquely determined; 47 the physical quantities are the fields, E and B.

(a) Show that the potentials

φ'φ-Λt,A'A+Λ

(whereis an arbitrary real function of position and time). yield the same fields asφand A. Equation 4.210 is called a gauge transformation, and the theory is said to be gauge invariant.

(b) In quantum mechanics the potentials play a more direct role, and it is of interest to know whether the theory remains gauge invariant. Show that

Ψ'eiqΛ/Ψ

satisfies the Schrödinger equation (4.205) with the gauge-transformed potentialsφ'andA', SinceΨ'differs fromψonly by a phase factor, it represents the same physical state, 48and the theory is gauge invariant (see Section 10.2.3for further discussion).

Two particles of mass mare attached to the ends of a massless rigid rod of length a. The system is free to rotate in three dimensions about the center (but the center point itself is fixed).

(a) Show that the allowed energies of this rigid rotor are

En=h2n(n+1)ma2, for n=0,1,2,...

Hint: First express the (classical) energy in terms of the total angular momentum.

(b) What are the normalized Eigen functions for this system? What is the degeneracy of thenthenergy level?

Construct the matrixSrrepresenting the component of spin angular momentum along an arbitrary directionr. Use spherical coordinates, for which

rsinθcosΦı+sinθsinΦø+cosθk [4.154]

Find the eigenvalues and (normalized) eigen spinors ofSr. Answer:

x+(r)=(cosθ/2esinθ/2); x+(r)=(esin(θ/2)-cos(θ/2)) [4.155]

Note: You're always free to multiply by an arbitrary phase factor-say,eiϕ-so your answer may not look exactly the same as mine.

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