Nuclear Fission: The Basic Process — Question 1

Section 43-1 · Physics pages 7152–7153

Question 1 Conservation identifies the missing fragment in a fission channel An illustrative channel is 235 92 U + n →141 56 Ba + A ZX + 3n. Subsequent beta-minus decays change nuclear charge without changing A. n fragment 1 fragment 2 Schematic; labels, not drawing lengths, specify the data. (a) Identify A, Z and the element X (Z=36 is krypton). (b) If the A=141 fragment undergoes three beta-minus decays, write the net nuclear and lepton bookkeeping.
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Question 1 - Solution Conservation identifies the missing fragment in a fission channel n fragment 1 fragment 2 (a) Method and calculation 235 + 1 = 141 + A + 3 ⇒A = 92 . 92 = 56 + Z ⇒Z = 36, X = 92 36Kr . (b) Interpretation and further calculation 141 56 Ba →141 59 Pr + 3e−+ 3¯νe . Qcharge : 56 = 59 −3; L : 0 = 3 −3. Physical check Fission produces a distribution of channels. Mass number counts nucleons, not rest mass, so its conservation does not imply zero released energy.

Question 1

Conservation identifies the missing fragment in a fission channel

An illustrative channel is 92235U+n→56141Ba+ZAX+3n^{235}_{92}\mathrm U+n\to{}^{141}_{56}\mathrm{Ba}+{}^{A}_{Z}X+3n. Subsequent beta-minus decays change nuclear charge without changing A.

Diagram shown in the original SVG worksheet.

  1. Identify A, Z and the element X (Z=36 is krypton).

  2. If the A=141 fragment undergoes three beta-minus decays, write the net nuclear and lepton bookkeeping.

Question 1 - Solution

Conservation identifies the missing fragment in a fission channel

Diagram shown in the original SVG worksheet.

(a) Method and calculation

235+1=141+A+3⇒A=92.235+1=141+A+3\Rightarrow\boxed{A=92}.92=56+Z⇒Z=36,X=3692Kr.92=56+Z\Rightarrow\boxed{Z=36,\quad X={}^{92}_{36}\mathrm{Kr}}.

(b) Interpretation and further calculation

56141Ba→59141Pr+3e−+3ν‾e.\boxed{{}^{141}_{56}\mathrm{Ba}\to{}^{141}_{59}\mathrm{Pr}+3e^-+3\bar\nu_e}.Qcharge:56=59−3;L:0=3−3.Q_{\mathrm{charge}}:\ 56=59-3;\qquad L:\ 0=3-3.

Physical check

Fission produces a distribution of channels. Mass number counts nucleons, not rest mass, so its conservation does not imply zero released energy.