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

  1. What are the initial and final energy levels for the third (i.e., third-longest wavelength) line in the Paschen series? (See Figure 7.5)
  2. Determine the wavelength of this line.

Short Answer

Expert verified

(a) Energy of initial state is -0.378eVand Energy of final state -1.512eV.

(b) Wavelength of the third line of the Paschen series is 1.1x10-6m.

Step by step solution

01

The Paschen series:

The Paschen series is a set of emission lines from atomic hydrogen gas due to electrons descending from an electron shell with n greater than 3 up to n = 3, or analogous absorption lines when absorbed electromagnetic radiation causes the electrons to do the opposite.

02

(a) Initial and final energy levels of the third line in the Paschen series:

All the spectrum lines which originate on n = 4,5,6,7,... and end at n = 3 are said to be in the Paschen series of Spectral lines. Where, n is the principal quantum number.

As you know, the third line of the Paschen series has an initial state, n = 6, and the final state as n = 3.

You also know that Energies of different quantized levels of the hydrogen atom can be given by

En=-13.6eV32n=1,2,3,....

Now, energy of initial state (n = 6) :

E6=-13.6eV62=-0.378eV

Now, energy of final state ( n = 3) :

E6=-13.6eV32=-1.512eV

03

(b) Wavelength of 6→3  transition:

As you know that, energy of photon emitted during 63transition is given by,

EPhoton=E6-E3=-0.378eV--1.512eV

EPhoton=1.13eV ….. (1)

You also know that, energy of emitted photon is given by

E=hcλ ….. (2)

Where, h is Plank’s constant, c is the speed of light, λis the wavelength of the photon.

Now, by using equation (1) and equation (2), you get,

1.13eV=1240eVnmλλ=1.1×10-6m

Hence, wavelength of the required third line of the Paschen series will be λ=1.1×10-6m.

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

How many different 3d states are there? What physical property (as opposed to quantum number) distinguishes them, and what different values may this property assume?

For states where l = n - t the radial probability assumes the general form given in Exercise 54. The proportionality constant that normalizes this radial probability is given in Exercise 64.

(a) Show that the expectation value of the hydrogen atom potential energy is exactly twice the total energy. (It turns out that this holds no matter what l may be)

(b) Argue that the expectation value of the kinetic energy must be the negative of the total energy.

The Diatomic Molecule: Exercise 80 discusses the idea of reduced mass. Classically or quantum mechanically, we can digest the behavior of a two-particle system into motion of the center of mass and motion relative to the center of mass. Our interest here is the relative motion, which becomes a one-particle problem if we merely use μfor the mass for that particle. Given this simplification, the quantum-mechanical results we have learned go a long way toward describing the diatomic molecule. To a good approximation, the force between the bound atoms is like an ideal spring whose potential energy is 12kx2, where x is the deviation of the atomic separation from its equilibrium value, which we designate with an a. Thus,x=r-a . Because the force is always along the line connecting the two atoms, it is a central force, so the angular parts of the Schrödinger equation are exactly as for hydrogen, (a) In the remaining radial equation (7- 30), insert the potential energy 12kx2and replace the electron massm with μ. Then, with the definition.f(r)=rR(r), show that it can be rewritten as

-ħ22μd2dr2f(r)+ħ2I(I+1)2μr2f(r)+12kx2f(r)=Ef(r)

With the further definition show that this becomes

-ħ22μd2dx2g(x)+ħ2I(I+1)2μ(x+a)g(x)+12kx2g(x)=Eg(x)

(b) Assume, as is quite often the case, that the deviation of the atoms from their equilibrium separation is very small compared to that separation—that is,x<<a. Show that your result from part (a) can be rearranged into a rather familiar- form, from which it follows that
E=(n+12)ħkμ+ħ2I(I+1)2μa2n=0,1,2,...I=0,1,2,...

(c)

Identify what each of the two terms represents physically.

The space between two parallel metal plates is filled with an element in a gaseous stale. Electrons leave one plate at negligible speed and are accelerated toward the other by a potential differenceVapplied between the plates. As Vis increased from 0, the electron current increases more or less linearly, but when Vreaches 4.9 V , the current drops precipitously. From nearly 0 , it builds again roughly linearly as Vis increased beyond 4.9 V .

(a) How can the presence of the gas explain these observations?

(b) The Gas emits pure “light” when Vexceeds 4.9 V . What is its wavelength?

An electron is trapped in a quantum dot, in which it is continued to a very small region in all three dimensions, If the lowest energy transition is to produce a photon of 450nm wavelength, what should be the width of the well (assumed cubic)?

See all solutions

Recommended explanations on Physics 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