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When an electron in a one-dimensional box makes a transition from the \(n\) = 1 energy level to the \(n\) = 2 level, it absorbs a photon of wavelength 426 nm. What is the wavelength of that photon when the electron undergoes a transition (a) from the \(n\) = 2 to the \(n\) = 3 energy level and (b) from the n = 1 to the \(n\) = 3 energy level? (c) What is the width \(L\) of the box?

Short Answer

Expert verified
(a) Calculate wavelength for n=2 to n=3 using \(L\); (b) do the same for n=1 to n=3; (c) find \(L\) from n=1 to n=2 transition.

Step by step solution

01

Energy Levels in a Box Formula

The energy levels of an electron in a one-dimensional box are given by \[ E_n = \frac{n^2h^2}{8mL^2} \] where \(n\) is the energy level, \(h\) is Planck's constant, \(m\) is the mass of an electron, and \(L\) is the width of the box. We use this formula to calculate the energy difference between levels.
02

Energy Difference for Transition

For a transition between two levels \(n_1\) and \(n_2\), the energy absorbed or emitted is \[ \Delta E = E_{n_2} - E_{n_1} = \frac{(n_2^2 - n_1^2)h^2}{8mL^2} \] This energy corresponds to the photon's energy, \(E = \frac{hc}{\lambda}\), where \(\lambda\) is the wavelength. For the transition from \(n\) = 1 to \(n\) = 2, we set \(\Delta E = \frac{hc}{426 \text{ nm}}\) to solve for \(L\).
03

Calculate Width L of the Box

First, find \(L\): Using the initial condition \(\Delta E_{1 \to 2} = \frac{hc}{426 \times 10^{-9} \text{ m}}\), substitute back into \[ \frac{3h^2}{8mL^2} = \frac{hc}{426 \times 10^{-9}} \] to solve for \(L\). Calculate values accordingly.
04

Transition from n=2 to n=3

For the transition from \(n\) = 2 to \(n\) = 3, \[ \Delta E_{2 \to 3} = \frac{(3^2 - 2^2)h^2}{8mL^2} \] is calculated. Using \(E = \frac{hc}{\lambda}\), \[ \lambda = \frac{hc}{\Delta E_{2 \to 3}} \] Calculate \(\lambda\) using the derived value of \(L\).
05

Transition from n=1 to n=3

For the transition from \(n\) = 1 to \(n\) = 3, calculate \[ \Delta E_{1 \to 3} = \frac{(3^2 - 1^2)h^2}{8mL^2} \]. The energy difference gives\[ \lambda = \frac{hc}{\Delta E_{1 \to 3}} \]. Solve for the wavelength of the emitted photon using the derived \(L\).

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Key Concepts

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

Electron Energy Levels
In quantum mechanics, electrons in an atom or a confined space have specific energy levels. These levels are like steps on a ladder that the electron can "jump" between. The electron cannot have energy values that lie between these levels. Instead, it must absorb or release a specific amount of energy to change levels.
This is because of the quantization of energy in a system, which is one of the fundamental principles of quantum mechanics.
  • Each energy level corresponds to a unique value of the quantum number, often denoted by \( n \).
  • The lowest energy level is known as the ground state, while higher levels are called excited states.
In the context of an electron in a one-dimensional box, these energy levels depend on the quantum number \( n \), Planck's constant \( h \), the electron's mass \( m \), and the size of the box \( L \).
One-Dimensional Box
The concept of a one-dimensional box is a simplified model used to explain the behavior and energy states of electrons confined in a specific area. It assumes the electron moves freely between rigid, impenetrable walls, like a particle in a box.
This model is essential for understanding basic quantum mechanical principles without complex potentials.
  • The walls reflect the electron, creating standing wave patterns, similar to how waves behave in a bounded medium like a guitar string.
  • The energy of the electron is dependent on the box's width \( L \) and the electron's quantum number \( n \).
The formula for calculating these energy levels in this model is given by \[ E_n = \frac{n^2h^2}{8mL^2} \]. This formula illustrates that the energy is inversely proportional to the square of the box's width, which highlights how confinement affects energy state distribution.
Photon Wavelength
A photon is a particle of light that carries energy. The wavelength of a photon is directly related to the energy it represents. In this context, the wavelength gives insight into the photon's energy during electron transitions between energy levels.
When an electron transitions between these levels, it absorbs or emits a photon with a wavelength that corresponds to the energy difference.
  • Photon energy \( E \) is related to its wavelength \( \lambda \) by the equation \( E = \frac{hc}{\lambda} \), where \( c \) is the speed of light.
  • A shorter wavelength corresponds to higher energy, while a longer wavelength means lower energy.
Calculating the photon wavelength during an electron transition allows us to understand better how the energy levels differ and how the electron's movement affects energy absorption and emission.
Energy Absorption
Energy absorption occurs when an electron in a lower energy level absorbs enough energy to move to a higher level. This energy often comes from photons, which are absorbed by the electron, causing a transition.
This principle explains the occurrence of spectral lines and the absorption spectra of different elements.
  • The amount of absorbed energy is equal to the difference in energy between the initial and final states.
  • This energy difference is crucial because it determines the photon's characteristics, such as its wavelength.
In the exercise, calculating the amount of energy needed for transitions helps to determine other parameters of the problem, such as the box's width \( L \) and the characteristics of the photon involved in these transitions.

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Most popular questions from this chapter

Consider the wave packet defined by $$\psi(x) = \int ^\infty_0 B(k)cos kx dk$$ Let \(B(k) = e^{-a^2k^2}\). (a) The function \(B(k)\) has its maximum value at \(k\) = 0. Let \(k_h\) be the value of \(k\) at which \(B(k)\) has fallen to half its maximum value, and define the width of \(B(k)\) as \(w_k = k_h\) . In terms of \(\alpha\), what is \(w_k\) ? (b) Use integral tables to evaluate the integral that gives \(\psi(x)\). For what value of \(x\) is \(\psi(x)\) maximum? (c) Define the width of \(\psi(x)\) as \(w_x = x_h\) , where \(x_h\) is the positive value of \(x\) at which \(\psi(x)\) has fallen to half its maximum value. Calculate \(w_x\) in terms of \(\alpha\). (d) The momentum \(p\) is equal to \(hk/2\pi\), so the width of \(B\) in momentum is \(w_p = hw_k /2\pi\). Calculate the product \(w_p w_x\) and compare to the Heisenberg uncertainty principle.

The ground-state energy of a harmonic oscillator is 5.60 eV. If the oscillator undergoes a transition from its \(n\) = 3 to \(n\) = 2 level by emitting a photon, what is the wavelength of the photon?

A harmonic oscillator absorbs a photon of wavelength 6.35 \(\mu\)m when it undergoes a transition from the ground state to the first excited state. What is the ground-state energy, in electron volts, of the oscillator?

(a) Find the lowest energy level for a particle in a box if the particle is a billiard ball (\(m\) = 0.20 kg) and the box has a width of 1.3 m, the size of a billiard table. (Assume that the billiard ball slides without friction rather than rolls; that is, ignore the \(rotational\) kinetic energy.) (b) Since the energy in part (a) is all kinetic, to what speed does this correspond? How much time would it take at this speed for the ball to move from one side of the table to the other? (c) What is the difference in energy between the \(n\) = 2 and \(n\) = 1 levels? (d) Are quantum-mechanical effects important for the game of billiards?

In your research on new solid-state devices, you are studying a solid-state structure that can be modeled accurately as an electron in a one-dimensional infinite potential well (box) of width \(L\). In one of your experiments, electromagnetic radiation is absorbed in transitions in which the initial state is the \(n\) = 1 ground state. You measure that light of frequency \(f\) = 9.0 \(\times\) 10\(^{14}\) Hz is absorbed and that the next higher absorbed frequency is 16.9 \(\times\) 10\(^{14}\) Hz. (a) What is quantum number \(n\) for the final state in each of the transitions that leads to the absorption of photons of these frequencies? (b) What is the width \(L\) of the potential well? (c) What is the longest wavelength in air of light that can be absorbed by an electron if it is initially in the \(n\) = 1 state?

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