Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

The energy of electron in the \(\mathrm{n}^{\text {th }}\) orbit of hydrogen atom is expressed as \(E_{n}=-\left[(13.6) / \mathrm{n}^{2}\right] e v .\) The shortest and longest wave length of lyman series will be. (A) \(912 \bar{\AA}, 1216 \AA\) (B) \(1315 \AA, 1530 \AA\) (C) \(5463 \AA, 7858 \AA\) (D) None of these

Short Answer

Expert verified
The shortest and longest wavelengths of the Lyman series are approximately \(912 \mathring{A}\) and \(1216 \mathring{A}\), respectively, which corresponds to answer choice (A).

Step by step solution

01

Calculate the energy difference between the energy levels

For the shortest and longest wavelength in Lyman series, we consider the transitions from orbit n = 2 to n = 1 (longest wavelength) and n = ∞ to n = 1 (shortest wavelength). Let's find the change in energy for these transitions: For n = 2 to n = 1: ΔE₁ = |E₂ - E₁| = \(\left|\frac{-13.6}{2^2} - \frac{-13.6}{1^2}\right|\) eV For n = ∞ to n = 1: ΔE₂ = |E_∞ - E₁| = \(\left|\frac{-13.6}{\infty^2} - \frac{-13.6}{1^2}\right|\) eV
02

Convert energy difference to wavelength

Next, we need to convert the energy differences ΔE₁ and ΔE₂ to wavelengths using the formula: ΔE = h\(\frac{c}{\lambda}\), where ΔE is the change in energy, h is Planck's constant (4.136 × 10⁻¹⁵ eV·s), and c is the speed of light (3 × 10⁸ m/s). Longest wavelength (n = 2 to n = 1): \(\lambda_1 = \frac{hc}{\Delta E_1}\) Shortest wavelength (n = ∞ to n = 1): \(\lambda_2 = \frac{hc}{\Delta E_2}\)
03

Calculate the wavelengths and convert to Ångströms

Calculate the shortest and longest wavelengths using the energy differences obtained in step 1: Longest wavelength (n = 2 to n = 1): \(\lambda_1 = \frac{(4.136 \times 10^{-15})(3 \times 10^8)}{\Delta E_1}\) Shortest wavelength (n = ∞ to n = 1): \(\lambda_2 = \frac{(4.136 \times 10^{-15})(3 \times 10^8)}{\Delta E_2}\) Finally, convert these wavelengths from meters to Ångströms by multiplying by \(10^{10}\): \(\lambda_1 \times 10^{10} = \) Longest wavelength in Ångströms \(\lambda_2 \times 10^{10} = \) Shortest wavelength in Ångströms After calculating the values, we find that the shortest and longest wavelengths of the Lyman series are approximately \(1216 \mathring{A}\) and \(912 \mathring{A}\), respectively. This corresponds to the answer choice (A) \(912 \mathring{A}, 1216 \mathring{A}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

It the radius of a nucleus of mass number 3 is \(\mathrm{R}\). then the radius of a nucleus of mass number 81 is (A) \(27 \mathrm{R}\) (B) \(9 \mathrm{R}\) (C) \(3 \mathrm{R}\) \((\mathrm{D})(27)^{(1 / 2)} \mathrm{R}\)

The radius of Ge nucleus is measured to be twice the radius of ${ }^{9}{ }_{4}$ Be. The number of nucleons in Ge are (A) 72 (B) 78 (C) 65 (D) 80

In each of the following question match column -I and column -II. Select correct Answer. (a) Bohr atom model (p) fixed for the atom (b) Ionization potential (q) Nucleus (c) Rutherford atom model (r) stationary orbits (d) Thomson atom model (s) In atom positive and Negative charge are distributed uniformly (A) $\mathrm{a} \rightarrow \mathrm{s}, \mathrm{b} \rightarrow \mathrm{r}, \mathrm{c} \rightarrow \mathrm{q}, \mathrm{d} \rightarrow \mathrm{p}$ (B) $\mathrm{a} \rightarrow \mathrm{r}, \mathrm{b} \rightarrow \mathrm{p}, \mathrm{c} \rightarrow \mathrm{q}, \mathrm{d} \rightarrow \mathrm{s}$ (C) $\mathrm{a} \rightarrow \mathrm{p}, \mathrm{b} \rightarrow \mathrm{r}, \mathrm{c} \rightarrow \mathrm{s}, \mathrm{d} \rightarrow \mathrm{q}$ (D) $\mathrm{b} \rightarrow \mathrm{p}, \mathrm{c} \rightarrow \mathrm{q}, \mathrm{b} \rightarrow \mathrm{r}, \mathrm{d} \rightarrow \mathrm{s}$

The half time of a radioactive substance is \(20 \mathrm{~min}\), difference between Points of time when it is \(33 \%\) disintegrated and \(67 \%\) disintegrated is approximately (A) \(10 \mathrm{~min}\) (B) \(20 \mathrm{~min}\) (C) \(40 \mathrm{~min}\) (D) \(30 \mathrm{~min}\)

A nucleus with \(\mathrm{Z}=92\) emits the following sequence $\alpha, \alpha, \beta^{-}\( \)\beta^{-}, \alpha, \alpha, \alpha, \alpha, \beta^{-}, \beta^{-}, \alpha, \beta^{+}, \beta^{+}, \alpha\( The \)\mathrm{Z}$ of the resulting nucleus is (A) 76 (B) 78 (C) 74 (D) 82

See all solutions

Recommended explanations on English Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free