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An electron is in a box of width \(3.0 \times 10^{-10} \mathrm{~m} .\) What are the de Broglie wavelength and the magnitude of the momentum of the electron if it is in (a) the \(n=1\) level; (b) the \(n=2\) level; (c) the \(n=3\) level? In each case how does the wavelength compare to the width of the box?

Short Answer

Expert verified
For \(n=1\), the de Broglie wavelength is \(3.0 \times 10^{-10} m\) and the momentum is \(2.21 \times 10^{-24} kg m/s\). For \(n=2\), the de Broglie wavelength is \(1.5 \times 10^{-10} m\) and the momentum is \(4.42 \times 10^{-24} kg m/s\). For \(n=3\), the de Broglie wavelength is \(1.0 \times 10^{-10} m\) and the momentum is \(6.63 \times 10^{-24} kg m/s\). The de Broglie wavelength decreases as the energy state \(n\) rises, thus the size of the energy state is inversely proportional to the wavelength.

Step by step solution

01

Recall the formula for the de Broglie wavelength

The de Broglie wavelength \(\lambda\) of a particle is given by the equation \(\lambda = h/p\), where \(h\) is Planck's constant and \(p\) is the magnitude of the particle's momentum.
02

Apply the conditions of an electron in a box

For a particle in a one-dimensional box, the particle can be found anywhere within the box, so the width of the box \(\L\) is equal to a whole number of de Broglie wavelengths. This yields the formula \(L = n \lambda\), where \(n\) is a positive integer representing the level of energy state. Rearranging this formula gives us \(\lambda = L/n\). Each level \(n\) will result in a different value for the de Broglie wavelength.
03

Calculate the de Broglie wavelength for each level

For \(n=1\), we have \(\lambda = (3.0 \times 10^{-10} m)/1 = 3.0 \times 10^{-10} m\). For \(n=2\), we have \(\lambda = (3.0 \times 10^{-10} m)/2 = 1.5 \times 10^{-10} m\). For \(n=3\), we have \(\lambda = (3.0 \times 10^{-10} m)/3 = 1.0 \times 10^{-10} m\).
04

Calculate the magnitude of the momentum for each level

By rearranging the de-Broglie equation for momentum, \(p = h/\lambda\), we can find the momentum for each level. Given that Planck's constant \(h = 6.626 \times 10^{-34} \, \mathrm{m^2 kg/s}\), we get, for \(n=1\), \(p = 6.626 \times 10^{-34} \, \mathrm{m^2 kg/s} / 3.0 \times 10^{-10} \, \mathrm{m} = 2.21 \times 10^{-24} \, \mathrm{kg \, m/s}\), for \(n=2\), \(p = 6.626 \times 10^{-34} \, \mathrm{m^2 kg/s}/ 1.5 \times 10^{-10} \, \mathrm{m} = 4.42 \times 10^{-24} \, \mathrm{kg \, m/s}\), and for \(n=3\), \(p = 6.626 \times 10^{-34} \, \mathrm{m^2 kg/s} / 1.0 \times 10^{-10} \, \mathrm{m} = 6.63 \times 10^{-24} \, \mathrm{kg \, m/s}\).
05

Comparison each wavelength to the width of the box

For \(n=1\), the de Broglie wavelength is equal to the width of the box. For \(n=2\), the de Broglie wavelength is half the width of the box, and for \(n=3\), the de Broglie wavelength is one third of the width of the box. This quantitative relationship indicates that as the energy state \(n\) increases, the wavelength decreases and thus the electron's wave behaviour is more localized within the box.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Quantum Mechanics
Quantum mechanics is a fundamental framework in physics. It describes how particles like electrons behave on a very small scale. Unlike classical mechanics, which uses continuous trajectories, quantum mechanics introduces probabilities and wave-particle duality.
At this small scale, particles such as electrons don't follow simple paths. Instead, they are described by wave functions that show the probability of finding the particle in a particular location.
Wave functions are pivotal in quantum mechanics. They are complex mathematical functions that give us important information, including how a particle is likely to be found in various positions in a system. In this context, de Broglie proposed that all matter, including electrons, could be thought of as having wave-like properties, leading to the idea of de Broglie wavelength.
The dual behavior—acting both as a particle and a wave—allows us to predict characteristics like the electron's momentum and its position probability distribution in a confined space like a box.
Particle in a Box
The concept of a 'particle in a box' is a foundational quantum mechanics model. It helps us understand how particles behave when confined in a small, fixed space. Imagine an electron trapped in a tiny box with completely rigid walls; this is a common way to introduce boundary conditions in quantum mechanics.
In this model, the width of the box determines the allowed energy levels of the particle. Inside the box, the particle's wave functions must satisfy certain mathematical equations. Specifically, the wave functions must have nodes at the walls, meaning they go to zero at these points. This leads to quantized energy levels and discrete values of momentum and wavelength.
The simplest form of the model is one-dimensional. Here, the de Broglie wavelength of the electron depends on its energy level, denoted by the quantum number \(n\). The wavelength is inversely proportional to \(n\), meaning as \(n\) increases, the wavelength decreases. This relationship gives insight into the particle's behavior at different energy levels.
Momentum
Momentum in quantum mechanics differs somewhat from classical concepts. For a particle in a box, the momentum is related directly to the particle's wavelength. The de Broglie equation connects these two properties nicely by the formula \(p = h/\lambda\), where \(h\) is Planck's constant and \(\lambda\) the de Broglie wavelength.
When a particle's momentum is considered, its wave-like properties become important. This is because, unlike in classical physics where momentum depends solely on mass and velocity, in quantum physics, it also involves the particle's wave characteristics.
As a particle moves to higher energy levels within a box, its de Broglie wavelength shortens, leading to an increase in momentum. This change in momentum signifies how the particle's energy and behavior are more confining and localized with higher energy states. Thus, understanding momentum from a quantum perspective requires considering both particle's wave properties and the physical constraints, like box size, that influence it.

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Most popular questions from this chapter

An electron is bound in a square well that has a depth equal to six times the ground-level energy \(E_{1-\mathrm{IDW}}\) of an infinite well of the same width. The longest-wavelength photon that is absorbed by this electron has a wavelength of \(582 \mathrm{nm}\). Determine the width of the well.

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An electron is in a one-dimensional box. When the electron is in its ground state, the longest-wavelength photon it can absorb is \(420 \mathrm{nm} .\) What is the next longest-wavelength photon it can absorb, again starting in the ground state?

A fellow student proposes that a possible wave function for a free particle with mass \(m\) (one for which the potential-energy function \(U(x)\) is zero) is $$ \psi(x)=\left\\{\begin{array}{ll} e^{+\kappa x}, & x<0 \\ e^{-\kappa x}, & x \geq 0 \end{array}\right. $$ where \(\kappa\) is a positive constant. (a) Graph this proposed wave function. (b) Show that the proposed wave function satisfies the Schrödinger equation for \(x<0\) if the energy is \(E=-\hbar^{2} \kappa^{2} / 2 m-\) that is, if the energy of the particle is negative. (c) Show that the proposed wave function also satisfies the Schrödinger equation for \(x \geq 0\) with the same energy as in part (b). (d) Explain why the proposed wave function is nonetheless not an acceptable solution of the Schrödinger equation for a free particle. (Hint: What is the behavior of the function at \(x=0 ?\) ) It is in fact impossible for a free particle (one for which \(U(x)=0\) ) to have an energy less than zero.

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