Physica

05 Biology

Incomplete-repair BED (two fractions)

θ = e^{−μ Δt}. BED = n d [1 + g d/(α/β)] with g = 1 + 2θ/(n−…) for two doses: 2d(1 + (d(1+θ))/(α/β)).

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Simulation

Incomplete-repair BED (two fractions) — Change the numbers; the scene follows.

Where it works

Linear accelerator

Linear accelerator

Isocenter

In the treated volume — tumour and OARs at isocenter, after the dose has been delivered.

Open this machine

Formula

θ=eμΔt,E=2αd+2βd2(1+θ)\theta=e^{-\mu\Delta t},\quad E=2\alpha d+2\beta d^2(1+\theta)

Variables

Results

  • θ

    Remaining fraction

    0.0625

  • BED

    BED of the pair

    6.8333Gy

  • BED_∞

    BED at infinite gap

    6.6667Gy

Curve

Explanation

θ=eμΔt,E=2αd+2βd2(1+θ)\theta=e^{-\mu\Delta t},\quad E=2\alpha d+2\beta d^2(1+\theta)

What it means

When two fractions (or two HDR pulses, or two daily IMRT beams many hours apart? usually not) are separated by a gap Δt comparable to the repair half-time, some sublethal damage remains and the β term is inflated by 1+θ, θ = e^{−μ Δt}. Repair T½ is ~0.5–1 h for early tissues and ~1.5–4 h for late. This is why twice-daily treatments need ≥6 h and why pulsed-dose-rate HDR is not equivalent to a single LDR dwell of the same total dose. This is a working relation in Radiobiology.

Where it is used

Clinically it sits on the Linear accelerator — Isocenter. In the treated volume — tumour and OARs at isocenter, after the dose has been delivered. Radiobiology sits between the prescription and the organ-at-risk: LQ, BED, EQD2, and why 2 Gy is not 2 Gy if the fraction size changed. Use it to compare regimens, not to invent one.

Linear accelerator · Open this machine

How to use it

Enter d (each), gap Δt (h), repair T½ (h) and α/β. Read θ, the extra β factor (1+θ), and BED for the pair (n=2). Δt = 0 → fully additive (one 2d fraction); Δt → ∞ → two independent fractions. Change one input and watch the curve and the simulation follow.

Symbols

  • dDose each2 Gy
  • ΔtGap6 h
  • Repair half-time1.5 h
  • α/βAlpha/beta3 Gy

Worked example

A typical case from the default values: d = 2 Gy (Dose each); Δt = 6 h (Gap); T½ = 1.5 h (Repair half-time); α/β = 3 Gy (Alpha/beta). Substituting into the relation gives θ = 0.0625; BED = 6.8333 Gy; BED_∞ = 6.6667 Gy. These are teaching numbers — align them with your machine.

Typical values give

  • θ = 0.0625
  • BED = 6.8333Gy
  • BED_∞ = 6.6667Gy

Where it comes from

The displayed formula is the working relation. θ = e^{−μ Δt}. BED = n d [1 + g d/(α/β)] with g = 1 + 2θ/(n−…) for two doses: 2d(1 + (d(1+θ))/(α/β)). Usual reference: Thames / Dale / Lea–Catcheside. Derive it in the specialty lesson, then return here to pin the numbers.

Reference: Thames / Dale / Lea–Catcheside

Assumptions & limits

Mono-exponential repair, two equal fractions, no repopulation. Multi-fraction g is the Lea–Catcheside sum (see the g-factor calculator). Not a full PDR / HDR schedule.

Pitfalls

α/β is a model parameter, not a measured organ. BED from incomplete repair or a changed overall time is not the simple n·d·(1+d/(α/β)). Never EQD2 a stereotactic dose with an α/β you did not state. Mono-exponential repair, two equal fractions, no repopulation. Multi-fraction g is the Lea–Catcheside sum (see the g-factor calculator). Not a full PDR / HDR schedule.

Keep this

Always write α/β and the fraction size next to a BED or EQD2. Mono-exponential repair, two equal fractions, no repopulation. Multi-fraction g is the Lea–Catcheside sum (see the g-factor calculator). Not a full PDR / HDR schedule.

In this specialty

Radiobiology