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Engineering reference // radiation protection

Drawing No. EH–NR–016 // Nuclear Engineering & Radiation

Radiation Protection Formula Sheet

A compact health-physics reference for the core relations behind activity, external exposure control, shielding and protection quantities. The page keeps activity, absorbed dose, equivalent dose and effective dose separate because they describe different physical and protection concepts.

Fast reference, with engineering context

Use the equations directly for screening calculations, then open the linked EngineerHub tools for input handling and unit conversion. Formula applicability and major limitations are stated beside each relation.

Reference conventions

1 Gy = 1 J/kgAbsorbed dose
1 Sv = 100 remProtection quantity conversion
λ = ln2/T½Decay constant
ALARA / optimisationTime · distance · shielding are controls, not a dose formula

Time, distance and shielding

THE THREE CONTROLS SOURCE r₁ r₂ SHIELD thickness x SHIELDING I = I₀e^−μx, HVL = ln2/μ DISTANCE Ḋ₂ = Ḋ₁(r₁/r₂)² TIME D = Ḋ · t Doubling distance quarters the dose rate.
External exposure can often be reduced by shortening time, increasing distance and adding suitable shielding. Real source geometry, scatter and shielding buildup must be considered.

01 // Radioactive decay and activity

For one radionuclide with no production term, the number of atoms and activity decrease exponentially.

Core relation
A(t) = A₀e−λt = A₀·2−t/T½
λ = ln2/T½   ;   A = λN
SymbolMeaningSI unitsUS customary
AActivityBq = s⁻¹Ci or Bq
A₀Initial activityBqCi or Bq
λDecay constants⁻¹, d⁻¹s⁻¹, d⁻¹
Physical half-lifes, h, d, ys, h, d, y
NNumber of radioactive atomsatomsatoms
Worked example — three half-lives

Given: A₀ = 100 MBq, physical half-life = 8 days, elapsed time = 24 days.

t/T½ = 24/8 = 3
A = 100×2⁻³ = 12.5 MBq
Answer: A = 12.5 MBq.

Biological clearance is not included in physical radioactive decay.

For internal activity, an effective half-life can be useful when physical decay and biological removal are both approximately first order: 1/Teff = 1/Tphys + 1/Tbio.

02 // Dose from a known dose rate

If dose rate is approximately constant over the exposure interval, accumulated dose is rate times time.

Core relation
D = Ḋ·t
For varying rate: D = ∫Ḋ(t)dt
SymbolMeaningSI unitsUS customary
DDose quantity being accumulatedGy or Sv as appropriaterad/rem as appropriate
Corresponding dose rateGy/h, Sv/hrad/h, rem/h
tExposure timeh, sh, min
Worked example — 20 minutes in a field

Given: dose-equivalent rate = 0.50 mSv/h for 20 min.

t = 20/60 = 0.3333 h
H = 0.50×0.3333 = 0.1667 mSv
Answer: H ≈ 0.167 mSv.

US check: ≈0.0167 rem = 16.7 mrem.

Only multiply quantities of the same type; do not mix absorbed-dose rate with effective dose without a valid conversion basis.

Time reduction is a practical exposure-control method, but job planning must also consider source changes, occupancy, task constraints and uncertainty.

03 // Inverse-square scaling for a point source

For an isotropic point source in free space with negligible attenuation and scatter, fluence and dose rate scale approximately with 1/r².

Core relation
Ḋ₂ = Ḋ₁(r₁/r₂)²
Ḋ·r² ≈ constant
SymbolMeaningSI unitsUS customary
Dose-rate quantityGy/h or Sv/hrad/h or rem/h
rDistance from effective point sourcemft
Worked example — moving away from a point source

Given: Dose rate = 2.0 mSv/h at 1.0 m; new distance = 3.0 m.

Ḋ₂ = 2.0(1/3)² = 0.222 mSv/h
Answer: Ḋ₂ ≈ 0.222 mSv/h.

Do not use the point-source inverse-square law in the near field of an extended source without geometry correction.

Large area/line sources, contact measurements, shielded sources and strong scatter fields can depart substantially from ideal 1/r² behavior.

04 // Exponential attenuation, HVL and TVL

For a narrow monoenergetic photon beam in a homogeneous absorber, uncollided intensity decreases exponentially.

Core relation
I = I₀e−μx
HVL = ln2/μ   ;   TVL = ln10/μ   ;   I/I₀ = 2−x/HVL
SymbolMeaningSI unitsUS customary
I,I₀Transmitted / incident intensity or uncollided fluenceconsistent unitsconsistent units
μLinear attenuation coefficientm⁻¹, cm⁻¹in⁻¹
xShield thicknessm, cmin
HVLHalf-value layerm, cmin
TVLTenth-value layerm, cmin
Worked example — two half-value layers

Given: HVL = 6.0 cm, so μ = ln2/6 = 0.1155 cm⁻¹; shield x = 12 cm.

I/I₀ = 2⁻² = 0.25
TVL = ln10/μ = 19.93 cm
Answer: 25% of the uncollided beam remains; TVL ≈19.9 cm.

Broad-beam shielding often requires a buildup factor; μ is energy- and material-dependent.

Exponential attenuation is exact for the ideal uncollided component. Real protection calculations may include scatter, secondary radiation, source spectrum and geometry.

05 // Absorbed dose

Absorbed dose is energy imparted by ionizing radiation per unit mass.

Core relation
D = dε̄/dm
1 Gy = 1 J/kg   ;   1 Gy = 100 rad
SymbolMeaningSI unitsUS customary
DAbsorbed doseGy = J/kgrad
dε̄Mean energy impartedJerg or J
dmMass receiving energykgg or kg
Worked example — energy deposited in tissue

Given: 0.020 J is imparted to 2.0 kg of material.

D = 0.020/2.0 = 0.010 Gy
Answer: D = 0.010 Gy = 10 mGy.

US check: 1 rad.

Absorbed dose is physical energy per mass; it does not by itself include radiation or tissue weighting.

For nonuniform irradiation, dose is spatially dependent. Organ/tissue averages used for protection quantities are defined by the relevant dosimetry framework.

06 // Equivalent dose to a tissue or organ

Equivalent dose weights absorbed dose in a tissue by radiation type using ICRP radiation weighting factors.

Core relation
HT = ΣR wRDT,R
Unit: sievert (Sv)
SymbolMeaningSI unitsUS customary
HTEquivalent dose in tissue TSvrem
DT,RMean absorbed dose in tissue T from radiation RGyrad
wRRadiation weighting factordimensionlessdimensionless
Worked example — illustrative alpha dose

Given: Mean absorbed dose to one tissue = 5 mGy from alpha particles; use wR = 20.

HT = 20×0.005 Gy = 0.100 Sv
Answer: HT = 0.100 Sv = 100 mSv.

US check: 10 rem.

Equivalent dose is a protection quantity; do not use it to predict deterministic tissue reactions in an individual.

Radiation weighting factors are specified by the adopted protection framework. ICRP Publication 103 is the basis used here.

07 // Effective dose

Effective dose combines equivalent doses in tissues using tissue weighting factors to represent overall stochastic detriment for protection purposes.

Core relation
E = ΣT wTHT
ΣwT = 1 in the ICRP tissue-weighting scheme
SymbolMeaningSI unitsUS customary
EEffective doseSvrem
HTEquivalent dose to tissue TSvrem
wTTissue weighting factordimensionlessdimensionless
Worked example — two illustrative tissue contributions

Given: HT,1 = 20 mSv with wT,1 = 0.12; HT,2 = 10 mSv with wT,2 = 0.04.

Econtribution = 0.12×20 + 0.04×10 = 2.8 mSv
Answer: These two tissues contribute 2.8 mSv to effective dose.

Effective dose is intended for radiological protection, not individual medical risk prediction.

A complete effective-dose calculation sums all relevant tissue contributions under the adopted ICRP weighting scheme.

08 // Committed effective dose from intake

For a known radionuclide intake and an applicable committed effective dose coefficient, committed dose is intake times coefficient.

Core relation
E(τ) = I · e(g)
Dose coefficient e(g): Sv/Bq
SymbolMeaningSI unitsUS customary
IActivity intakeBqµCi/Bq as needed
e(g)Committed effective dose coefficient for nuclide, form, route and ageSv/Bqrem/Ci equivalent
E(τ)Committed effective dose over integration period τSvrem
Worked example — illustrative dose coefficient

Given: Intake = 5000 Bq; applicable committed effective dose coefficient = 2.0×10⁻⁸ Sv/Bq.

E = 5000×2.0×10⁻⁸ = 1.0×10⁻⁴ Sv
Answer: E = 0.10 mSv.

US check: 10 mrem.

Never reuse a coefficient across radionuclides, chemical forms, intake routes or age groups unless the reference explicitly permits it.

Internal dosimetry requires biokinetic and dosimetric models. Use current ICRP/IAEA or regulatory dose coefficients applicable to the radionuclide and exposure scenario.

09 // Quick formula summary

Compact print reference. Use the detailed sections above for definitions and limitations.

TopicEquationPurposeTool
DecayA=A₀e⁻λtActivity over timeDose guide
TimeD=ḊtExposure durationDose guide
DistanceḊ∝1/r²Point-source scalingShielding
AttenuationI=I₀e⁻μxPhoton shieldingShielding
Absorbed doseD=dε/dmEnergy per massDose guide
Equivalent doseHT=ΣwRDT,RRadiation weightingDose guide
Effective doseE=ΣwTHTTissue weightingDose guide
Internal doseE(τ)=I·e(g)Intake × coefficientNORM worker

10 // Assumptions & limitations

Fundamental equations are only useful when their assumptions match the actual problem.

11 // Technical references

IAEA GSR Part 3 and ICRP Publication 103 provide the protection framework; NRC Part 20 is used here for SI/traditional dose-unit conversions. Regulatory requirements must be checked for the user's jurisdiction.

12 // Related EngineerHub tools