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Файл:Ординатура / Хирургия / Библиотека им академика М.И. Перельмана / Книга_5545_Библиотеки_им_академика_М_И_Перельмана.pdf
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- •Preface
- •Contents
- •1: Structure of Matter
- •2: Radioactive Decay
- •2.1 Spontaneous Fission
- •1.1.1 Radiation
- •1.2 The Atom
- •1.2.3 Nuclear Binding Energy
- •1.3 Nuclear Nomenclature
- •1.5 Questions
- •Suggested Readings
- •2.2 Isomeric Transition
- •2.2.1 Gamma (γ)-Ray Emission
- •2.2.2 Internal Conversion
- •2.2.2.1 Problem 2.1
- •2.2.2.2 Answer
- •2.3 Alpha (α)-Decay
- •2.4 Beta (β−)-Decay
- •2.5 Positron (β+)-Decay
- •2.6 Electron Capture
- •2.7 Questions
- •Suggested Readings
- •3.1 Radioactive Decay Equation
- •3.1.1 General Equation
- •3.1.2 Half-Life
- •3.1.3 Mean Life
- •3.1.4 Effective Half-Life
- •3.2 Units of Radioactivity
- •3.3 Specific Activity
- •3.4 Calculation
- •3.5 Successive Decay Equations
- •3.5.1 General Equation
- •3.5.2 Transient Equilibrium
- •3.5.3 Secular Equilibrium
- •3.6 Questions
- •Suggested Readings
- •4.5 Poisson Distribution
- •4.6 Gaussian Distribution
- •4.7 Chi-Square Test
- •4.8 Minimum Detectable Activity
- •4.10 Questions
- •Suggested Readings
- •5.1 Cyclotron-Produced Radionuclides
- •5.2 Reactor-Produced Radionuclides
- •5.2.1 Fission or (n, f) Reaction
- •5.2.2 Neutron Capture or (n, γ) Reaction
- •5.6 Radionuclide Generators
- •5.8 Questions
- •Suggested Readings
- •6.1.1 Specific Ionization
- •6.1.2 Linear Energy Transfer
- •6.1.3 Range
- •6.1.4 Bremsstrahlung
- •6.1.5 Positron Annihilation
- •6.2.1.1 Photoelectric Effect
- •6.2.1.2 Compton Scattering
- •6.2.1.3 Pair Production
- •6.2.1.4 Raleigh Scattering
- •6.2.1.5 Photodisintegration
- •6.3.2 Half-Value Layer
- •6.5 Questions
- •Suggested Readings
- •7: Gas-Filled Detector
- •7.1 Principles of Gas-Filled Detector
- •7.2 Ionization Chamber
- •7.2.1 Ion Chamber Survey Meter
- •7.2.2 Dose Calibrator
- •7.2.2.1 Constancy
- •7.2.2.2 Accuracy
- •7.2.2.3 Linearity
- •7.2.2.4 Geometry
- •7.2.3 Pocket Dosimeter
- •7.3 Proportional Counter
- •7.4 Geiger–Müller Counter
- •7.5 Questions
- •Suggested Readings
- •8.1 Scintillation Counter
- •8.4.3 Characteristic X-Ray Peak
- •8.4.4 Backscatter Peak
- •8.4.5 Iodine Escape Peak
- •8.2 Solid Scintillation Detector
- •8.2.1 NaI (Tl) Detector
- •8.2.2 Bismuth Germanate Detector
- •8.2.3 Barium Fluoride Detector
- •8.2.4 Lutetium Oxyorthosilicate Detector
- •8.2.5 Gadolinium Oxyorthosilicate Detector
- •8.2.6 Yttrium Oxyorthosilicate Detector
- •8.2.7 Yttrium Aluminum Perovskite Detector
- •8.2.8 Lutetium Yttrium Oxyorthosilicate Detector
- •8.2.9 Lanthanum Bromide Detector
- •8.3 Solid-State Detector
- •8.3.2 Cadmium–Zinc–Tellurium Detector
- •8.3.3 Cesium Iodide (CsI(Tl)) Detector
- •8.3.4 Solid Scintillation Counter
- •8.3.4.1 NaI(Tl) Detector
- •8.3.4.2 Photomultiplier Tube
- •8.3.4.3 Preamplifier
- •8.3.4.4 Linear Amplifier
- •8.3.4.5 Pulse-Height Analyzer
- •8.3.4.6 Display or Storage
- •8.4 Gamma-Ray Spectrometry
- •8.4.1 Photopeak
- •8.4.6 Positron Annihilation Peak
- •8.4.7 Coincidence Peak
- •8.5 Liquid Scintillation Counter
- •8.5.1 Quenching
- •8.6.1 Energy Resolution
- •8.6.2 Detection Efficiency
- •8.6.2.1 Intrinsic Efficiency
- •8.6.2.2 Photopeak Efficiency or Photofraction
- •8.6.2.3 Geometric Efficiency
- •8.6.3 Dead Time
- •8.7 Gamma Well Counter
- •8.8 Thyroid Probe
- •8.8.1 Thyroid Uptake Measurement
- •8.9 Questions
- •Suggested Readings
- •9: Gamma Camera
- •9.1 Gamma Camera
- •9.1.2 Detector
- •9.1.3 Collimator
- •9.1.4 Photomultiplier Tube
- •9.1.5 X-, Y-Positioning Circuit
- •9.1.6 Pulse-Height Analyzer
- •9.2 Digital Camera
- •9.2.1 Solid State Digital Camera
- •9.3 Questions
- •Suggested Readings
- •10.1.1 Spatial Resolution
- •10.1.1.1 Intrinsic Resolution
- •10.1.1.2 Collimator Resolution
- •10.1.1.3 Scatter Resolution
- •10.1.2.1 Bar Phantom
- •10.1.2.2 Line-Spread Function
- •10.1.2.3 Modulation Transfer Function
- •10.1.3 Sensitivity
- •10.1.3.1 Collimator Efficiency
- •10.1.4 Uniformity
- •10.1.5 Pulse-Height Variation
- •10.1.6 Nonlinearity
- •10.1.7 Edge Packing
- •10.2 Gamma Camera Tuning
- •10.4 Contrast
- •10.4.1 Count Density
- •10.4.2 Image Noise
- •10.4.4 High Count Rate
- •10.4.6 Patient Motion
- •10.5.1 Daily Checks
- •10.5.1.2 Uniformity
- •10.5.2 Weekly Checks
- •10.5.3 Monthly Checks
- •10.5.3.1 High-Count Uniformity Calibration
- •10.5.3.2 Collimator Integrity
- •10.5.4 Annual, Semiannual, or As-Needed Checks
- •10.6 Questions
- •References and Suggested Readings
- •11.1.1 Central Processing Unit
- •11.1.2 Computer Memory
- •11.1.3 External Storage Device
- •11.1.4 Input/Output Device
- •11.1.7 Digital-to-Analog Conversion
- •11.1.8 Digital Image
- •11.2.1 Digital Data Acquisition
- •11.2.2 Static Study
- •11.2.3 Dynamic Study
- •11.2.4 Gated Study
- •11.2.7 Display
- •11.3.1 PACS
- •11.4 Questions
- •Suggested Readings
- •12: Single Photon Emission Computed Tomography
- •12.1 Tomographic Imaging
- •12.2 Single Photon Emission Computed Tomography
- •12.2.1 Data Acquisition
- •12.2.2 Image Reconstruction
- •12.2.2.1 Simple Backprojection
- •12.2.2.2 Filtered Backprojection
- •12.2.2.3 The Convolution Method
- •12.2.2.4 The Fourier Method
- •12.2.2.6 Iterative Reconstruction
- •12.3 SPECT/CT Scanner
- •12.4 Factors Affecting SPECT
- •12.4.1 Photon Attenuation
- •12.4.2 Attenuation Correction Methods
- •12.5 Partial-Volume Effect
- •12.5.2 Sampling
- •12.5.3 Scattering
- •12.6.1 Spatial Resolution
- •12.6.2 Sensitivity
- •12.6.3 Other Parameters
- •12.7.1 Daily Tests
- •12.7.2 Weekly Tests
- •12.7.2.1 Spatial Resolution
- •12.9 Questions
- •References and Suggested Readings
- •13: Positron Emission Tomography
- •13.1 Introduction
- •13.2 PET Radiopharmaceuticals
- •13.3.2 Block Detector
- •13.5 Coincidence Timing Window
- •13.6 PET/CT Scanner
- •13.7 PET/MR Scanner
- •13.7.2 MR Scanner
- •13.7.3 Commercial PET/MR Scanner
- •13.8 Mobile PET or PET/CT Scanner
- •13.9 Micro-PET Scanner
- •13.11 Data Acquisition
- •13.12 Image Reconstruction
- •13.13 Factors Affecting PET
- •13.13.1 Normalization
- •13.13.2 Photon Attenuation Correction
- •13.13.4 Random Coincidences
- •13.13.5 Scatter Coincidences
- •13.13.6 Dead Time
- •13.13.7 Radial Elongation
- •13.14.1 Spatial Resolution
- •13.14.2 Sensitivity
- •13.14.2.1 Noise Equivalent Count Rate
- •13.15.1 Daily Tests
- •13.15.1.1 Sinogram Check
- •13.15.2 Weekly Tests
- •13.15.2.1 Normalization
- •13.18 Questions
- •References and Suggested Reading
- •14.1 Background
- •14.5 Artificial Neural Network
- •14.7 Machine Learning
- •14.7.1 Decision Tree
- •14.7.2 Random Forest
- •14.7.3 Support Vector Machine
- •14.7.4 Computer Vision
- •14.8 Deep Learning
- •14.8.1 Convolutional Network
- •14.8.2 Recurrent Neural Network
- •14.8.3 Generative Adversarial Network
- •14.8.4 Transfer Learning
- •14.9 Radiomics
- •14.10 Natural Language Processing
- •14.11 Large Language Model
- •14.12 Generative Artificial Intelligence
- •14.13.1 Prompt
- •14.13.2 Token
- •14.13.3 Hallucination
- •14.13.4 Deepfake
- •14.13.5 Overfitting
- •14.15 Chatbot
- •14.18 Legal Implication
- •14.20 Questions
- •References
- •15.1 Introduction
- •15.2.1 Scheduling
- •15.2.2 Image Acquisition
- •15.2.3 Image Processing
- •15.2.4 Interpretation
- •15.2.5 Reporting
- •15.3.1 Oncology
- •15.3.2 Cardiovascular Disease
- •15.3.3 Bone Scintigraphy
- •15.3.4 Thyroid Imaging
- •15.5 Drug Development
- •15.6 Questions
- •References and Suggested Reading
- •16: Internal Radiation Dosimetry
- •16.1 Radiation Unit
- •16.1.1 Roentgen
- •16.1.2 Rad
- •16.1.3 Gray
- •16.1.4 Rem
- •16.1.5 Radiation Weighting Factor
- •16.1.6 Quality Factor
- •16.1.7 Sievert
- •16.2 Dose Calculation
- •16.2.1 Radiation Dose Rate
- •16.2.2 Cumulative Radiation Dose
- •16.2.3 Factors Affecting Ã
- •16.2.4 The S Values
- •16.4 Pediatric Dosage
- •16.5 Questions
- •References and Suggested Readings
- •17: Radiation Biology
- •17.1 The Cell
- •17.2.1 DNA Molecule
- •17.2.2 Chromosome
- •17.5 Cell Survival Curves
- •17.6 Factors Affecting Radiosensitivity
- •17.6.1 Dose Rate
- •17.6.2 Linear Energy Transfer
- •17.6.4 Chemicals
- •17.7 Radiosensitizer
- •17.7.1 Oxygen
- •17.7.2 Pyrimidine
- •17.7.3 Others
- •17.8 Radioprotector
- •17.9 Apoptosis
- •17.13.1 Hematopoietic Syndrome
- •17.13.2 Gastrointestinal Syndrome
- •17.13.3 Cerebrovascular Syndrome
- •17.14.1 Somatic Effects
- •17.14.1.1 Carcinogenesis
- •17.14.1.3 Dose–Response Relationship
- •17.14.1.5 Leukemia
- •17.14.1.6 Breast Cancer
- •17.14.1.7 Other Cancers
- •17.14.1.10 Nonspecific Life-Shortening
- •17.14.1.11 Cataractogenesis
- •17.14.2 Genetic Effects
- •17.14.2.1 Spontaneous Mutation
- •17.14.2.2 Doubling Dose
- •17.14.2.3 Genetically Significant Dose
- •17.17 Questions
- •References and Suggested Readings
- •18.1 Introduction
- •18.2 Radiation Protection
- •18.2.3 Occupational Dose Limits
- •18.2.4 ALARA Program
- •18.2.5.1 Time
- •18.2.5.2 Distance
- •18.2.5.3 Shielding
- •18.2.5.4 Activity
- •18.2.6 Personnel Monitoring
- •18.2.6.1 Film Badge
- •18.2.6.2 Thermoluminescent Dosimeter
- •18.2.6.3 Optically Stimulated Luminescence Dosimeter
- •18.3 Radiation Regulations
- •18.3.1 License
- •18.3.1.1 General License
- •18.3.1.2 Specific License of Limited Scope
- •18.3.1.3 Specific Licenses of Broad Scope
- •18.3.2 Radiation Safety Committee
- •18.3.3 Radiation Safety Officer
- •18.3.4.3 Supervision
- •18.3.4.4 Mobile Nuclear Medicine Service
- •18.3.4.5 Written Directives
- •18.4 Bioassay
- •18.6 Radioactive Waste Disposal
- •18.6.2 Release into Sewerage Systems
- •18.6.4 Other Disposal Methods
- •18.7 Radioactive Spill
- •18.8 Recordkeeping
- •18.10 Dirty Bombs
- •18.11 Types of Accidental Radiation Exposure
- •18.12 Protective Measures in Case of Explosion of a Dirty Bomb
- •18.13 Verification Card for Radioactive Patients
- •18.14 Radiation Phobia
- •18.15 European Regulations Governing Radiation
- •18.16 Questions
- •References and Suggested Readings
- •Index

318
ab
cd
17 Radiation Biology
Fig. 17.3 Different phases of mitosis. See text for details

M
G
17.2 Eects ofRadiation onCells
319
Fig. 17.4 Phase. M is the
period of mitosis during
which the prophase,
metaphase, anaphase, and
telophase take place. G
the period between the
telophase and S, and G
the period between S
The cell cycle. S is the
DNA synthesis the
prophase
1
2
and.
is
is
G
1
2
S
17.2 Effects ofRadiation onCells
17.2.1 DNA Molecule
The nucleus of the cell is the most sensitive part to radiation and this sensitivity has
been attributed to the DNA molecule. To understand the effect of radiation on the
DNA molecule, a knowledge of its structure is essential. It has a double helical
structure consisting of two strands, which are like the two rails of a ladder
(Fig.17.5a). The strands are composed of sugars interlinked by phosphate bonds.
The two strands are connected to each other by rungs made of four bases: thymine
(T), adenine (A), guanine (G), and cytosine (C) (Fig.17.5b). The bases are bonded
to the sugar molecule on the strands on both sides, and are paired to each other by
hydrogen bonds. These four bases are arranged in a very specic manner to form a
specic gene in every living species and provide the unique characteristics to these
species.
Radiation damage to the DNA molecule can be due to
(a) Loss of a base
(b) Cleavage of the hydrogen bond between bases
(c) Breakage of one strand of the DNA molecule (single strand)
(d) Breakage of both strands of the DNA molecule (double strand)
These radiation effects on DNA molecules are illustrated in Fig. 17.6. The
changes result in so-called mutations, which have adverse effects on the genetic
code. The number of mutations increases with increasing radiation exposure. At
low-dose exposures, the breaks are single stranded and can be repaired by joining
the broken components in the original order. At higher exposures, however, double
strand breaks occur and the odds for repair decrease. Also, high-LET radiations
cause more damage to the DNA molecule because of the double strand breaks. If the
cell is not repaired, it may suffer a minor functional impairment or a major

320
ab
17 Radiation Biology
Fig. 17.5 (a) Double-helical structure of DNA molecule composed of four bases: adenine (A),
guanine (G), thymine (T), and cytosine (C). (b) Conguration of a DNA molecule: strands are
formed by sugar molecules bonded by phosphate groups. The rungs of the ladder-like structure are
formed by bases connected to each other by the hydrogen band (dashed line) and to the sugar
molecule on the strands on both sides
consequence (cell death). If DNA damage occurs in germ cells, future offspring
may be affected.
17.2.2 Chromosome
Chromosomes are likely to be affected by mutations of the DNA molecules.
However, chromosomes themselves can be cleaved by radiation, producing single
or double breaks in the arms. These structural changes are called aberrations,
anomalies, or lesions. These aberrations are categorized as chromatid aberrations
and chromosome aberrations. In chromatid aberrations, irradiation occurs after
DNA synthesis, prior to mitosis, and thus only one chromatid will be affected. On

17.2 Eects ofRadiation onCells
a
b
c
d
321
e
f
Fig. 17.6 Illustration of radiation effects on DNA molecules: (a) Normal DNA molecule; (b)
hydrogen bond is broken without the loss of the base; (c) hydrogen bond is broken with the loss of
the base Τ; (d) single strand break that can repair; (e) double strand breaks which are well separated and can repair; (f) double strand breaks that are too close to repair

322
ab
17 Radiation Biology
the other hand, in chromosome aberrations, irradiation occurs after mitosis, prior to
DNA synthesis, and hence the broken chromatids will be duplicated, producing
daughter cells with damaged chromosomes.
Whether chromosome aberrations are induced by single-strand breaks or doublestrand breaks in the structure determines the fate of the cell. In single-strand breaks,
the chromosome tends to repair by joining the two fragments in a process called
restitution, provided sufcient time is allowed. The cell becomes functionally normal and replicates normally (Fig.17.7a). However, if the fragments are replicated
during DNA synthesis prior to restitution, two strands with centromeres and two
strands without centromeres will be produced. Random combination of these fragments will then produce acentric and dicentric chromatids as illustrated in Fig.17.7b.
Such chromosomes suffer severe consequences due to the mismatch of genetic
information.
If radiation produces single-strand breaks in two separate chromosomes, then
there are four ways of recombining the broken ends as shown in Fig.17.8. The
dicentric and acentric combinations (Fig.17.8a) are similar to those formed after
replication of single strands in the same chromosome shown in Fig.17.7b. However,
these cells suffer severe consequences because of the mismatch of genetic information from two separate damaged chromosomes. The translocation is a process in
which two fragments—one with a centromere from one chromosome and one without a centromere from another chromosome—combine to form a new chromosome
(Fig.17.8b). In another scenario, radiation can cause two breaks in one arm of a
chromosome, resulting in three fragments, only two of which combine with the loss
of the third. Such a process is called deletion (Fig. 17.9a). Translocation and
Fig. 17.7 (a) Illustration
of restitution, in which the
fragments produced by a
single-strand break in one
arm of the chromosome by
radiation join together to
produce the original
chromosome. (b)
Formation of dicentric and
acentric chromosomes by
the combination of the
fragments, after replication
from a single-strand break
in a chromosome
Restitution
Replication
Dicentri c Fragment

Acentric Fragment Translocation
17.2 Eects ofRadiation onCells
Dicentric Fragment
323
Fig. 17.8 Single-strand breaks in one arm of each of two separate chromosomes. A combination
of these four fragments leads to dicentric and acentric chromosomes (a) or translocation (b)
deletion, although not as harmful to the cell, causes late effects such as carcinogenesis and hereditary effects due to mismatch or loss of genetic material. An alternative to deletion is the combination of all three fragments into a chromosome with
changes along the broken line as shown in Fig.17.9b. This process is called inversion, which has all the original genetic material except for a change in the sequence
of genes and hence is not as detrimental to the cell.
Repair of chromosomes after irradiation depends on the sites of break in the
DNA molecule or the chromosome, the total radiation dose, the dose rate, and the
LET of the radiation. Chromosome aberrations by double-strand breaks occur more
frequently at high-dose rates than at low-dose rates because of less time to repair
and fewer chances of combining two fragments in the correct sequence of genes.
High LET radiations cause more double-strand breaks in chromosomes than lowLET radiations, and thus repair becomes difcult in the former. For example,
α-particles, protons, and neutrons will cause more chromosome aberrations
than γ-rays.

324
ab
Fig. 17.9 Two breaks in
one arm of a chromosome
producing three fragments.
(a) In deletion, two of the
fragments combine with
the loss of the third, or (b)
in inversion, all three
fragments combine with
the interchange of
positions
17 Radiation Biology
Deletion
Inversion
17.3 Direct andIndirect Actions ofRadiation
The DNA molecule of a cell is the most sensitive target to radiation. Radiation damage to the cell can be caused by the direct or indirect action of radiation on the DNA
molecules. In the direct action, the radiation hits the DNA molecule directly, disrupting the molecular structure (Fig.17.10). Such structural change leads to cell
damage or even cell death. Damaged cells that survive may later induce carcinogenesis or other abnormalities. This process becomes predominant with high-LET
radiations such as α-particles and neutrons, and high radiation doses.
In the indirect action, the radiation hits the water molecules, the major constituent of the cell, and other organic molecules in the cell, whereby free radicals such
as perhydroxyl (HO2•) and alkoxy (RO2•) are produced. A variety of reactions that
can occur after radiation interacts with water molecules is shown below.
HO energy HO e
22
HO e HOH
2
HO HOH free radical
2
HOH
OH H free radical
HOHHO
HOHHO
OH OH HO
H
OHOperhydroxyl radical
22
2
2
22

17.3 Direct andIndirect Actions ofRadiation
325
Fig. 17.10 Illustration of direct and indirect action of radiation on the DNA molecule. In direct
action, radiation hits the DNA structure directly, whereas in indirect action, radiations produce free
radicals in the cytoplasm, which react adversely with the DNA molecule to cause structural damage
Free radicals are characterized by an unpaired electron in the structure, which is
very reactive, and therefore reacts with DNA molecules to cause molecular structural damage (Fig.17.10). Hydrogen peroxide, H2O2, is also toxic to the DNA molecule. The result of indirect action of radiation on DNA molecules is the impairment
of function or death of the cell. The number of free radicals produced by ionizing
radiation depends on the total dose but not on the dose rate. It has been found that
the majority of radiation-induced damage results from the indirect action mechanism because water constitutes nearly 70% of the composition of the cell.

326
17 Radiation Biology
17.4 Radiosensitivity ofCells
In living matter, there are two types of cells: differentiated and undifferentiated.
Undifferentiated cells do not have any specic physiologic function except to
develop into mature cells. They undergo mitosis and serve as the precursors for
mature cells. In contrast, all mature cells are differentiated and perform specic
functions in the living body. For example, red blood cells (RBCs) are mature and
differentiated cells performing the function of oxygen carriers, whereas erythroblasts are undifferentiated cells that develop into RBCs through mitosis.
According to the law of Bergonié and Tribondeau, undifferentiated cells that are
undergoing active mitosis or mature cells are least affected by radiation. For example, in a sample of mixed RBCs, erythroblasts are most damaged and mature RBCs
are least affected by radiation. Undifferentiated cells that are killed by radiation may
be replaced by new cells, but those that survive with defective DNAs can induce late
effects, such as cancer (see later). In contrast, the S phase of DNA synthesis in the
cell cycle is least radiosensitive. Radiosensitivity is best assessed by cell death. For
differentiated cells, it means loss of cellular function, whereas for undifferentiated
cells it means loss of reproductivity.
Groups of cells and their relative radiosensitivity are listed in Table17.1. As can
be seen, lymphocytes, though mature cells, are most sensitive to radiation, owing to
a large nucleus; nuclear material is more radiosensitive. Nerve cells and muscle
cells are totally differentiated cells and therefore are highly resistant to radiation.
The tissue or organ that contains more radiosensitive cells will be highly radiosensitive and vice versa. For example, bone marrow containing radiosensitive
Table 17.1 Different types of cells and their radiosensitivity
Types of cells
VIM Mature lymphocytes
DIM Myelocytes
MCT Osteoblasts
RPM Spermatozoa
FPM Nerve cells
Adapted from Casarett AP.Radiation Biology. Englewood Cliffs, NJ: PrenticeHall; 1968:168–169
a
VIM vegetative intermitotic, DIM Differentiating intermitotic, MCT multipotential connective tis-
sue, RPM reverting postmitotic, FPM xed postmitotic
a
Erythroblasts
Spermatogonia
Intestinal crypt cells
Basal cells of epidermis
Spermatocytes
Chondroblasts
Endothelial cells
Granulocytes
Erythrocytes
Osteocytes
Muscle cells
Fibrocytes
Radiosensitivity
Highly sensitive
Relatively sensitive
Intermediate sensitivity
Relatively resistant
Highly resistant

log/
eq
nDD=
17.5 Cell Survival Curves
327
erythroblasts is very radiosensitive, whereas nerves and muscles containing radioresistant cells are less radiosensitive. Following irradiation of blood, depressed blood
counts are observed as follows: lymphocytes on the same day, granulocytes in
3days, platelets in 6days, and RBCs in 10days.
17.5 Cell Survival Curves
When mammalian cells are irradiated, not all cells are affected to the same extent.
Different factors such as the total dose, the dose rate, the LET of the radiation, the
particular stage of the cell cycle (M, G1, S, or G2) and the type of cell will affect the
radiation-induced damage. Some cells may die, and some will survive. The cellular
response to radiation is illustrated by what is called the cell survival curve. It is
obtained by plotting the dose along the linear X-axis and the surviving fraction
along the logarithmic Y-axis. Surviving cells are those cells that retain all reproductive as well as functional activities after irradiation, whereas the death of cells is
indicated by the loss of their function in differentiated cells and by the loss of reproductive activity in undifferentiated cells. It should be noted that thousands of grays
are needed to kill differentiated cells, whereas only hundreds of grays are needed for
undifferentiated cells.Typical cell survival curves are shown in Fig.17.11. For high-
LET radiations such as α-particles and low-energy neutrons, the survival curves are
nearly a straight line starting from the lowest doses. In contrast, for low- LET radiations (e.g., x- and γ-radiations), the survival curve exhibits an initial shoulder, followed by a straight line. This straight line portion on the semilog plot is an
exponential curve on a linear plot. This curve based on a multitarget model is char-
acterized by three parameters: D0 (dose at which 37% of cells survive), the extrapolation number n, and the quasithreshold dose Dq, and they are related by the
expression.
The quasithreshold dose, D
, is the dose given by the width of the shoulder of the
q
0
curve. The Dq indicates that, at low doses, almost all cells repair after irradiation,
and cell killing is minimal, which is due to very limited radiation damage to the cell.
D0 is determined from the slope of the straight line portion of the survival curve. It
is the dose that kills 63% of the total number of cells. The value of D0 is a measure
of radiosensitivity of a given type of cell. For example, a large value of D0 for a type
of cell means that the cells are less radiosensitive and vice versa.
The extrapolation number n is obtained by extrapolating the straight line portion
of the survival curve back to the Y-axis. Its value depends on the width of the shoulder of the survival curve, that is, the quasithreshold value, D
. Its value for mam-
q
malian cells varies between 1 and 10.
(17.1)
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