Physica

05 Biology

LQ-linear (high dose per fraction)

LQ is applied only up to D_t = 2 α/β; beyond that the survival curve is linear with slope γ = α + 2 β D_t.

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Simulation

LQ-linear (high dose per fraction) — 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.

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Formula

lnS={αD+βD2DDtαDt+βDt2+γ(DDt)D>Dt-\ln S=\begin{cases}\alpha D+\beta D^2 & D\le D_t\\ \alpha D_t+\beta D_t^2+\gamma(D-D_t)& D>D_t\end{cases}

Variables

Results

  • D_t

    Transition dose

    20Gy

  • −ln S

    LQ-L

    6

  • −ln S_LQ

    Pure LQ

    6

  • ratio

    LQ / LQ-L

    1

Explanation

lnS={αD+βD2DDtαDt+βDt2+γ(DDt)D>Dt-\ln S=\begin{cases}\alpha D+\beta D^2 & D\le D_t\\ \alpha D_t+\beta D_t^2+\gamma(D-D_t)& D>D_t\end{cases}

What it means

LQ overestimates cell kill (and BED) at the large doses per fraction of SBRT because the log-survival curve is seen to straighten. LQ-L (or USC, universal survival curve) keeps LQ up to a transition dose D_t ≈ 2 α/β and then a linear tangent. For α/β = 10 Gy, D_t ≈ 20 Gy so a 18 Gy × 3 SBRT scheme is only mildly affected; for α/β = 3 Gy, D_t ≈ 6 Gy and a 10 Gy fraction is well into the linear region. 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.

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How to use it

Enter α, β, dose per fraction D and optionally D_t (defaults to 2 α/β). Read −ln S, the pure-LQ value, and the ratio. Use it as a sanity check on BED for d > 8 Gy. Change one input and watch the curve and the simulation follow.

Symbols

  • αAlpha0.3 Gy⁻¹
  • βBeta0.03 Gy⁻²
  • DDose per fraction10 Gy
  • D_tTransition (0 = 2α/β)0 Gy

Worked example

A typical case from the default values: α = 0.3 Gy⁻¹ (Alpha); β = 0.03 Gy⁻² (Beta); D = 10 Gy (Dose per fraction); D_t = 0 Gy (Transition (0 = 2α/β)). Substituting into the relation gives D_t = 20 Gy; −ln S = 6; −ln S_LQ = 6; ratio = 1. These are teaching numbers — align them with your machine.

Typical values give

  • D_t = 20Gy
  • −ln S = 6
  • −ln S_LQ = 6
  • ratio = 1

Where it comes from

The displayed formula is the working relation. LQ is applied only up to D_t = 2 α/β; beyond that the survival curve is linear with slope γ = α + 2 β D_t. Usual reference: Astrahan / Guerrero & Li / Joiner. Derive it in the specialty lesson, then return here to pin the numbers.

Reference: Astrahan / Guerrero & Li / Joiner

Assumptions & limits

One of several high-dose recipes (USC, MKM, G-function). Transition dose is not a measured universal. Does not include reoxygenation, which may dominate SBRT biology more than the shape of SF.

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. One of several high-dose recipes (USC, MKM, G-function). Transition dose is not a measured universal. Does not include reoxygenation, which may dominate SBRT biology more than the shape of SF.

Keep this

Always write α/β and the fraction size next to a BED or EQD2. One of several high-dose recipes (USC, MKM, G-function). Transition dose is not a measured universal. Does not include reoxygenation, which may dominate SBRT biology more than the shape of SF.

In this specialty

Radiobiology