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An electron is confined in a one-dimensional box of length \(L\). Another electron is confined in a box of length 2 \(L\). Both are in the ground state. What is the ratio of their energies $E_{2 l} / E_{L} ?$

Short Answer

Expert verified
Answer: The ratio of the energies of the electrons is \(E_{2L}/E_{L} = \frac{1}{4}\).

Step by step solution

01

Calculate the energy of the electron in a box of length L

Using the formula for the energy of a particle in a one-dimensional box, we can calculate the ground-state energy (\(E_1\)) of an electron in a box of length \(L\): $$ E_{L} = \frac{1^2 \hbar^2 \pi^2}{2mL^2} $$
02

Calculate the energy of the electron in a box of length 2L

Similarly, we can calculate the ground-state energy (\(E'_1\)) of an electron in a box of length \(2L\): $$ E_{2L} = \frac{1^2 \hbar^2 \pi^2}{2m(2L)^2} $$
03

Find the ratio of their energies \(E_{2L} / E_{L}\)

Dividing the energy of the electron in the box of length \(2L\) by the energy of the electron in the box of length \(L\), we get: $$ \frac{E_{2L}}{E_{L}} = \frac{\frac{1^2 \hbar^2 \pi^2}{2m(2L)^2}}{\frac{1^2 \hbar^2 \pi^2}{2mL^2}} $$
04

Simplify the expression

Simplifying the expression, we get: $$ \frac{E_{2L}}{E_{L}} = \frac{\frac{1^2 \hbar^2 \pi^2}{2m(2L)^2}}{\frac{1^2 \hbar^2 \pi^2}{2mL^2}} = \frac{1^2 \hbar^2 \pi^2 \cdot 2mL^2}{2m(2L)^2\cdot 1^2 \hbar^2 \pi^2} = \frac{1}{2^2} = \frac{1}{4} $$ Therefore, the ratio of the energies of the electrons is \(E_{2L}/E_{L} = \frac{1}{4}\).

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Before the discovery of the neutron, one theory of the nucleus proposed that the nucleus contains protons and electrons. For example, the helium-4 nucleus would contain 4 protons and 2 electrons instead of - as we now know to be true- 2 protons and 2 neutrons. (a) Assuming that the electron moves at nonrelativistic speeds, find the ground-state energy in mega-electron- volts of an electron confined to a one-dimensional box of length $5.0 \mathrm{fm}\( (the approximate diameter of the \)^{4} \mathrm{He}$ nucleus). (The electron actually does move at relativistic speeds. See Problem \(80 .)\) (b) What can you conclude about the electron-proton model of the nucleus? The binding energy of the \(^{4} \mathrm{He}\) nucleus - the energy that would have to be supplied to break the nucleus into its constituent particles-is about \(28 \mathrm{MeV} .\) (c) Repeat (a) for a neutron confined to the nucleus (instead of an electron). Compare your result with (a) and comment on the viability of the proton-neutron theory relative to the electron-proton theory.
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