medical-physics

Layer 1 — Physics24 concepts in this subtree

Physics of medical diagnosis and treatment. Four principal sub-fields: (i) radiotherapy physics — treatment planning, dosimetry, and quality assurance for tele- and brachytherapy (linear-accelerator beams, stereotactic radiosurgery,…

Beer-Lambert I(x) = I₀ exp(−μx): photoelectric + Compton + pair-production
HVL = ln 2 / μ: thickness halving narrow-beam intensity
H = w_R · D: w_R(photon)=1, w_R(α)=20, w_R(neutron)=f(E)
μ·HVL = ln 2; TVL/HVL = log(10)/log(2) ≈ 3.32
exp(−μ·n·HVL) = 2^{−n}: 1/2, 1/4, 1/8 at n=1,2,3; 1/1024 at n=10
w_R(α) = 20: 1 Gy α absorbed ⇒ 20 Sv equivalent
Beer-Lambert exponential attenuation I(x) = I_0 e^{-mu x}; first-order linear ODE
Compton scattering: Delta lambda = (h / m_e c)(1 - cos theta); 4-momentum conservation
Stejskal-Tanner DWI: S(b)/S_0 = e^{-bD}; heat-kernel of Laplacian on R^3
Theorem: dI/dx + mu I = 0 for I(x) = I_0 e^{-mu x} (Beer-Lambert ODE residual)
Theorem: Delta lambda(theta = pi/2) - h/(m_e c) = 0 (Compton wavelength at 90 deg)
Theorem: dS/db + D S = 0 for S(b) = S_0 e^{-b D} (DWI signal-decay ODE)
X-ray CT (Radon transform)
MRI (Bloch equations)
PET (positron emission)
Radiation therapy (LQ model + fractionation)
Ultrasound imaging (acoustic impedance)
Photodynamic therapy (PDT)
Rayleigh resolution (1879)
CT (Hounsfield 1973)
MRI (Lauterbur-Mansfield 1973)
IMRT (Bortfeld 1990)
Bragg peak (Wilson 1946)
Ultrasound (Curie 1880)
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