\documentclass[10pt,a4paper]{article} % Packages \usepackage{fancyhdr} % For header and footer \usepackage{multicol} % Allows multicols in tables \usepackage{tabularx} % Intelligent column widths \usepackage{tabulary} % Used in header and footer \usepackage{hhline} % Border under tables \usepackage{graphicx} % For images \usepackage{xcolor} % For hex colours %\usepackage[utf8x]{inputenc} % For unicode character support \usepackage[T1]{fontenc} % Without this we get weird character replacements \usepackage{colortbl} % For coloured tables \usepackage{setspace} % For line height \usepackage{lastpage} % Needed for total page number \usepackage{seqsplit} % Splits long words. %\usepackage{opensans} % Can't make this work so far. Shame. Would be lovely. \usepackage[normalem]{ulem} % For underlining links % Most of the following are not required for the majority % of cheat sheets but are needed for some symbol support. \usepackage{amsmath} % Symbols \usepackage{MnSymbol} % Symbols \usepackage{wasysym} % Symbols %\usepackage[english,german,french,spanish,italian]{babel} % Languages % Document Info \author{Molly} \pdfinfo{ /Title (3-4-the-five-rs-of-radiobiology.pdf) /Creator (Cheatography) /Author (Molly) /Subject (3.4 The Five Rs of Radiobiology Cheat Sheet) } % Lengths and widths \addtolength{\textwidth}{6cm} \addtolength{\textheight}{-1cm} \addtolength{\hoffset}{-3cm} \addtolength{\voffset}{-2cm} \setlength{\tabcolsep}{0.2cm} % Space between columns \setlength{\headsep}{-12pt} % Reduce space between header and content \setlength{\headheight}{85pt} % If less, LaTeX automatically increases it \renewcommand{\footrulewidth}{0pt} % Remove footer line \renewcommand{\headrulewidth}{0pt} % Remove header line \renewcommand{\seqinsert}{\ifmmode\allowbreak\else\-\fi} % Hyphens in seqsplit % This two commands together give roughly % the right line height in the tables \renewcommand{\arraystretch}{1.3} \onehalfspacing % Commands \newcommand{\SetRowColor}[1]{\noalign{\gdef\RowColorName{#1}}\rowcolor{\RowColorName}} % Shortcut for row colour \newcommand{\mymulticolumn}[3]{\multicolumn{#1}{>{\columncolor{\RowColorName}}#2}{#3}} % For coloured multi-cols \newcolumntype{x}[1]{>{\raggedright}p{#1}} % New column types for ragged-right paragraph columns \newcommand{\tn}{\tabularnewline} % Required as custom column type in use % Font and Colours \definecolor{HeadBackground}{HTML}{333333} \definecolor{FootBackground}{HTML}{666666} \definecolor{TextColor}{HTML}{333333} \definecolor{DarkBackground}{HTML}{A3A3A3} \definecolor{LightBackground}{HTML}{F3F3F3} \renewcommand{\familydefault}{\sfdefault} \color{TextColor} % Header and Footer \pagestyle{fancy} \fancyhead{} % Set header to blank \fancyfoot{} % Set footer to blank \fancyhead[L]{ \noindent \begin{multicols}{3} \begin{tabulary}{5.8cm}{C} \SetRowColor{DarkBackground} \vspace{-7pt} {\parbox{\dimexpr\textwidth-2\fboxsep\relax}{\noindent \hspace*{-6pt}\includegraphics[width=5.8cm]{/web/www.cheatography.com/public/images/cheatography_logo.pdf}} } \end{tabulary} \columnbreak \begin{tabulary}{11cm}{L} \vspace{-2pt}\large{\bf{\textcolor{DarkBackground}{\textrm{3.4 The Five Rs of Radiobiology Cheat Sheet}}}} \\ \normalsize{by \textcolor{DarkBackground}{Molly} via \textcolor{DarkBackground}{\uline{cheatography.com/30516/cs/9557/}}} \end{tabulary} \end{multicols}} \fancyfoot[L]{ \footnotesize \noindent \begin{multicols}{3} \begin{tabulary}{5.8cm}{LL} \SetRowColor{FootBackground} \mymulticolumn{2}{p{5.377cm}}{\bf\textcolor{white}{Cheatographer}} \\ \vspace{-2pt}Molly \\ \uline{cheatography.com/molly} \\ \end{tabulary} \vfill \columnbreak \begin{tabulary}{5.8cm}{L} \SetRowColor{FootBackground} \mymulticolumn{1}{p{5.377cm}}{\bf\textcolor{white}{Cheat Sheet}} \\ \vspace{-2pt}Not Yet Published.\\ Updated 21st October, 2016.\\ Page {\thepage} of \pageref{LastPage}. \end{tabulary} \vfill \columnbreak \begin{tabulary}{5.8cm}{L} \SetRowColor{FootBackground} \mymulticolumn{1}{p{5.377cm}}{\bf\textcolor{white}{Sponsor}} \\ \SetRowColor{white} \vspace{-5pt} %\includegraphics[width=48px,height=48px]{dave.jpeg} Measure your website readability!\\ www.readability-score.com \end{tabulary} \end{multicols}} \begin{document} \raggedright \raggedcolumns % Set font size to small. Switch to any value % from this page to resize cheat sheet text: % www.emerson.emory.edu/services/latex/latex_169.html \footnotesize % Small font. \begin{multicols*}{3} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Acute Hypoxia}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Can develop in tumours when blood vessels are temporarily closed or blocked.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{There is evidence that the blood vessels in tumours open and close in a random fashion so that different parts of the tumour become hypoxic intermittently.} \tn % Row Count 6 (+ 4) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{As a result, some cells may be hypoxic during a radiation dose, but if the radiation is delayed a different group of cells may become hypoxic.} \tn % Row Count 9 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Acute Hypoxia}} is due to transient closure of capillaries or arterioles servicing parts of the tumour.} \tn % Row Count 12 (+ 3) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{While this vessel is closed, the tumour cells become hypoxic and resistant to the indirect action of radiation.} \tn % Row Count 15 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{These vessels are usually only closed for short times but may occur during a fractionated dose of radiation.} \tn % Row Count 18 (+ 3) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Splitting the dose into fractions raises the possibility of the closed vessel being open the next time around, and therefore allowing the tumour cells to be killed.} \tn % Row Count 22 (+ 4) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Clinical Applications}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Clinical Use of the α/β Ratio}}} \tn % Row Count 1 (+ 1) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The α/β ratio provides the dose in Gray where cell killing from linear and quadratic components of the linear quadratic equation are equal. At points below this value, linear cell kill is dominant; in those after quadratic cell kill takes over. This ratio may be used in many areas of radiotherapy.} \tn % Row Count 7 (+ 6) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Differentiating early and late responding normal tissue}}} \tn % Row Count 9 (+ 2) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Early responding tissues (high α/β ratio) sensitive to total dose but with minimal effect with fractionation. Late responding tissues (low α/β ratio), demonstrating increased survival at low doses and significantly greater toxicity at higher doses.} \tn % Row Count 15 (+ 6) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Determining sensitivity of tumour cells to fractionation}}} \tn % Row Count 17 (+ 2) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Most tumours are rapidly growing and have high α/β values, making them sensitive to overall dose with less effect from fraction size. Some tumours, notably prostate cancer and melanoma, have low α/β values. This makes them more sensitive to {\bf{large}} fraction sizes and resistant to small fraction sizes. In practice: high dose rate brachytherapy → delivers a small number of large doses to the vicinity of the prostate, has potential for increasing cure rates of prostate cancer.} \tn % Row Count 27 (+ 10) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Choosing fractionation schedules}}} \tn % Row Count 28 (+ 1) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Low α/β tissues typically suffer less toxicity at low doses compared with high α/β tissues. Most tumours also possess high α/β values. In areas where late toxicity requires high dose, such as in the skin or limbs, it is possible to shorten treatment times without significant late normal tissue toxicity. This becomes problematic in areas with organs sensitive to late effects; in these cases a more fractionated regime is recommended to exploit the cell kill between the tumour cells and late responding cells.} \tn % Row Count 39 (+ 11) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Clinical Applications (cont)}} \tn % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Clinical Use Of Dose Response Curves}}} \tn % Row Count 1 (+ 1) % Row 9 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Dose response curves can be generated for tumour control or normal tissue complications. If compared, the ratio between the two curves at a particular dose is the therapeutic index. If the curves can be shifted (eg. by drugs, oxygenation etc) then the therapeutic index is altered, possibly providing a beneficial effect.} \tn % Row Count 8 (+ 7) % Row 10 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Chemotherapy and Dose Response Curves}}} \tn % Row Count 9 (+ 1) % Row 11 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Chemotherapy agents which sensitise cells to radiation will usually shift the tumour control and normal tissue complication curves to the left (a greater effect for a similar dose). If chemotherapy widens the gap between tumour control and normal tissue complications for a particular dose, then the therapeutic index will be improved and chemotherapy may be beneficial. This explains why, for some treatments, a reduced fraction size or dose is used when concurrent treatment is used instead of radiation alone.} \tn % Row Count 20 (+ 11) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{X} \SetRowColor{DarkBackground} \mymulticolumn{1}{x{5.377cm}}{\bf\textcolor{white}{RBE as a function of LET}} \tn \SetRowColor{LightBackground} \mymulticolumn{1}{p{5.377cm}}{\vspace{1px}\centerline{\includegraphics[width=5.1cm]{/web/www.cheatography.com/public/uploads/molly_1477041771_Capture.PNG}}} \tn \hhline{>{\arrayrulecolor{DarkBackground}}-} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{RBE as a function of LET}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{As LET increases, survival curves become steeper and the extrapolation number tends towards unity.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Another way to present these data is to plot the RBE as a function of LET.} \tn % Row Count 4 (+ 2) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{As the LET increases, the RBE increases slowly at first and then more rapidly as the LET increases beyond 10 keV/µm, reaching a peak at about 100 keV/µm after which it falls again to lower values.} \tn % Row Count 8 (+ 4) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The shape of the survival curve for mammalian cells exposed to sparsely ionising radiation strongly suggests that more than one target in the cell must be inactivated before the cell will lose its reproductive integrity.} \tn % Row Count 13 (+ 5) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{In order to understand the RBE/LET relationship, it is convenient to consider a cell as having two sensitive sites.} \tn % Row Count 16 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Low LET radiation produces ionising events that are well separated and in most cases only one event will be deposited per cell, which is insufficient to kill the cell. Cell kill is only possible when two separate particles pass through the cell.} \tn % Row Count 21 (+ 5) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{At the peak of the graph, radiation is of optimum LET where the average distance between ionising events is just exactly matched to the average spacing between the sensitive sites in the cell.} \tn % Row Count 25 (+ 4) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{This radiation is efficient at killing since no radiation is wasted.} \tn % Row Count 27 (+ 2) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{As the LET is further increased, ionising events are clustered even closer together. The radiation becomes less efficient at killing cells because of the 'overkill effect'.} \tn % Row Count 31 (+ 4) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{RBE as a function of LET (cont)}} \tn % Row 9 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Many cells have three or more ionising events in them, when only two are necessary to kill; this leads to a waste of radiation} \tn % Row Count 3 (+ 3) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{X} \SetRowColor{DarkBackground} \mymulticolumn{1}{x{5.377cm}}{\bf\textcolor{white}{Therapeutic gain factor TGF}} \tn \SetRowColor{LightBackground} \mymulticolumn{1}{p{5.377cm}}{\vspace{1px}\centerline{\includegraphics[width=5.1cm]{/web/www.cheatography.com/public/uploads/molly_1477041399_Capture.PNG}}} \tn \hhline{>{\arrayrulecolor{DarkBackground}}-} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{RBE for different cells and tissues}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Even for a given total dose or dose per fraction, the RBE varies greatly according to the tissue or end point studied because of differences in the intrinsic radiosensitivity of various types of cells.} \tn % Row Count 5 (+ 5) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{In general, cells characterised by an x-ray survival curve with a large shoulder, indicating that they can accumulate and repair a large amount of sublethal damage, will show a large RBE for neutrons.} \tn % Row Count 9 (+ 4) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Conversely, cells for which the x-ray survival curve has little if any shoulder will exhibit small neutron RBE values.} \tn % Row Count 12 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{When considering the possibility of using neutrons for radiation therapy, we need to know the response of both tumour cells and normal cells.} \tn % Row Count 15 (+ 3) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{For neutrons to be more effective than x-rays in a clinical case, the RBE for tumours would need to be larger than the RBE for the relevant dose-limiting tissue.} \tn % Row Count 19 (+ 4) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{This is, the {\bf{therapeutic gain factor TGF}}} \tn % Row Count 20 (+ 1) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{X} \SetRowColor{DarkBackground} \mymulticolumn{1}{x{5.377cm}}{\bf\textcolor{white}{Relative Biological Effectiveness (RBE)}} \tn \SetRowColor{LightBackground} \mymulticolumn{1}{p{5.377cm}}{\vspace{1px}\centerline{\includegraphics[width=5.1cm]{/web/www.cheatography.com/public/uploads/molly_1477041211_Capture.PNG}}} \tn \hhline{>{\arrayrulecolor{DarkBackground}}-} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Relative Biological Effectiveness (RBE)}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Equal doses of different types of ionising radiations do not produce equal biological effects and when comparing these effects, x-rays are routinely used as the standard.} \tn % Row Count 4 (+ 4) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Relative Biological Effectiveness (RBE)}} allows comparison of a test radiation with a standard radiation.} \tn % Row Count 7 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{It is the ratio of dose between the radiations to give a certain biological effect.} \tn % Row Count 9 (+ 2) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{For example, if 10 Gy of 60Co gamma rays kills 50\% of the mice in a group, and 1 Gy of heavy ion radiotherapy kills the other group, the RBE would be 10/1=10} \tn % Row Count 13 (+ 4) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The {\bf{higher the RBE}} for a type of radiation, the {\bf{more damaging}} is the type of radiation, per unit of energy deposited in biological tissues.} \tn % Row Count 16 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{RBE depends on a number of other factors:} \tn % Row Count 17 (+ 1) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{The chosen biological effect}}: It may be that to kill 100\% of the mice, a different ratio of doses is required.} \tn % Row Count 20 (+ 3) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Fractionation of each dose}}: Fractionation may split the survival curves of the mice, meaning that 20 Gy of gamma rays versus 1.5 Gy of heavy ions are required, giving a RBE of 13.3.} \tn % Row Count 24 (+ 4) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Changes in dose rate}} can also impact on the survival of cells. This can therefore alter the RBE.} \tn % Row Count 26 (+ 2) % Row 9 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{In summary, it is found that the relative biological effectiveness depends on: 1. radiation quality (LET) 2. radiation dose 3. number of dose fractions 4. dose rate 5. biological system or end point.} \tn % Row Count 31 (+ 5) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{X} \SetRowColor{DarkBackground} \mymulticolumn{1}{x{5.377cm}}{\bf\textcolor{white}{Low vs High LET}} \tn \SetRowColor{LightBackground} \mymulticolumn{1}{p{5.377cm}}{\vspace{1px}\centerline{\includegraphics[width=5.1cm]{/web/www.cheatography.com/public/uploads/molly_1477040724_Capture.PNG}}} \tn \hhline{>{\arrayrulecolor{DarkBackground}}-} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Linear Energy Transfer}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{When radiation is absorbed in biological material, the ionising events are localised along the tracks of the individual charged particles in a pattern that depends on the type of radiation involved as well as the density of the material.} \tn % Row Count 5 (+ 5) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The spatial distribution or density of these events can be classified as sparse, intermediate or dense.} \tn % Row Count 8 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Electrons}} (unit charge and small mass), set in motion by gamma photons or x-rays, are said to be sparsely ionising.} \tn % Row Count 11 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Neutrons}} give rise to recoil protons carrying unit charge but having a mass \textasciitilde{}2000 times that of electrons. These have an intermediate ionising density.} \tn % Row Count 15 (+ 4) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Alpha-particles}} (double charge, mass 4 times proton) have a charge to mass ratio of 4000 times that of electrons and are said to be densely ionising.} \tn % Row Count 19 (+ 4) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Linear Energy Transfer (LET)}} accounts for all the energy liberated along the path of an ionising particle.} \tn % Row Count 22 (+ 3) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{LET is the average amount of energy a particular radiation imparts to the local medium per unit length (ie. Energy per Length).} \tn % Row Count 25 (+ 3) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{It is defined as the ratio dE/dL where dE is the average energy (keV) deposited in the medium by a charged particle of specified energy in moving a distance dL (micrometers).} \tn % Row Count 29 (+ 4) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{For radiotherapy, we are normally concerned about small amounts of energy over small distances, so the units we use are keV/μm.} \tn % Row Count 32 (+ 3) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Linear Energy Transfer (cont)}} \tn % Row 9 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The rate of loss of energy by ionising particles will be affected by the velocity of and the electronic charge on such a particle.} \tn % Row Count 3 (+ 3) % Row 10 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{A relatively slow moving, highly charged particle will have a high LET because of their greater energy deposition along the track.} \tn % Row Count 6 (+ 3) % Row 11 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{A faster moving particle and/or one with a lesser charge will have a much smaller LET.} \tn % Row Count 8 (+ 2) % Row 12 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{In practice, most radiations are not mono-energetic but consist of a wide spectrum of energiesConsequently, the LET can only be an average quantity for such radiations.} \tn % Row Count 12 (+ 4) % Row 13 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Energy loss events are essentially randomly distributed along the track of the photon or charged particle.} \tn % Row Count 15 (+ 3) % Row 14 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{For low LET radiations the energy deposition events along the track of the photon are sparse relative to the dimensions of biomolecules such as DNA with the result that photons may pass through such a molecule without depositing any energy.} \tn % Row Count 20 (+ 5) % Row 15 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{For such radiations the amount of energy deposited in a region of the track similar in dimensions to biological molecules also various widely from a few eV up to 100s of eV.} \tn % Row Count 24 (+ 4) % Row 16 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{For high LET radiation the energy loss events are much more closely spaced and significant energy will be deposited along all parts of the track similar in dimension to biomolecules.} \tn % Row Count 28 (+ 4) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{X} \SetRowColor{DarkBackground} \mymulticolumn{1}{x{5.377cm}}{\bf\textcolor{white}{Radioresistance of cell types}} \tn \SetRowColor{LightBackground} \mymulticolumn{1}{p{5.377cm}}{\vspace{1px}\centerline{\includegraphics[width=5.1cm]{/web/www.cheatography.com/public/uploads/molly_1477040211_Capture.PNG}}} \tn \hhline{>{\arrayrulecolor{DarkBackground}}-} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Radiosensitivity}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{There is an intrinsic radiosensitivity or radioresistance in different cell types.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Radiosensitivity}} is the relative susceptibility of cells, tissues, organs or organisms to the harmful effect of ionising radiation.} \tn % Row Count 5 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{In general, it has been found that cell radiosensitivity is directly proportional to the rate of cell division and inversely proportional to the degree of cell differentiation.} \tn % Row Count 9 (+ 4) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{This means that actively dividing cells or those not fully mature are most at risk from radiation.} \tn % Row Count 11 (+ 2) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The most radio-sensitive cells are those which: \{\{nl\}\}-have a high division rate \{\{nl\}\}-have a high metabolic rate \{\{nl\}\}-are of a non-specialised type \{\{nl\}\}-are well nourished} \tn % Row Count 15 (+ 4) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Factors that Affect Cellular Radiosensitivity}}:} \tn % Row Count 16 (+ 1) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Conditional factors}} - physical or chemical factors that exist previous to and/or at irradiation: \{\{nl\}\}Dose rate \{\{nl\}\}LET \{\{nl\}\}Fractionation \{\{nl\}\}Presence of oxygen} \tn % Row Count 20 (+ 4) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Inherent factors}} - biologic factors characteristic of the cell: \{\{nl\}\}Mitotic rate \{\{nl\}\}Degree of differentiation \{\{nl\}\}Cell cycle phase} \tn % Row Count 23 (+ 3) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Reoxygenation}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Reoxygenation is the phenomenon by which tumours with hypoxic regions become oxic again during radiotherapy treatment.} \tn % Row Count 3 (+ 3) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Tumours under 1 mm in size are fully oxic, but tumours over this size develop regions of hypoxia.} \tn % Row Count 5 (+ 2) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Reoxygenation occurs through several proposed mechanisms:} \tn % Row Count 7 (+ 2) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{1. Reopening of temporarily occluded blood vessels occurs in the minutes following radiation exposure} \tn % Row Count 10 (+ 3) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{2. Reduced respiration of lethally damaged cells leads to increased oxygen supply to anoxic cells within minutes to hours of radiation} \tn % Row Count 13 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{3. Death of cells due to mitotic catastrophe occurs within hours of radiotherapy. The resorption of dead cells leads to decreased distance from capillaries to tumour cells, improving their oxygen supply. This is the longest process, taking days.} \tn % Row Count 18 (+ 5) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Tumours contain a mixture of aerated and hypoxic cells. A dose of x-rays kills a greater proportion of aerated than hypoxic cells because they are more radiosensitive.} \tn % Row Count 22 (+ 4) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Immediately after irradiation, most cells in the tumour are hypoxic, but the pre-irradiation pattern tends to return because of reoxygenation.} \tn % Row Count 25 (+ 3) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{There are numerous ways to overcome hypoxia, of which fractionation is the most commonly used in the modern setting.} \tn % Row Count 28 (+ 3) % Row 9 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Fractionation of dose kills oxygenated cells first, allowing the hypoxic population to migrate closer to the vascular network and become oxygenated.} \tn % Row Count 31 (+ 3) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Reoxygenation (cont)}} \tn % Row 10 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The remaining fractionated dose then kills these previously hypoxic cells.} \tn % Row Count 2 (+ 2) % Row 11 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{If the radiation is given in a series of fractions separated in time sufficient for reoxygenation to occur, the presence of hypoxic cells does not greatly influence the response of the tumour.} \tn % Row Count 6 (+ 4) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Repair of Radiation Damage}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Radiation damage can be divided into three categories:} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{1. {\bf{Lethal damage}}, which is irreversible, and leads to cell death;} \tn % Row Count 4 (+ 2) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{2. {\bf{Potentially lethal damage}}, which can be modified by post-irradiation environmental conditions; and} \tn % Row Count 7 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{3. {\bf{Sublethal damage}}, which under normal circumstances can be repaired in hours unless additional sublethal damage is added with which it can interact to form lethal damage.} \tn % Row Count 11 (+ 4) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Chronic Hypoxia}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{In a histological study of human bronchial carcinomas, it was found that larger tumours had many centres of dead cells, which were far from their source of nutrients and oxygen, and were surrounded by intact tumour cells that were close to blood vessels.} \tn % Row Count 6 (+ 6) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{As the tumours grew larger, the necrotic centres enlarged so that the thickness of the layer of viable cells remained almost constant.} \tn % Row Count 9 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Assuming a steadily decreasing oxygen concentration, cells lying between these two cell types would be at an oxygen tension high enough to survive but low enough to protect them from the effects of ionising radiation.} \tn % Row Count 14 (+ 5) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Consequently, these cells could provide the focus for the subsequent regrowth of the tumour following radiotherapy.} \tn % Row Count 17 (+ 3) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Chronic Hypoxia}} is due to the poor vasculature of tumours and the distance oxygen must travel to reach cells that are far from the capillaries.} \tn % Row Count 20 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{These chronically hypoxic cells are also resistant to radiation.} \tn % Row Count 22 (+ 2) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Fractionated radiotherapy kills cells that lie close to the capillary more effectively. As these cells are removed, the chronically hypoxic cells are able to move closer to their nutrient source, and therefore become relatively oxic. Oxic cells can be killed.} \tn % Row Count 28 (+ 6) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Chronic and Acute Hypoxia of Tumours}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Cellular hypoxia in tumours}} can be caused by two different mechanisms;} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Chronic hypoxia}}, which is a consequence of the limited diffusion distance of oxygen.} \tn % Row Count 4 (+ 2) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Acute hypoxia}}, which results from the temporary closing of a blood vessel.} \tn % Row Count 6 (+ 2) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Mechanism of the oxygen effect}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{It is believed that oxygen acts at the level of the free radicals.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{When x-radiation is absorbed by tissue, fast charged particles are produced. These produce ion pairs. The ion pairs have a very short lifetime and produce free radicals that, because of their unpaired valance electrons, are highly reactive molecules.} \tn % Row Count 7 (+ 5) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{In most cases, it is these free radicals that break chemical bonds and ultimately produce biological damage.} \tn % Row Count 10 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{If oxygen is not present many of the ionised target molecules can repair themselves and recover the ability to function normally.} \tn % Row Count 13 (+ 3) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{However, with oxygen present there is less chance that restoration of damaged molecules will occur.} \tn % Row Count 15 (+ 2) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Oxygen is said to 'fix' the radiation damage in the sense of making it permanent and the process is known as the {\bf{'oxygen fixation hypothesis'.}}} \tn % Row Count 18 (+ 3) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The oxygen effect is large and important in the case of sparsely ionising radiations, such as x-rays, is absent for densely ionising radiations, such as α-particles, and has an intermediate value for moderately ionising radiations, such as 15-MeV neutrons.} \tn % Row Count 24 (+ 6) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{This is because the actions of high-LET radiations are less susceptible to enhancement than that of low-LET radiations.} \tn % Row Count 27 (+ 3) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The oxygen effect is only important for the indirect component of radiation damage.} \tn % Row Count 29 (+ 2) % Row 9 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{High-LET radiations are, in themselves, very effective at producing damage and very high LET radiations are so effective that the passage through a cell by one of them is lethal.} \tn % Row Count 33 (+ 4) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Mechanism of the oxygen effect (cont)}} \tn % Row 10 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The oxygen effect has no known practical significance in diagnostic radiology or nuclear medicine. Radiations used are low-LET, but doses are so low that little cell killing occurs.} \tn % Row Count 4 (+ 4) % Row 11 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Its main significance is in radiotherapy. It is likely that most, if not all, cancers contain cells that are hypoxic and also some which probably are severely hypoxic.} \tn % Row Count 8 (+ 4) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{X} \SetRowColor{DarkBackground} \mymulticolumn{1}{x{5.377cm}}{\bf\textcolor{white}{The Oxygen Effect}} \tn \SetRowColor{LightBackground} \mymulticolumn{1}{p{5.377cm}}{\vspace{1px}\centerline{\includegraphics[width=5.1cm]{/web/www.cheatography.com/public/uploads/molly_1477025011_Capture.PNG}}} \tn \hhline{>{\arrayrulecolor{DarkBackground}}-} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{The Oxygen Effect}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Results from survival curves show that mammalian cells are much more radiosensitive to x-rays in the presence of oxygen ({\bf{oxic}}) than they are in its absence ({\bf{anoxic}}).} \tn % Row Count 4 (+ 4) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{For some radiation types, there is a great difference in the biological effect seen in oxic versus anoxia conditions.} \tn % Row Count 7 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{It is particularly important for radiation types that cause damage through indirect action (eg. photons, electrons).} \tn % Row Count 10 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{This is because oxygen is required to 'fix', or make permanent, the damage caused by free radicals.} \tn % Row Count 12 (+ 2) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Without oxygen, the DNA radical that is created after reacting with the hydroxyl radical is simply repaired.} \tn % Row Count 15 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The ratio of hypoxic to aerated doses needed to achieve the same biological effect (for example, the same level of cell killing) is called the {\bf{oxygen enhancement ratio (OER). }}} \tn % Row Count 19 (+ 4) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{For low-LET radiation, it has a value close to 3 at high doses but may have a value of about 2 at doses below about 2 Gy (200 rads), which are typical of daily doses used in radiotherapy.} \tn % Row Count 23 (+ 4) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{For photons and electrons, the OER approaches 3 for most cell types. This means that cell killing is three times more effective in oxic conditions versus anoxic conditions for indirectly acting radiation. }}} \tn % Row Count 28 (+ 5) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Radiation types that rely more on {\bf{direct action}} (eg. protons, alpha particles, heavy ions) show minimal changes in the presence or absence of oxygen.} \tn % Row Count 32 (+ 4) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{The Oxygen Effect (cont)}} \tn % Row 9 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{This is because oxygen is not required to 'fix' the damage caused by these radiations, as they interact directly with the DNA molecule to cause damage.} \tn % Row Count 4 (+ 4) % Row 10 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The oxygen effect is seen in cell survival curves as a shift in the steepness of the curve.} \tn % Row Count 6 (+ 2) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Dose-Rate Effect}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Dose rate is one of the principal factors that determine the biological consequences of a given absorbed dose from low-LET radiation.} \tn % Row Count 3 (+ 3) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{As the dose rate is lowered and the exposure time extended, the biological effect is generally reduced.} \tn % Row Count 6 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The magnitude of the dose-rate effect from the repair of sublethal damage varies enormously between different types of cells.} \tn % Row Count 9 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Cells such as HeLa, which have a survival curve with a small initial shoulder, show only a modest dose-rate effect.} \tn % Row Count 12 (+ 3) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Chinese hamster cells have a broad shoulder to their survival curve and show a large dose-rate effect.} \tn % Row Count 15 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Three main biologic processes}} are involved:} \tn % Row Count 16 (+ 1) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{1. {\bf{Repair of sublethal damage}} occurs when radiation is delivered at a low dose rate, and the treatment time is extended to a point where it is comparable to the repair half-time. As the dose rate is reduced, more sublethal damage is repaired because the radiation injury is spread over a longer period. The cell survival curves become progressively less steep, and at the same time the extrapolation number approaches unity.} \tn % Row Count 25 (+ 9) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{2. {\bf{Cell proliferation}} occurs during protracted radiation exposure if the dose rate is low enough or the cell cycle time is short enough.} \tn % Row Count 28 (+ 3) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{3. {\bf{Reassortment and accumulation of cells}} throughout the cell cycle occur with a low dose rate in which proliferation is decreased because cells are arrested and accumulate in G2. This phase of the cycle is relatively radiosensitive. As a result, cell killing may be greater for a lower dose rate. This effect occurs over a narrow dose-rate range and is known as the inverse dose-rate effect.} \tn % Row Count 36 (+ 8) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Repopulation}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{As cellular damage and cell death occur during the course of the treatment, the tissue may respond with an increased rate of cell proliferation.} \tn % Row Count 3 (+ 3) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The effect of this cell proliferation during treatment, known as repopulation (regeneration), will be to increase the number of cells during the course of the treatment and {\bf{reduce the overall response to irradiation.}}} \tn % Row Count 8 (+ 5) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{This effect is most important in early-responding normal tissues (e.g., skin, gastrointestinal tract) or in tumours whose stem cells are capable of rapid proliferation.} \tn % Row Count 12 (+ 4) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{It will be of little consequence in late-responding, slowly proliferating tissues (e.g., kidney), which do not suffer much early cell death and hence do not produce an early proliferative response to the radiation treatment.} \tn % Row Count 17 (+ 5) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Important factor influencing local tumour control in patients with head and neck or cervical cancer.} \tn % Row Count 19 (+ 2) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Local control is reduced by approximately 0.5 percent for each day that overall treatment time is prolonged.} \tn % Row Count 22 (+ 3) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Repopulation provides the biological rationale for accelerating fractionated radiation therapy.} \tn % Row Count 24 (+ 2) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Repopulation is likely to be more important toward the end of a course of treatment, when sufficient damage has accumulated (and cell death occurred) to induce a regenerative response - for tumours as well as for normal tissues.} \tn % Row Count 29 (+ 5) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{\seqsplit{Reassortment/Redistribution}}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Variation in the radiosensitivity of cells in different phases of the cell cycle results in the cells in the more resistant phases being more likely to survive a dose of radiation.} \tn % Row Count 4 (+ 4) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Two effects can make the cell population {\bf{more sensitive}} to a subsequent dose of radiation:} \tn % Row Count 6 (+ 2) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{1. Some of the cells will be blocked in the G2 phase of the cycle, which is usually a sensitive phase.} \tn % Row Count 9 (+ 3) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{2. Some of the surviving cells will redistribute into more sensitive parts of the cell cycle.} \tn % Row Count 11 (+ 2) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Both effects will tend to make the whole population more sensitive to fractionated treatment as compared with a single dose.} \tn % Row Count 14 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{When radiotherapy is given to a population of cells, they may be in different parts of the cell cycle.} \tn % Row Count 17 (+ 3) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Cells in S-phase are typically radioresistant, whereas those in late G2 and M phase are relatively sensitive.} \tn % Row Count 20 (+ 3) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{A small dose of radiation delivered over a short time period (external beam or high dose brachytherapy) will kill a lot of the sensitive cells and less of the resistant cells.} \tn % Row Count 24 (+ 4) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Over time, the surviving cells will continue to cycle. If a second dose of radiation is delivered some time later, some of these cells will have left the resistant phase and be in a more sensitive phase, allowing them to be killed more easily.} \tn % Row Count 29 (+ 5) % Row 9 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{As reassortment inevitably involves cell proliferation, the survival will also be influenced by repopulation, which reduces the effect of reassortment.} \tn % Row Count 33 (+ 4) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{\seqsplit{Reassortment/Redistribution} (cont)}} \tn % Row 10 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Both reassortment and repopulation are important primarily in proliferating cell populations.} \tn % Row Count 2 (+ 2) % Row 11 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{In many normal tissues (and probably in some tumours), stem cells can be in a resting phase (G0) but can be recruited into the cell cycle to repopulate the tissue.} \tn % Row Count 6 (+ 4) % Row 12 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{There is some evidence that cells in cycle are slightly more sensitive to radiation than G0 cells, possibly because G0 cells may repair more potentially lethal damage.} \tn % Row Count 10 (+ 4) % Row 13 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Recruitment of resting cells into the proliferative cycle during the course of fractionated treatment, therefore, may tend to increase the sensitivity of the whole population.} \tn % Row Count 14 (+ 4) % Row 14 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Neither recruitment nor reassortment would be expected to have much influence on late responses that occur predominantly as a result of injury to tissues in which the rate of proliferation is low.} \tn % Row Count 18 (+ 4) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Repair}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{One of the primary reasons to fractionate radiotherapy.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{By splitting radiation dose into small parts, cells are allowed to repair sublethal damage.} \tn % Row Count 4 (+ 2) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The amount of damage that is repaired depends on the ability of the cell to recognise the damage and activate a){\bf{ repair pathways}} and b) {\bf{cell cycle arrest.}}} \tn % Row Count 8 (+ 4) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{{\bf{Malignant cells}} have often suppressed these pathways, often through mutation or inhibition of TP53, preventing them from undergoing efficient repair.} \tn % Row Count 12 (+ 4) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{{\bf{Normal tissue cells}} with intact repair pathways are able to repair the sublethal damage by the time the next fraction is delivered.} \tn % Row Count 15 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The shoulder on a survival curve after single radiation doses is indicative of the capacity of the cells to accumulate and repair radiation damage.} \tn % Row Count 18 (+ 3) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{If multiple doses are given with sufficient time between the fractions for repair to occur (4 to 24 hrs depending on the cells or tissue involved) the effective survival curves is straight on a semi-logarithmic plot and has a shallower slope than the curve for big single doses (ie. Repair is responsible for shoulder of survival curve).} \tn % Row Count 25 (+ 7) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The effective slope depends on the size of the individual dose fractions, becoming shallower as the fraction size is reduced. This effect is also seen for irradiation of different tissues.} \tn % Row Count 29 (+ 4) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The single dose survival curve for most cells has a finite initial slope apparently due to a (single-hit) non-repairable damage component, so there is a limit below which further reduction of the fraction size will no longer reduce the effective slope of the survival curve.} \tn % Row Count 35 (+ 6) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Repair (cont)}} \tn % Row 9 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{At this limit, essentially all the repairable damage is being repaired between each fraction so that the cell killing is due almost entirely to non-repairable events.} \tn % Row Count 4 (+ 4) % Row 10 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The fraction size at which this limit is reached is different for different cell populations depending on their repair capacity.} \tn % Row Count 7 (+ 3) % Row 11 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{When the size of the individual dose fractions is such that the survival is represented by the shoulder region of the survival curve, as for most dose fractions used clinically, then repair will be maximal when equal-sized dose fractions are given.} \tn % Row Count 12 (+ 5) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Split-Dose Experiments}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Recovery from sublethal damage is demonstrated by split-dose experiments.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Cells are exposed to sufficient radiation so that any survivors will have accumulated the maximum amount of sublethal damage.} \tn % Row Count 5 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{After a time interval, the survivors are irradiated again. In the absence of any recovery, the proportion of irradiated cells expected to survive the two radiation exposures should be the same as would survive a single radiation exposure equal to the sum of the two doses.} \tn % Row Count 11 (+ 6) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{In experiments, however, the observed proportion of survivors can be greater than this. In the time between the two exposures, cells that survive the first exposure are thought to recover from damage done during that exposure.} \tn % Row Count 16 (+ 5) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The pattern of repair is a combination of three processes occurring simultaneously:} \tn % Row Count 18 (+ 2) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{1. {\bf{Repair}}: First there is the prompt repair of sublethal radiation damage.} \tn % Row Count 20 (+ 2) % Row 6 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{2. {\bf{Reassortment/Redistribution}}: Second there is progression of cells through the cell cycle during the interval between the split doses.} \tn % Row Count 23 (+ 3) % Row 7 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{3. {\bf{Repopulation}}: Third, there is an increase of surviving fraction due to cell division when the interval between the split doses exceeds the cell cycle.} \tn % Row Count 27 (+ 4) % Row 8 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The dramatic dip in the split-dose curve at six hours, caused by reassortment, and the increase in survival by 12 hours, because of repopulation, is seen only for rapidly growing cells.} \tn % Row Count 31 (+ 4) \end{tabularx} \par\addvspace{1.3em} \vfill \columnbreak \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Split-Dose Experiments (cont)}} \tn % Row 9 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The phenomenon of repair is one of the important factors in the sparing effect on normal tissues by the multi-fraction dosage regimens that are commonly used in radiotherapy, even though sublethal damage repair occurs in both tumours and normal tissues.} \tn % Row Count 6 (+ 6) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Sublethal Damage}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Thought to be responsible for shoulders on survival curves.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The existence of this form of damage is inferred from the shape of the survival curves, but so far it has not been demonstrated directly.} \tn % Row Count 5 (+ 3) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Survival curves are a graphic representation of the relationship between the fraction of cells surviving and those being killed by given radiation doses. Survival curves, therefore, are a record of the production of lethal damage.} \tn % Row Count 10 (+ 5) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{Sublethal damage is presumed to occur because of the steep slope in the dose range beyond the shoulder.} \tn % Row Count 13 (+ 3) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{The change in slope shows increased vulnerability to radiation at higher doses, suggesting an accumulation of sublethal injuries has occurred in the low- dose range and is reaching lethal levels in the high-dose range.} \tn % Row Count 18 (+ 5) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{The sublethal injuries themselves are not detected; the only time anything is noted is when a cell is lethally injured and dies.} \tn % Row Count 21 (+ 3) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} \begin{tabularx}{5.377cm}{p{0.4977 cm} p{0.4977 cm} } \SetRowColor{DarkBackground} \mymulticolumn{2}{x{5.377cm}}{\bf\textcolor{white}{Potentially Lethal Damage (PLD)}} \tn % Row 0 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Under normal circumstances PLD is lethal, but under others is not.} \tn % Row Count 2 (+ 2) % Row 1 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{If we irradiate two identical cell populations with single doses of low-LET radiation under identical conditions, the probability of survival will differ according to the post- irradiation conditions.} \tn % Row Count 6 (+ 4) % Row 2 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{PLD is repaired and the survival fraction is increased if post- irradiation conditions are sub-optimal for growth, so that cells do not have to attempt mitosis while their chromosomes are damaged.} \tn % Row Count 10 (+ 4) % Row 3 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{If mitosis is delayed, DNA damage can be repaired.} \tn % Row Count 11 (+ 1) % Row 4 \SetRowColor{LightBackground} \mymulticolumn{2}{x{5.377cm}}{Therefore, there is a form of injury which can cause death in cells that are actively replicating, but which is not lethal in cells that are resting.} \tn % Row Count 14 (+ 3) % Row 5 \SetRowColor{white} \mymulticolumn{2}{x{5.377cm}}{In clinical radiation therapy, the importance of PLD repair is still not proved. However, it may be responsible for the radioresistance exhibited by some tumours, that is, these tumours can repair PLD efficiently, but this is still a matter of debate.} \tn % Row Count 20 (+ 6) \hhline{>{\arrayrulecolor{DarkBackground}}--} \end{tabularx} \par\addvspace{1.3em} % That's all folks \end{multicols*} \end{document}