The energy of a particle of mass m in a box having perfectly rigid walls is given by
En=8ma2n2ℏ2, n = 1, 2, 3, . . . , (4.285)
where a is the size of the box.
(a) (i) For the electron in the box of size 10−10m, we have
En=mec2a2ℏ2c284π2n2≡0.5MeV×1010fm24×104(MeVfm)22π2n2
=4π2n2eV≃39n2eV. (4.286)
Hence E1=39eV,E2=156eV , and E3=315eV.
(ii) For the sphere in the box of side 10 cm we have
En=10−3kg×10−2m2(6.6×10−34Js)2n2=43.6×10−63n2J (4.287)
Hence E1=43.6×10−63J,E2=174.4×10−63J, and E3=392.4×10−63J.
(b) The differences between the energy levels are
(E2−E1)electron=117eV, (E3−E2)electron=195eV, (4.288)
(E2−E1)sphere=130×10−63J, (E3−E2)sphere=218×10−63J (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∼ℏ/(ma). For the electron, the typical distances are atomic, a≃10−10m; hence
υ∼mc2aℏcc∼0.5MeV×105fm200eVfmc≃4×10−3c=1.2×106ms−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:
υ∼maℏ∼10−3kg×10−2m6.6×10−34Js≃6.6×10−29ms−1 (4.291)
At this speed the sphere is practically at rest.