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The Kαline in copper is a very common one to use in X-ray crystallography. To produce it, electrons are accelerated through a potential difference and smashed into a copper target. Section 7.8 gives the energies in a hydrogen like atom asZ2(-13.6eV/n2) . Making the reasonable approximation that ann=1 electron in copper orbits the nucleus and half of its fellow n=1electron, being unaffected by the roughly spherical cloud of other electrons around it. Estimate the minimum accelerating potential needed to make a hole in copper'sKshell.

Short Answer

Expert verified

The resultant answer is11kV

Step by step solution

01

Given data

The given data isKα line in copper is used in x-ray.

02

Concept of Energy

The energyEof the emitted ray is inversely proportional to the wavelengthλ:

E~1λ

03

Determine the charge

Since a copper nucleus has 29 protons, its charge will be +29.

However, when the K-shell electron is ejected it sees half of the other K-shell electron screening the nucleus.

That will thus make the effective charge that the ejected electron sees as +28.5.

That is used in equationE=Z2-13.6eVn2 for Z, along with 1 for (since it's the K-shell):

E=Z2-13.6eVn2E=(28.5)2-13.6eV(1)2E=-11046.6eV

In order for the electron to be ejected, the sum of that and the kinetic energy of the accelerated electron have to be at least zero.

0<KE+E0<qΔV-11046.6eVqΔV-11046.6eV

And since it's an electron that was accelerated, the charge q will be the elementary unit of charge q

11046.6eV<qΔV11046.6eV<(e)ΔV11046.6eV<ΔV

The electrons were able to drop out due to the definition of one VV being the energy that an electron gains by passing through a potential difference of one Volt.

So, the potential difference that the X-ray electron would have to be accelerated through is shown below.

ΔV=11,000VΔV=11,000V1kV1000VΔV=11kV

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Most popular questions from this chapter

Whether adding spins to get total spin, spin and orbit to get total angular momentum, or total angular momenta to get a "grand total" angular momentum, addition rules are always the same: Given J1=j1(j1+1)andJ2=j2(j2+1) . Where is an angular momentum (orbital. spin. or total) and a quantum number. the total isJT=jT(jT+1) , where jTmay take on any value between |j1-j2|and j1+j2in integral steps: and for each value ofJΓJTz=mπf . where mπmay take on any of2jr+I possible values in integral steps from-jT for +jTSince separately there would be 2j1+1possible values form11 and2j2+ I formρ2 . the total number of stales should be(2j1+1)(2j2+1) . Prove it: that is, show that the sum of the2jT+1 values formit over all the allowed values forj7 is (2j1+1)(2j2+1). (Note: Here we prove in general what we verified in Example 8.5for the specialcase j1=3,j2=12.)

Verify that the normalization constant given in Example 8.2is correct for both symmetric and antisymmetric states and is independent ofnand n'?

Question: Early on, the lanthanides were found to be quite uncooperative when attempts were made to chemically separate them from one another. One reason can be seen in Figure 8.16. Explain.

Using a beam of electrons accelerated in an X-ray tube, we wish to knock an electron out of the shell of given element in a target. Section \(7.8\) gives the energies in a hydrogen like atom as . Z2(-13.6eV/n2)Assume that for fairly high Z , aK-shell electron can be treated as orbiting the nucleus alone.

(a) A typical accelerating potential in an X-ray tube is50kV . In roughly how high aZcould a hole in the K -shell be produced?

(b) Could a hole be produced in elements of higher Z?

The radius of cesium is roughly0.26nm.

(a) From this estimate the effective charge its valence electron orbits

(b) Given the nature of the electron's orbit. is this effective nuclearcharge reasonable?

(c) Compare this effective Zwith that obtained for sodium in Example 8.3. Are the values at odds with the evidence given in Figure8.16that it takes less energy to remove an electron from cesium than from sodium? Explain.

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