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State whether each of the following statements is true or false. a) The energy of electrons is always discrete. b) The energy of a bound electron is continuous. c) The energy of a free electron is discrete. d) The energy of an electron is discrete when it is bound to an ion.

Short Answer

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Explain your reasoning. a) The energy of electrons is always discrete. b) The energy of a bound electron is continuous. c) The energy of a free electron is discrete. d) The energy of an electron is discrete when it is bound to an ion.

Step by step solution

01

Statement a) The energy of electrons is always discrete.

This statement is false. The energy of electrons can be both discrete and continuous, depending on whether the electron is bound or free. In atoms and ions, electrons are bound, and their energy levels are discrete (quantized). However, in a conducting material like a metal, electrons are free to move, and their energy levels form a continuous band. So, the energy of electrons is not always discrete.
02

Statement b) The energy of a bound electron is continuous.

This statement is false. The energy of a bound electron, like the ones in atoms and ions, is discrete (quantized). Bound electrons can only occupy specific energy levels, which are determined by their quantum numbers (n, l, m, and s). The energy levels of bound electrons are not continuous.
03

Statement c) The energy of a free electron is discrete.

This statement is false. Electrons that are free (not bound to atoms or ions) have continuous energy levels. For example, in a metal, the electrons are free to move and can occupy any energy level within a specific range. The energy levels of free electrons are not quantized and can vary continuously.
04

Statement d) The energy of an electron is discrete when it is bound to an ion.

This statement is true. When an electron is bound to an ion, its energy levels are quantized (discrete). These energy levels are determined by the electron's quantum numbers (n, l, m, and s) and are specific to the ion to which the electron is bound. The energy levels of bound electrons in ions are not continuous.

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Key Concepts

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

Quantum Mechanics

At the core of understanding the behavior of electrons lies quantum mechanics, the branch of physics that deals with the motions and interactions of subatomic particles. It is a foundational tenet of this theory that particles such as electrons exhibit both wave-like and particle-like characteristics. A critical aspect of quantum mechanics is the quantization of physical properties, particularly energy levels in atoms and molecules.

  • Quantum mechanics dictates that not all energy values are permissible for electrons bound within atoms, leading to quantized energy levels.
  • This quantization arises from the wave nature of electrons, which can only sustain stable standing waves at certain frequencies within the confines of an atomic nucleus's influence.
  • The permitted energy levels are basically the 'notes' of the atomic 'music' and define the unique electron configurations that underlie the chemistry of elements.

Waves, Particles, and the Uncertainty Principle

Moreover, the quantum mechanical behavior of electrons is governed by the Heisenberg Uncertainty Principle, which states that certain pairs of physical properties, like position and momentum, cannot be simultaneously measured with arbitrary precision. From an educational perspective, quantum mechanics encourages a shift from deterministic to probabilistic thinking – a challenging but essential intellectual leap for students grappling with modern physics.

Quantization of Energy

When delving into the nature of electron energy levels, it's significant to comprehend the concept of quantization of energy. This principle describes how electrons can only possess specific values of energy and nothing in between. The discrete energy levels are akin to the rungs of a ladder: an electron can 'jump' from one rung to another, but it cannot exist halfway between two rungs.

  • Energies of bound electrons in atoms are quantized, which is why they can only absorb or emit photons (light particles) of certain energies—corresponding to the differences between these fixed rungs.
  • Quantization explains a host of phenomena, from the colors emitted by fireworks to the absorption lines in the spectra of stars.
  • It also underlies the understanding of chemical bonding, where electron transitions between quantized energy levels lead to energy absorption or release.

Quantum Numbers and Electron Orbits

Conceptually, quantization can be explored through quantum numbers that define an electron's state. These include the principal quantum number (n), angular momentum quantum number (l), magnetic quantum number (m), and spin quantum number (s), which together specify the discrete energy levels within atoms.

Bound and Free Electrons

The concept of bound and free electrons is central to understanding the differences in energy state behavior. Bound electrons are those attached to an atom or molecule and are confined to specific energy levels as dictated by the laws of quantum mechanics. These electrons can only jump to another level by absorbing or emitting a photon of precise energy. These jumps are what give rise to the spectral lines we see in emission and absorption spectra.

  • In contrast, free electrons, such as those found in metals or in plasma states, are not restricted to discrete energy levels. These electrons have the freedom to move within a continuum of energy states.
  • This distinction between bound and free electrons explains the differing electrical and thermal properties of materials; conductors, semiconductors, and insulators display unique behaviors based on the freedom of their electrons.
  • Understanding the concept of bound and free electrons also clarifies the exercise statements, particularly in comprehending why the energy of free electrons is continuous while that of bound electrons is quantized.

Applications in Technology

The concepts of bound and free electrons are not just theoretical but have practical implications in semiconductor technology, lasers, and even the functioning of solar cells, all of which rely on the manipulation of electron energy states.

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Most popular questions from this chapter

Electrons from a scanning tunneling microscope encounter a potential barrier that has a height of \(U=4.0 \mathrm{eV}\) above their total energy. By what factor does the tunneling current change if the tip moves a net distance of \(0.10 \mathrm{nm}\) farther from the surface?

Two long, straight wires that lie along the same line have a separation at their tips of \(2.00 \mathrm{nm}\). The potential energy of an electron in the gap is about \(1.00 \mathrm{eV}\) higher than it is in the conduction band of the two wires. Conduction-band electrons have enough energy to contribute to the current flowing in the wire. What is the probability that a conduction electron in one wire will be found in the other wire after arriving at the gap?

The ground state wave function for a harmonic oscillator is given by \(\Psi_{0}(x)=A_{2} e^{-x^{2} / 2 b^{2}}\). a) Determine the normalization constant \(A\). b) Determine the probability that a quantum harmonic oscillator in the \(n=0\) state will be found in the classically forbidden region.

An electron is confined in a three-dimensional cubic space of \(L^{3}\) with infinite potentials. a) Write down the normalized solution of the wave function in the ground state. b) How many energy states are available up to the second excited state from the ground state? (Take the electron spin into account.)

An approximate one-dimensional quantum well can be formed by surrounding a layer of GaAs with layers of \(\mathrm{Al}_{x} \mathrm{Ga}_{1-x}\) As. The GaAs layers can be fabricated in thicknesses that are integral multiples of the single-layer thickness, \(0.28 \mathrm{nm}\). Some electrons in the GaAs layer behave as if they were trapped in a box. For simplicity, treat the box as an infinite one-dimensional well and ignore the interactions between the electrons and the Ga and As atoms (such interactions are often accounted for by replacing the actual electron mass with an effective electron mass). Calculate the energy of the ground state in this well for these cases: a) 2 GaAs layers b) 5 GaAs layers

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