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The Bohr's energy of a stationary state of hydrogen atom is given as \(E_{n}=\frac{-2 \pi^{2} m e^{4}}{n^{2} h^{2}}\). Putting the values of \(m\) and \(e\) for \(n^{\text {th }}\) energy level which is not the correct value? (a) \(E_{n}=\frac{-21.8 \times 10^{-19}}{n^{2}} \mathrm{~J}\) atom \(^{-1}\). (b) \(E_{n}=\frac{-13.6}{n^{2}} \mathrm{eV}\) atom \(^{-1}\) (c) \(E_{n}=\frac{-1312}{n^{2}} \mathrm{~kJ} \mathrm{~mol}^{-1}\) (d) \(E_{n}=\frac{-12.8 \times 10^{-19}}{n^{2}}\) erg \(\mathrm{atom}^{-1}\)

Short Answer

Expert verified
(d) \(-12.8 \times 10^{-19}\) erg atom\(^{-1}\) is not the correct value.

Step by step solution

01

- Understanding Bohr's energy formula

The formula given, \(E_{n}=\frac{-2 \pi^{2} me^{4}}{n^{2}h^{2}}\), represents the energy of an electron in the nth energy level of a hydrogen atom in the Bohr model. The formula includes Planck's constant (h), the mass of an electron (m), the charge of an electron (e), and the principle quantum number (n).
02

- Calculation for the correct value

To find the correct value, substitute the constants into the formula. We need the values of the mass of an electron (\(m\)) which is approximately \(9.11 \times 10^{-31} \) kg, the charge of an electron (\(e\)) \(1.6 \times 10^{-19} \) C, Planck's constant (\(h\)) \(6.626 \times 10^{-34} \) Js, and the value of \(\pi\).
03

- Conversion of units

To check the validity of the given options, we may need to convert the resulting energy from Joules to electronvolts (eV), kilojoules per mole (kJ/mol), and ergs to match the given units.
04

- Evaluate the options

Calculate the energy using Bohr's formula and convert the units to compare with the given options. If an option's numerical coefficient doesn't match the calculated value after simplifying and converting units, it is incorrect. The conversion factors are: \(1\) eV \(= 1.602 \times 10^{-19}\) J, \(1\) erg \(= 10^{-7}\) J, and \(1\) kJ/mol is \(\frac{10^{3}}{N_{A}}\) J per atom, where \(N_{A}\), Avogadro's number, is \(6.022 \times 10^{23}\) mol\(^{-1}\).
05

- Identify the incorrect value

Using the constants provided, the energy for one atom is approximately \(-13.6\) eV when converted from Joules. This matches option (b). When using the conversions, if one of the provided options doesn't align with this value, it will be identified as incorrect.

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Key Concepts

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

Hydrogen Atom Energy Levels
Understanding the energy levels of a hydrogen atom is essential for comprehending the behavior of electrons in atoms. The energy levels, or orbits, in a hydrogen atom are quantized, meaning electrons can only exist at certain discrete energy levels.

The simplest atom, hydrogen, has one electron surrounding the nucleus, and according to Niels Bohr's model, this electron can occupy certain permitted orbits. Each orbit corresponds to a specific energy level, denoted by the principal quantum number, 'n'. As 'n' increases, the electron's energy also increases, and it resides further from the nucleus.

Calculating Energy Levels

Using Bohr's formula, En = -13.6 eV/n^2, we can calculate the energy of an electron at any given level 'n'. For example, the first energy level (n=1) has an energy of -13.6 eV, the second (n=2) has an energy of -3.4 eV, indicating that electrons require energy to move to higher levels. When they drop to lower energy levels, they emit energy in the form of electromagnetic radiation.

This quantization explains the distinct lines observed in the atomic emission spectra and is fundamental to understanding atomic and quantum physics.
Planck's Constant
Planck's constant is a significant number in quantum mechanics. Named after physicist Max Planck, it represents the quantization of energy in mathematical form and is denoted by the symbol 'h'.

The Role in Quantum Mechanics

Planck's constant links the energy (E) of a photon and the frequency (f) of its electromagnetic wave through the relation E = hf. This constant sets the scale for the quantum world and is critical in the formula for calculating the energy levels of the hydrogen atom.

The value of Planck's constant is approximately 6.626 x 10^-34 Js (Joule seconds), underscoring the very subtle action scales in quantum phenomena. It is this 'magic number' that made the connection between the macroscopic and quantum worlds and paved the way for the development of Quantum Mechanics.
Electron Charge
The charge of an electron is one of the fundamental properties of particles in the universe. Representing a basic unit of electric charge, the electron charge is a constant and is denoted by 'e'.

Importance of Electron Charge in Formulas

In Bohr's energy formula, the electron charge appears as e^4, highlighting its pivotal role in determining the energy of hydrogen atom orbits. The magnitude of a single electron charge is approximately 1.6 x 10^-19 Coulombs (C), which is negative, indicating that an electron has a negative charge.

This constant is fundamental in many equations and laws across physics, including the classical Coulomb's law, which describes the electrostatic force between two charged particles, and in defining the ampere, the standard unit of current in the International System of Units (SI).
Quantum Numbers
Quantum numbers are sets of numerical values that provide detailed information about the energy and position of an electron within an atom. They are crucial for the understanding of the arrangement of electrons in atoms, known as the electron configuration.

Types of Quantum Numbers

There are four types of quantum numbers:
  • The principal quantum number, 'n', describes the energy level of an electron in an atom.
  • The azimuthal quantum number, 'l', defines the shape of the electron's orbital.
  • The magnetic quantum number, 'm_l', specifies the orientation of the orbital in space.
  • The spin quantum number, 'm_s', describes the electron's spin direction in the magnetic field.

In the context of the Bohr model, the principal quantum number 'n' determines the energy of an electron in a specific orbit. As 'n' increases, so does the electron's energy and average distance from the nucleus. Each value of 'n' corresponds to a 'shell' or energy level in the atom where an electron can be found.

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Most popular questions from this chapter

The energy difference between the ground state of an atom and its excited state is \(3 \times 10^{-19} \mathrm{~J}\). What is the wavelength of the photon required for this transition? (a) \(6.6 \times 10^{-34} \mathrm{~m}\) (b) \(3 \times 10^{-8} \mathrm{~m}\) (c) \(1.8 \times 10^{-7} \mathrm{~m}\) (d) \(6.6 \times 10^{-7} \mathrm{~m}\)

Electromagnetic radiation of wavelength \(242 \mathrm{~nm}\) is just sufficient to ionise the sodium atom. What is the ionisation energy of sodium per atom? (a) \(494.5 \times 10^{-6} \mathrm{~J} /\) atom (b) \(8169.5 \times 10^{-10} \mathrm{~J} /\) atom (c) \(5,85 \times 10^{-15} \mathrm{~J} /\) atom (d) \(8.214 \times 10^{-19} \mathrm{~J} / \mathrm{atom}\)

An element with mass number 81 contains \(31.7 \%\) more neutrons as compared to protons. Find the symbol of the atom. (a) \({ }_{3}^{81} \mathrm{Se}\) (b) \({ }_{35}^{81} \mathrm{Br}\) (c) \({ }_{36}^{81} \mathrm{Kr}\) (d) \({ }_{37}^{81} \mathrm{Rb}\)

Match the values of column II with column \(\mathrm{I}\) and mark the appropriate choice. $$ \begin{array}{|l|l|l|l|} \hline {\text { Column I }} & && {\text { Column II }} \\ \hline \text { (A) } & \begin{array}{l} \text { The shape of rubber heel } \\ \text { changes under stress } \end{array} & \text { (p) } & \begin{array}{l} \text { Young's } \\ \text { modulus of } \\ \text { elasticity is } \\ \text { involved } \end{array} \\ \hline \text { (B) } & \begin{array}{l} \text { In a suspended bridge, } \\ \text { there is a strain in the } \\ \text { ropes by the load of the } \\ \text { bridge } \end{array} & \text { (q) } & \begin{array}{l} \text { Bulk modulus } \\ \text { of elasticity is } \\ \text { involved } \end{array} \\ \hline \text { (C) } & \begin{array}{l} \text { In an automobile tyre, } \\ \text { when air is compressed, } \\ \text { the shape of tyre changes } \end{array} & \text { (r) } & \begin{array}{l} \text { Modulus of } \\ \text { rigidity is } \\ \text { involved } \end{array} \\ \hline \text { (D) } & \begin{array}{l} \text { A solid body is subjected } \\ \text { to a deforming force } \end{array} & \text { (s) } & \begin{array}{l} \text { All the moduli } \\ \text { of elasticity } \\ \text { are involved } \end{array} \\ \hline \end{array} $$ (a) \((A) \rightarrow(i),(B) \rightarrow(i i),(C) \rightarrow(\) iv),\((D) \rightarrow(\) iii) (b) (A) \(\rightarrow\) (iii), (B) \(\rightarrow\) (i), (C) \(\rightarrow\) (ii), (D) \(\rightarrow\) (iv) (c) (A) \(\rightarrow\) (ii), (B) \(\rightarrow\) (iii), (C) \(\rightarrow\) (iv), (D) \(\rightarrow\) (i) (d) \((\mathrm{A}) \rightarrow(\mathrm{i}),(\mathrm{B}) \rightarrow\) (iii), (C) \(\rightarrow\) (ii), (D) \(\rightarrow\) (iv)

Which of the following observations was not correct during Rutherford's scattering experiment? (a) Most of the \(\alpha\)-particles passed through the gold foil undeflected. (b) A small fraction of the \(\alpha\)-particles was deflected by small angles. (c) A large number of the \(\alpha\)-particles were bounced back. (d) A very few \(\alpha\)-particles \((-1\) in 20,000\()\) were bounced back.

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