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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=±õÓ¬.

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

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

L=25mr2vr=25mrg∴r=re=e24πo0mc2‵andL=h/2h2=25me24πo0mc2‵θh=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,

Ï‘=5Ï€³óo'c2e2=5Ï€1.055×10-348.85×10-123×10821.6×10-192=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.,Ï‘>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

The fundamental commutation relations for angular momentum (Equation 4.99) allow for half-integer (as well as integer) eigenvalues. But for orbital angular momentum only the integer values occur. There must be some extra constraint in the specific formL=r×p that excludes half-integer values. Let be some convenient constant with the dimensions of length (the Bohr radius, say, if we're talking about hydrogen), and define the operators

q1≡12[x+a2/ħpy];p1≡12[px-(ħ/a2)y];q2≡12[x-(a2/ħ)py];p2≡12[px-(ħ/a2)y];

(a) Verify that [q1,q2]=[p1,p2]=0;[q1,p1]=[p2,q2]=iħ. Thus the q's and the p's satisfy the canonical commutation relations for position and momentum, and those of index 1are compatible with those of index 2 .

(b) Show that[q1,q2]=[p1,p2]Lz=ħ2a2(q12-q22)+a22ħ(p12-p22)

(c) Check that , where each is the Hamiltonian for a harmonic oscillator with mass and frequency .

(d) We know that the eigenvalues of the harmonic oscillator Hamiltonian are , where (In the algebraic theory of Section this follows from the form of the Hamiltonian and the canonical commutation relations). Use this to conclude that the eigenvalues of must be integers.

Work out the normalization factor for the spherical harmonics, as follows. From Section 4.1.2we know that

Ylm=BlmeimϕPlmcosθ

the problem is to determine the factor (which I quoted, but did not derive, in Equation 4.32). Use Equations 4.120, 4.121, and 4.130to obtain a recursion

relation giving Blm+1 in terms of Blm. Solve it by induction on to get Blm up to an overall constant Cl, .Finally, use the result of Problem 4.22 to fix the constant. You may find the following formula for the derivative of an associated Legendre function useful:

1-x2dPlmdx=1-x2Plm+1-mxPlm [4.199]

Consider the three-dimensional harmonic oscillator, for which the potential is

V(r)=12mÓ¬2r2

(a) Show that separation of variables in cartesian coordinates turns this into three one-dimensional oscillators, and exploit your knowledge of the latter to determine the allowed energies. Answer:

En=(n+3/2)hÓ¬

(b) Determine the degeneracyofd(n)ofEn.

What is the probability that an electron in the ground state of hydrogen will be found inside the nucleus?

  1. First calculate the exact answer, assuming the wave function is correct all the way down tor=0. Let b be the radius of the nucleus.
  2. Expand your result as a power series in the small numbera=2bla, and show that the lowest-order term is the cubic:P≈(4l3)(bla)3. This should be a suitable approximation, provided thatb≪a(which it is).
  3. Alternatively, we might assume thatψ(r)is essentially constant over the (tiny) volume of the nucleus, so thatP≈(4l3)πb3lψ(0)l2.Check that you get the same answer this way.
  4. Useb≈10-15manda≈0≈5×10-10mto get a numerical estimate forP. Roughly speaking, this represents the fraction of its time that the electron spends inside the nucleus:"

(a) If you measured the component of spin angular momentum along the x direction, at time t, what is the probability that you would get +h/2?

(b) Same question, but for the ycomponent.

(c) Same, for the z component.

See all solutions

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