X Rays and the Ordering of the Elements — Question 3

Section 40-9 · Physics pages 6736–6737

Question 3 Moseley scaling identifies an element through its nuclear charge Use the approximate Kα law Eα = C(Z −1)2, where C is the same for two neighboring targets. For target A, ZA = 25 and EA = 6.00 keV. Target B has EB = 6.5104167 keV within the precision of this model. Z √Eα 1 Schematic; labels, not drawing lengths, specify the data. (a) Infer ZB. (b) Find C and predict the line energy for Z = 27.
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Question 3 - Solution Moseley scaling identifies an element through its nuclear charge Z √Eα 1 (a) Method and calculation √ EB/EA = ZB −1 ZA −1 ⇒ZB = 1 + 24 √ 6.5104167/6.00. ZB ≃26 . (b) Interpretation and further calculation C = 6.00/242 = .0104167 keV . Eα(27) = C(26)2 = 7.04167 keV . Physical check The model orders elements by atomic number rather than mean atomic mass. Screening and relativistic corrections limit its accuracy; inferred integer Z should be judged against those model uncertainties.

Question 3

Moseley scaling identifies an element through its nuclear charge

Use the approximate KαK_\alpha law Eα=C(Z−1)2E_\alpha=C(Z-1)^2, where C is the same for two neighboring targets. For target A, ZA=25Z_A=25 and EA=6.00keVE_A=6.00\,\mathrm{keV}. Target B has EB=6.5104167keVE_B=6.5104167\,\mathrm{keV} within the precision of this model.

Diagram shown in the original SVG worksheet.

  1. Infer ZBZ_B.

  2. Find C and predict the line energy for Z=27Z=27.

Question 3 - Solution

Moseley scaling identifies an element through its nuclear charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

EB/EA=ZB−1ZA−1⇒ZB=1+246.5104167/6.00.\sqrt{E_B/E_A}=\frac{Z_B-1}{Z_A-1}\Rightarrow Z_B=1+24\sqrt{6.5104167/6.00}.ZB≃26.\boxed{Z_B\simeq26}.

(b) Interpretation and further calculation

C=6.00/242=.0104167keV.\boxed{C=6.00/24^2=.0104167\,\mathrm{keV}}.Eα(27)=C(26)2=7.04167keV.\boxed{E_\alpha(27)=C(26)^2=7.04167\,\mathrm{keV}}.

Physical check

The model orders elements by atomic number rather than mean atomic mass. Screening and relativistic corrections limit its accuracy; inferred integer Z should be judged against those model uncertainties.