Problem 88
Question
As the orbit number increases, the difference in two consecutive energy levels (a) remain constant (b) increases (c) decreases (d) is unpredictable
Step-by-Step Solution
Verified Answer
As the orbit number increases, the difference in two consecutive energy levels decreases.
1Step 1: Understanding the Energy Levels in an Atom
The energy levels in an atom can be described by the Bohr model, where electrons orbit the nucleus at certain discrete energy levels. The energy of each level is given by the formula: \( E_n = -\frac{Z^2 me^4}{8h^2\epsilon_0^2n^2} \), where \( E_n \) is the energy of the nth level, \( Z \) is the atomic number, \( m \) is the electron mass, \( e \) is the charge of the electron, \( h \) is Planck's constant, \( \epsilon_0 \) is the permittivity of free space, and \( n \) is the principal quantum number (orbit number).
2Step 2: Analyzing the Difference in Energy Between Consecutive Levels
To find how the difference in energy between consecutive levels changes, we calculate the difference between the energies of the nth and (n+1)th levels: \( \Delta E = E_n - E_{n+1} \). By using the energy formula, this becomes: \( \Delta E = -\frac{Z^2 me^4}{8h^2\epsilon_0^2} \left( \frac{1}{n^2} - \frac{1}{(n+1)^2} \right) \).
3Step 3: Determining the Trend in Energy Difference
As \( n \) increases, the difference \( \left( \frac{1}{n^2} - \frac{1}{(n+1)^2} \right) \) gets smaller because the terms \( \frac{1}{n^2} \) and \( \frac{1}{(n+1)^2} \) become closer in value. Therefore, the difference in energy between two consecutive levels decreases as the orbit number increases.
Key Concepts
Bohr ModelQuantum NumberAtomic Structure
Bohr Model
The Bohr model of the atom is a conceptually enlightening framework introduced by Niels Bohr in 1913. This model revolutionized the understanding of atomic structure by postulating discrete energy levels for electrons. According to the Bohr model, electrons orbit the nucleus in specific paths or 'shells' without radiating energy, contrary to classical electrodynamics predictions.
The energy of an electron in an orbit is quantized, meaning it can only occupy certain allowed energy levels. Mathematically, the energy associated with an orbit is calculated using the formula: \( E_n = -\frac{Z^2 e^4 m}{8h^2\epsilon_0^2 n^2} \), where \( E_n \) represents the energy of the nth orbit, and \( n \) is an integer known as the principal quantum number. Each of these orbits corresponds to a different energy level, and transitions between them result in the absorption or emission of photons with specific frequencies.
It's notable that the Bohr model, while fundamental, is an approximation and has been superseded by quantum mechanics. However, it remains a valuable tool for simplifying complex concepts and is applicable for explaining the spectra of hydrogen and hydrogen-like atoms.
The energy of an electron in an orbit is quantized, meaning it can only occupy certain allowed energy levels. Mathematically, the energy associated with an orbit is calculated using the formula: \( E_n = -\frac{Z^2 e^4 m}{8h^2\epsilon_0^2 n^2} \), where \( E_n \) represents the energy of the nth orbit, and \( n \) is an integer known as the principal quantum number. Each of these orbits corresponds to a different energy level, and transitions between them result in the absorption or emission of photons with specific frequencies.
It's notable that the Bohr model, while fundamental, is an approximation and has been superseded by quantum mechanics. However, it remains a valuable tool for simplifying complex concepts and is applicable for explaining the spectra of hydrogen and hydrogen-like atoms.
Quantum Number
In atomic physics, quantum numbers are values that describe the quantum state of a particle within an atom. These numbers are crucial for understanding the arrangement of electrons in atoms, referred to as the electronic configuration. The principal quantum number, denoted by \( n \), plays a central role in determining the energy of an electron in an atom.
The principal quantum number defines the shell or energy level of an electron and can take positive integer values starting from 1 upward. Higher values of \( n \) indicate electrons are further away from the nucleus, occupying higher-energy orbits. These quantum numbers also correspond to the periods on the periodic table, giving insight into an element's chemical properties and reactivity.
Other quantum numbers include the azimuthal quantum number (\( l \)), the magnetic quantum number (\( m_l \)), and the spin quantum number (\( m_s \)), each further describing orbital shape, orientation, and electron spin, respectively. The full set of quantum numbers defines the unique quantum state of an electron and follows the Pauli exclusion principle, ensuring no two electrons in an atom have the same set of all four quantum numbers.
The principal quantum number defines the shell or energy level of an electron and can take positive integer values starting from 1 upward. Higher values of \( n \) indicate electrons are further away from the nucleus, occupying higher-energy orbits. These quantum numbers also correspond to the periods on the periodic table, giving insight into an element's chemical properties and reactivity.
Other quantum numbers include the azimuthal quantum number (\( l \)), the magnetic quantum number (\( m_l \)), and the spin quantum number (\( m_s \)), each further describing orbital shape, orientation, and electron spin, respectively. The full set of quantum numbers defines the unique quantum state of an electron and follows the Pauli exclusion principle, ensuring no two electrons in an atom have the same set of all four quantum numbers.
Atomic Structure
The atomic structure encompasses the arrangement of subatomic particles within an atom, which comprises a dense nucleus surrounded by a cloud of electrons. The nucleus contains protons and neutrons, which account for the majority of an atom's mass. The number of protons, or the atomic number \( Z \), uniquely identifies an element. Electrons, significantly lighter than nucleons, move around the nucleus occupying various energy levels.
In a simplified view, atomic structure is layered with electrons found at different energy levels or 'shells', determined by their principal quantum number \( n \). These shells serve as a model to visualize electron configuration, and are conceptually useful for understanding chemical bonding and reactivity. Energy levels closest to the nucleus have lower energy and are generally filled first, obeying a set of rules known as the Aufbau principle.
Additionally, the discrete nature of energy levels explains many phenomena in quantum mechanics and chemistry, such as ionization energies and the line spectra of elements. Understanding atomic structure is foundational to the study of physics and chemistry, as it provides a basis on which the behavior of atoms and molecules can be explained.
In a simplified view, atomic structure is layered with electrons found at different energy levels or 'shells', determined by their principal quantum number \( n \). These shells serve as a model to visualize electron configuration, and are conceptually useful for understanding chemical bonding and reactivity. Energy levels closest to the nucleus have lower energy and are generally filled first, obeying a set of rules known as the Aufbau principle.
Additionally, the discrete nature of energy levels explains many phenomena in quantum mechanics and chemistry, such as ionization energies and the line spectra of elements. Understanding atomic structure is foundational to the study of physics and chemistry, as it provides a basis on which the behavior of atoms and molecules can be explained.
Other exercises in this chapter
Problem 86
The potential energy of electron revolving in the ground state of \(\mathrm{H}\) atom is (a) \(-13.6 \mathrm{eV}\) (b) \(-6.8 \mathrm{eV}\) (c) \(-27.2 \mathrm{
View solution Problem 88
Photoelectrons are liberated by ultraviolet light of wavelength \(3000 \AA\) from a metallic surface for which the photoelectric threshold is \(4000 \AA\). The
View solution Problem 89
The minimum uncertainty in de-Broglie wavelength of an electron accelerated from rest by a potential difference of \(6.0 \mathrm{~V}\), if the uncertainty in me
View solution Problem 91
The orbital angular momentum of \(2 \mathrm{p}\) and \(3 \mathrm{p}\) -orbitals (a) are same (b) are different, more for 2p-orbital (c) are different, more for
View solution