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

Doubly ionized lithium, Li2+absorbs a photon and jumps from the ground state to its n=2level. What was the wavelength of the photon?

Short Answer

Expert verified

When, doubly ionized lithium,Li2+ absorbs a photon and jumps from the ground state to its n=2 level, the wavelength of the photon 13.5 nm.

Step by step solution

01

Finding absorbed energy by the ion:

Whenever an electron absorbs energy enough for it to transition to higher state, it jumps to the higher state, and it loses energy while jumping down to the lower state from the higher state.

As you know that, energy of an electron in its nth orbit is given by

En=-z213.6eVn2(n=1,2,3...........)

Where, z

is the atomic number of hydrogen-like atom and n

is the principal quantum number.

Hence, if the ion jumps from ground state to n=2 , the energy will be,

E2-E1=32-13.6eV2232--13.6eV12=91.8eV=1.47×10-17J

02

Finding wavelength of the photon

Energy of the photon is given by,

E=hcλ.......(1)

Here, h is the Planck’s constant, c is the speed of light, and λis the wavelength.

The numerical value of hc is,

hc = 1240 eV .nm

Substitute known values into equation (1), and you have

91.8eV=1240eV.nmλλ=13.5nm

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

Question: Show that the angular normalization constant in Table 7.3 for the case (l,ml)=(1,0) is correct.

We have noted that for a given energy, as lincreases, the motion is more like a circle at a constant radius, with the rotational energy increasing as the radial energy correspondingly decreases. But is the radial kinetic energy 0 for the largest lvalues? Calculate the ratio of expectation values, radial energy to rotational energy, for the(n,l,mt)=(2.1,+1)state. Use the operators

KErad=-h22m1r2r(rr)KErad=h2l(l+1)2mr2

Which we deduce from equation (7-30).

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.

Consider two particles that experience a mutual force but no external forces. The classical equation of motion for particle 1 is v˙1=F2on1/m1, and for particle 2 is v˙2=F1on2/m2, where the dot means a time derivative. Show that these are equivalent to v˙cm=constant, and v˙rel=FMutual/μ .Where, v˙cm=(m1v˙1+m2v˙2)/(m1m2),FMutual=-Fion2andμ=m1m2(m1+m2).

In other words, the motion can be analyzed into two pieces the center of mass motion, at constant velocity and the relative motion, but in terms of a one-particle equation where that particle experiences the mutual force and has the “reduced mass” μ.

A hydrogen atom electron is in a 2p state. If no experiment has been done to establish a z-component of angular momentum, the atom is equally likely to be found with any allowed value of LZ. Show that if the probability densities for these different possible states are added (with equal weighting), the result is independent of both ϕandθ

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