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(a) The doubly charged ion \(\mathrm{N}^{2+}\) is formed by removing two electrons from a nitrogen atom. What is the ground-state electron configuration for the \(N^{2+}\) ion? (b) Estimate the energy of the least strongly bound level in the \(L\) shell of \(N^{2+} .(c)\) The doubly charged ion \mathrm{P}^{2+}\( is formed by removing two electrons from a phosphorus atom. What is the ground-state electron configuration for the \)\mathrm{P}^{2+}\( ion? (d) Estimate the energy of the least strongly bound level in the \)M\( shell of \)\mathrm{P}^{2+}$ .

Short Answer

Expert verified
(a) N虏鈦: 1s虏 2s虏 2p鹿. (b) Use Z_eff to find energy for 2p electron. (c) P虏鈦: 1s虏 2s虏 2p鈦 3s虏 3p鹿. (d) Calculate 3p energy with Z_eff.

Step by step solution

01

Understand Electron Configurations

The electron configuration of an atom describes the distribution of electrons in the atomic orbitals. For the nitrogen atom (N), the atomic number is 7, so it has 7 electrons. Its neutral configuration is 1s虏 2s虏 2p鲁.
02

Determine the Ground-State Configuration for N虏鈦

The doubly charged ion \( N^{2+} \) is formed by removing two electrons from a neutral nitrogen atom. Removing two electrons from the 2p orbital (which is the outermost) results in: 1s虏 2s虏 2p鹿.
03

Energy of Least Strongly Bound Electron in N虏鈦

The L shell corresponds to the n=2 level (2s and 2p orbitals). For \( N^{2+} \), the least strongly bound electron is the one in the 2p orbital. Calculate using the effective nuclear charge (Z_eff) and energy level formula: \( E_n \approx -Z_{eff}^2/n^2 \times 13.6 \text{ eV} \). For nitrogen (approximate): Z_eff can be about 5 for the p-electron.
04

Understand Electron Configuration for Phosphorus

Phosphorus (P) has an atomic number of 15, meaning it has 15 electrons. Its neutral configuration is 1s虏 2s虏 2p鈦 3s虏 3p鲁.
05

Determine the Ground-State Configuration for P虏鈦

The doubly charged \( P^{2+} \) ion is formed by removing two electrons, typically from the outermost 3p orbital, resulting in: 1s虏 2s虏 2p鈦 3s虏 3p鹿.
06

Energy of Least Strongly Bound Electron in P虏鈦

The M shell corresponds to the n=3 level (3s and 3p orbitals). For \( P^{2+} \), the least strongly bound electron is in the 3p orbital. Use a similar calculation as Step 3, adjusting for phosphorus with Z_eff estimated around 13.

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Key Concepts

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

Atomic Orbitals
Atomic orbitals are regions in an atom where electrons are most likely to be found. Each electron in an atom occupies a specific atomic orbital, determined by its energy level and subshell.
The major types of atomic orbitals include:
  • s orbitals: Spherical in shape and can hold up to 2 electrons.
  • p orbitals: Dumbbell-shaped and can hold up to 6 electrons across three orientations (p鈧, p_y, and p_z).
  • d orbitals: More complex shapes, accommodating up to 10 electrons across five orientations.
  • f orbitals: Even more complex, holding up to 14 electrons across seven orientations.
Understanding atomic orbitals is crucial for determining the electron configuration of an atom. Electrons fill the lower-energy orbitals first (like s), before moving to higher-energy orbitals (like p and d). This principle follows the Aufbau Rule.
Ground State
The ground state of an atom or ion is its most stable and low-energy electron configuration. This configuration helps atom maintain the lowest possible energy.
In the ground state, electrons are distributed among orbitals in a way that they occupy the lowest available energy levels. For instance, in the nitrogen ion \(N^{2+}\), the electrons fill the 1s, 2s, and then the 2p orbitals sequentially according to their energy.
The electrons' distribution follows several key principles to establish the ground state:
  • Hund鈥檚 Rule: Electrons occupy degenerate orbitals singly before pairing up.
  • Pauli Exclusion Principle: No two electrons in an atom can have the same set of four quantum numbers.
  • Aufbau Principle: Electrons fill orbitals of the lowest energy first.
The understanding of ground-state electron configurations provides a fundamental basis for predicting chemical reactivity and bonding.
Effective Nuclear Charge
Effective nuclear charge (Z_eff) is the net positive charge experienced by an electron in a multi-electron atom or ion, reflecting how strongly the nucleus attracts a particular electron. This concept is crucial for explaining the energy levels and behavior of electrons within an atom.
Electrons closer to the nucleus partially shield outer electrons from the full nuclear charge, a phenomenon known as electron shielding. As a result, the effective nuclear charge can be significantly less than the actual charge of the nucleus.
  • Inner electron shielding: Core electrons shield outer electrons effectively, reducing the attraction from the nucleus.
  • Penetration effect: Electrons in s orbitals can penetrate closer to the nucleus, experiencing greater effective nuclear charge than electrons in p, d, or f orbitals of the same energy level.
Calculating (or estimating) Z_eff is important when considering the energy calculations of least bound electrons, like in \(N^{2+}\) or \(P^{2+}\), to determine ionization energies and affinity.
Energy Levels
Energy levels refer to the distinct layers or shells containing the electrons within an atom. They help describe the arrangement and stability of electrons surrounding an atomic nucleus. Each level can house a specific number of electrons, increasing with the higher levels.
The main characteristics of energy levels are:
  • Principal quantum number (): Indicates the relative size and energy of an electron shell.
  • Sublevels: Each energy level is made up of sublevels or orbitals (s, p, d, f), with the number and type depending on the principal quantum number.
  • Maximum electron capacity: The nth energy level can hold a maximum of \((2n^2)\) electrons. For instance, the first energy level can house up to 2 electrons, while the second can accommodate up to 8 electrons.
Energy levels determine where an electron resides around the nucleus and its potential energy. In doubly charged ions like \(N^{2+}\) and \(P^{2+}\), electrons in higher energy levels (e.g., =2 for L shell or =3 for M shell) are often the least strongly bound and most reactive. Understanding energy levels aids in predicting atomic behavior and properties.

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Most popular questions from this chapter

A hydrogen atom is in a d state. In the absence of an external magnetic field the states with different \(m_{l}\) values have (approximately) the same energy. Consider the interaction of the magnetic field with the atom's orbital magnetic dipole moment. (a) Calculate the splitting (in electron volts) of the \(m_{l}\) levels when the atom is put in a \(0.400-\mathrm{T}\) magnetic field that is in the \(+z\) -direction. (b) Which \(m_{l}\) level will have the lowest energy? (c) Draw an energy-level diagram that shows the \(d\) levels with and without the external magnetic field.

(a) Write out the ground-state electron configuration \(\left(1 s^{2},\right.\) \(2 s^{2}, \ldots .\) for the beryllium atom. (b) What element of next-larger \(Z\) has chemical properties similar to those of beryllium? Give the ground- state electron configuration of this element. (c) Use the procedure of part (b) to predict what element of next-larger \(Z\) than in (b) will have chemical properties similar to those of the element you found in part (b), and give its ground-state electron configuration.

Electron Spin Resonance. Electrons in the lower of two spin states in a magnetic field can absorb a photon of the right frequency and move to the higher state. (a) Find the magnetic-field magnitude \(B\) required for this transition in a hydrogen atom with \(n=1\) and \(l=0\) to be induced by microwaves with wavelength \(\lambda\) . (b) Calculate the value of \(B\) for a wavelength of 3.50 \(\mathrm{cm} .\)

For germanium \((\mathrm{Ge}, \mathrm{Z}=32),\) make a list of the number of electrons in each subshell \((1 s, 2 s, 2 p, \ldots) .\) Use the allowed values of the quantum numbers along with the exclusion principle; do not refer to Table \(41.3 .\)

(a) If the value of \(L_{z}\) is known, we cannot know either \(L_{x}\) or \(L_{y}\) precisely. But we can know the value of the quantity \(\sqrt{L_{x}^{2}+L_{y}^{2}}\) . Write an expression for this quantity in terms of \(l\) \(m_{l},\) and \(\hbar .\) (b) What is the meaning of \(\sqrt{L_{\mathrm{r}}^{2}+L_{\mathrm{y}}^{2}} ?(\mathrm{c})\) For a state of nonzero orbital angular momentum, find the maximum and minimum values of \(\sqrt{L_{x}^{2}+L_{y}^{2}}\) . Explain your results.

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