Question 4.P.10: Consider the box potential V(x) = {0, 0<xa, ∞, elsewhere....

Consider the box potential

V(x)={0,0<x<a,,elsewhere.V(x)=\begin{cases} 0, & 0<x<a, \\ \infty , & elsewhere.\end{cases} .

(a) Estimate the energies of the ground state as well as those of the first and the second excited states for (i) an electron enclosed in a box of size a=1010ma=10^{-10} m (express your answer in electron volts; you may use these values: c=200MeVfm,mec2=0.5MeV\hbar c=200Me V fm, m_{e}c^{2}=0.5Me V); (ii) a 1 g metallic sphere which is moving in a box of size a = 10 cm (express your answer in joules).
(b) Discuss the importance of the quantum effects for both of these two systems.
(c) Use the uncertainty principle to estimate the velocities of the electron and the metallic sphere.

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The energy of a particle of mass m in a box having perfectly rigid walls is given by

En=n228ma2E_{n}=\frac{n^{2}\hbar ^{2} }{8ma^{2}},       n = 1, 2, 3, . . . ,                      (4.285)

where a is the size of the box.
(a) (i) For the electron in the box of size 1010m10^{-10} m, we have

En=2c2mec2a24π2n284×104(MeVfm)20.5MeV×1010fm2π22n2E_{n}=\frac{\hbar ^{2}c^{2} }{m_{e}c^{2}a^{2} } \frac{4\pi ^{2}n^{2} }{8} \equiv \frac{4\times 10^{4}(MeV fm)^{2} }{0.5Me V\times 10^{10}fm^{2} } \frac{\pi ^{2}}{2}n^{2}

 

=4π2n2eV39n2eV=4\pi ^{2}n^{2}e V\simeq 39n^{2}eV.                    (4.286)

Hence E1=39eV,E2=156eV E_{1}=39eV,E_{2}=156eV , and E3=315eVE_{3}= 315 eV .

(ii) For the sphere in the box of side 10 cm we have

En=(6.6×1034Js)2103kg×102m2n2=43.6×1063n2JE_{n}=\frac{(6.6\times10^{-34}J s )^{2} }{10^{-3}kg\times 10^{-2}m^{2}} n^{2}=43.6\times 10^{-63}n^{2}J            (4.287)

Hence E1=43.6×1063J,E2=174.4×1063JE_{1}=43.6\times 10^{-63}J,E_{2}=174.4\times 10^{-63}J , and E3=392.4×1063JE_{3}=392.4\times 10^{-63}J.

(b) The differences between the energy levels are

(E2E1)electron=117eV(E_{2}-E_{1})_{electron} =117eV,      (E3E2)electron=195eV(E_{3}-E_{2}) _{electron} =195eV,             (4.288)

 

(E2E1)sphere=130×1063J(E_{2}-E_{1})_{sphere} =130\times 10^{-63}J,      (E3E2)sphere=218×1063J (E_{3}-E_{2})_{sphere} =218\times 10^{-63}J          (4.289)

These results show that:
• The spacings between the energy levels of the electron are quite large; the levels are far apart from each other. Thus, the quantum effects are important.

• The energy levels of the sphere are practically indistinguishable; the spacings between the levels are negligible. The energy spectrum therefore forms a continuum; hence the quantum effects are not noticeable for the sphere.

(c) According to the uncertainty principle, the speed is proportional to υ/(ma)\upsilon \sim \hbar /(ma). For the electron, the typical distances are atomic, a1010ma\simeq 10^{-10} m; hence

υcmc2ac200eVfm0.5MeV×105fmc4×103c=1.2×106ms1\upsilon \sim \frac{\hbar c}{mc^{2}a} c\sim \frac{200eV fm}{0.5MeV\times 10^{5} fm} c\simeq 4\times 10^{-3}c=1.2\times 10^{6} ms^{-1},           (4.290)

where c is the speed of light. The electron therefore moves quite fast; this is expected since we have confined the electron to move within a small region.
For the sphere, the typical distances are in the range of 1 cm:

υma6.6×1034Js103kg×102m6.6×1029ms1\upsilon \sim \frac{\hbar }{ma} \sim \frac{6.6\times 10^{-34}Js}{10^{-3}kg\times 10^{-2}m} \simeq 6.6\times 10^{-29}ms^{-1}             (4.291)

At this speed the sphere is practically at rest.

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