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Solutions Manual for Radiation Detection and Measurement, 4th Edition by Knoll (All 20 Chapters)

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This comprehensive Solutions Manual accompanies the classic textbook Radiation Detection and Measurement, 4th Edition, by Glenn F. Knoll. Prepared to provide complete, step-by-step solutions to all end-of-chapter problems, this manual is an essential resource for mastering the principles of nuclear radiation detectors and measurement systems. What's included: Complete solutions for all 20 chapters Detailed problem-solving approaches covering: Radiation sources, interactions, and energy spectra Gas-filled detectors (ion chambers, proportional counters, GM tubes) Scintillation detectors and PM tubes Semiconductor detectors (Si, Ge, Si(Li), HPGe) Pulse processing, shaping, and MCA electronics Counting statistics, error propagation, and MDA calculations Time measurements, coincidence techniques, and dead time models Neutron detectors, Cherenkov detectors, and special systems Background, shielding, and activation analysis Why this manual helps you: Verify homework answers with confidence Learn correct methodology for radiation detection problems Master complex topics like Fano factor, charge collection, and resolution Save hours of study time preparing for exams Understand detector selection, efficiency calculations, and spectroscopy Whether you're studying health physics, nuclear engineering, or medical physics, this manual gives you the clarity you need to succeed. Instant digital download – start studying immediately!

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All 20 Chapters Covered
o o o




SOLUTION MANUAL
o

, Chaptero 1o Solutions




Radiationo Sources


■ Problemo1.1.o RadiationoEnergyoSpectra:oLineovs.oContinuous

Lineo(orodiscreteoenergy):oa,oc,od,oe,of,oandoi.oContinuo
usoenergy:ob,og,oandoh.


■ Problemo1.2.o Conversionoelectronoenergiesocompared.

Sinceotheoelectronsoinoouteroshellsoareo boundolessotightlyothanothoseoinocloseroshells,oconversionoelectronsofromoouteroshellsowillo ha
veogreateroemergingoenergies.o Thus,otheoMoshelloelectronowilloemergeowithogreateroenergyothanoaoKooroLoshelloelectron.


■ Problemo1.3.o Nuclearodecayoandopredictedoenergies.

Weowriteotheoconservationoofoenergyoandomomentumoequationsoandosolveothemoforotheoenergyoofotheoalphaoparticle.o Momentumois
ogiven otheosymbolo"p",o andoenergyois o"E".o Forotheosubscripts,o"al"ostandsoforoalpha,owhileo"b"odenotesotheodaughteronucleus.


pal2 pb2
paloo pbooo0 E
o al oEb Ealoo Ebo oQ and Qoo5.5oMeV
2omal 2omb

Solvingoourosystemoofoequationsoforo Eal,o Eb,o pal,o pb,o weogetotheosolutionsoshownobelow.o Noteothatoweohaveotwoopossibleosetsoofosolutio
nso(thisodoesonotoeffectotheofinaloresult).
mal 5.5omalo
Ebo o5.5o 1o Ealo
maloomb maloomb

3.31662 mal mb 3.31662 mal mb
paloo pboo
maloomb maloomb

Weoareointerestedoinofindingotheoenergyoofotheoalphaoparticleoinothisoproblem,oandosinceoweoknowotheomassoofotheoalphaoparticleoan
dotheo daughtero nucleus,o theo resulto iso easilyo found.o Byosubstitutingoouro knownovalueso ofo maloo4o ando mboo206o intoo ouro derivedoEa
lequationoweoget:



Ealoo5.395oMeV


Noteo:oWeocanoobtainosolutionsoforoallotheovariablesobyosubstitutingomboo206oandomaloo4ointootheoderivedoequationsoaboveo:

Ealoo5.395oMeV Eboo0.105oMeV palooo6.570 amuoMeV pbo oo6.570 amuoMeV


■ Problemo1.4.o Calculationoofo WavelengthofromoEnergy.

Sinceoanox-rayomustoessentiallyobeocreatedobyotheode-excitationoofoaosingleoelectron,otheomaximumoenergyoofoanox-
rayoemittedoinoaotubeooperatingoatoaopotentialoofo195okVomustobeo195okeV.o Therefore,o weocanouseotheoequationoE=h,owhichoisoalso
oE=hc/Λ,ooroΛ=hc/E.o Pluggingoinoouromaximumoenergyovalueointoothisoequationogivesotheominimumox-rayowavelength.


hooc
Λo whereoweosubstituteohoo 6.626oo1034oJoos,o coo299o792o458omoosoandoEoo195okeV
E




1

, Chaptero 1o Solutions




1.01869oJ–m
Λo o 0.0636oAngstroms
KeV



■ Problemo 1.5.o o 235oUFissiono EnergyoRelease.
235 117
Usingotheo reactiono o Uo o o o Snoo118oSn,o andomassovalues,oweocalculateo theomassodefecto of:

Mo235oUoo o Mo117oSnooMo118oSnoo M
oandoan oexpectedoenerg



yoreleaseoofoMc2.

931.5oMeV
oo oo oo o223o MeV
AMU

Thiso iso oneoofotheo mostoexothermicoreactionso availableo toous.o Thiso iso oneoreasono why,oofocourse,o nuclearo powerofromouraniumofis
sionoisosooattractive.


■ Problemo1.6.o SpecificoActivityoofo Tritium.

Here,oweouseotheotextoequationoSpecificoActivityo=o(ln(2)*Av)/oT12*M),owhereoAvoisoAvogadro'sonumber,oT12oisotheohalf-
lifeoofotheoisotope,oandoMoisotheomolecularoweightoofotheosample.
ln2oAvogadroo'osoConstant
SpecificoActivityo
T12oM
3ograms
WeosubstituteoT12oo12.26oyearsoandoM= toogetotheospecificoactivityoinodisintegrations/(gram–year).
mole

1.13492oo1022
SpecificoActivityo
gramo–year

TheosameoresultoexpressedoinotermsoofokCi/goisoshownobelow

9.73okCi
SpecificoActivityo
gram



■ Problemo1.7.o Acceleratedoparticleoenergy.

Theo energyoofoao particleo withochargeo qofallingothroughoao potentialoVo isoqV.o Sinceo V=o 3oMVo isoouromaximumopotentialodifference,o theo
maximumoenergyoofo ano alphao particleo hereo iso q*(3o MV),o whereo qo iso theo chargeo ofo theo alphao particleo (+2).o Theomaximumoalphaoparticl
eoenergyoexpressedoinoMeVoisothus:

Energyoo3oMegaoVoltsoo2oElectronoChargeso o6.o MeV




2

, Chaptero 1o Solutions




■ Problemo1.8.o Photofissionoofo deuterium. 1oDo o Γo
2 1
0ono
1
1opo+o Qo (-2.226oMeV)

Theo reactionoofointerestoiso o 2oDo o o 0oΓo o 1onoo o 1o p+oQo(-2.226oMeV).o Thus,otheoΓomustobringoanoenergyoofoatoleasto2.226oMeV
1 0 0 1
inoorderoforothisoendothermicoreactionotooproceed.o Interestingly,otheooppositeoreactionowillobeoexothermic,oandooneocanoexpectotoofi
ndo2.226oMeVogammaoraysoinotheoenvironmentofromostrayoneutronsobeingoabsorbedobyohydrogenonuclei.


■ Problemo1.9.o NeutronoenergyofromoD-Toreactionobyo150okeVodeuterons.

Weowriteodownotheoconservationoofoenergyoandomomentumoequations,oandosolveothemoforotheodesiredoenergiesobyoeliminatingotheo
momenta.o Inothisosolution,o"a"orepresentsotheoalphaoparticle,o"n"orepresentsotheoneutron,oando"d"orepresentsotheodeuterono(and,oasob
efore,o"p"orepresentsomomentum,o"E"orepresentsoenergy,oando"Q"orepresentsotheoQ-valueoofotheoreaction).

pa2 pn2 pdo2
paoo pnoo pd E
o a E
o n Ed
o EaooEnooEdo oQ
2oma 2omn 2omd

Nexto weo wanto too solveotheo aboveo equationso foro theo unknownoenergieso byoeliminatingotheo momenta.o (Noteo :o Usingo computeros
oftwareosuchoasoMathematicaoisohelpfuloforopainlesslyosolvingotheseoequations).

Weo evaluateo theo solutionobyopluggingoino theo valuesoforo particleo masseso(weo useo approximateovaluesoofo "ma,"o "mn,"ando "md"o ino
AMU,owhichoisookayobecauseoweoareointerestedoinoobtainingoanoenergyovalueoatotheoend).o WeodefineoalloenergiesoinounitsoofoMeV,on
amelyotheo Q-value,oandotheo givenoenergyoofotheodeuterono(bothoenergyovaluesoareo inoMeV).o o Sooweosubstituteomao =o4,omno =o1,omd
=o2,oQo=o17.6,oEdo =o0.15ointooouromomentaoindependentoequations.o Thisoyieldsotwoopossibleosetsoofosolutionsoforotheoenergieso(ino
MeV).oOneocorrespondsotootheoneutronomovingoinotheoforwardodirection,owhichoisoofointerest.
Enoo 13.340o MeV Eaoo 4.410o MeV
Enoo 14.988o MeV Eaoo 2.762o MeV

Nextoweosolveoforotheomomentaobyoeliminatingotheoenergies.oWhenoweosubstituteomao =o4,omno =o1,omdo =o2,oQo=o17.6,oEdo =o0.15ointo
otheseoequationsoweogetotheofollowingoresults.


pd 1 1
pno o 2 3opdo2o o352 pao 8opdo o2 2 3opdo2o o352
5 5 10

Weodooknowotheoinitialomomentumoofotheodeuteron,ohowever,osinceoweoknowoitsoenergy.oWeocano furthero evaluateo ourosolutionsofor
pnoando paobyosubstituting:

pdo

Theoparticleo momentao(oinounitsoof amuMeV )oforoeachosetoofosolutionsoisothus:
pnoo 5.165 paoo 5.940
pnoo 5.475 paoo 4.700


Theo largestoneutronomomentumooccursoinotheoforwardo(+)odirection,osootheohighestoneutronoenergyoofo14.98oMeVocorrespondso
toothisodirection.




3

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