The fundamental question we ask ourselves about radiation's effect on biological tissue is: how much damage will a given amount of radiation cause? The answer, glibly, is: it depends. This unit is about what the response depends on.
There are, broadly, two kinds of modifiers: biological modifiers and physicochemical modifiers. We will treat the biological modifiers first. This constitutes a reversal of our normal practice: for the most part we've covered physics and chemistry first and moved on to biology only afterward.
There are a variety of ways that a biological system introduces its own set of modifiers to its response to radiation. An obvious way is the variation associated with cell type and tissue type. Cells that divide frequently are more radiation-sensitive than those that divide rarely. Tissues that are made up of rapidly dividing cells are similarly radiation-sensitive. It is fairly easy to understand this: the more frequently cells divide, the more likely it is that radiation-induced damage to DNA will manifest itself in phenotypic alterations at mitosis rather than being repaired somewhere along the cell cycle. Cells that are fully oxygenated tend to be more sensitive than those that are less well-oxygenated. The reasons for this will be discussed later in the lecture.
Probably the most evident biological mechanism that introduces variability in response to radiation is the cell cycle. This is a large subject, and a quick review of what constitutes the cell cycle is in order.
Cells that go through periodic cell division, i.e. all cells except terminally differentiated cells that are destined never to divide again, are considered to pass through four phases within a single life cycle, i.e. in the progression from one cell division to the next. These four phases are known as: the mitotic (M), presynthetic (G1), synthetic (S), and postsynthetic (G2) phases. Cells are more sensitive to radiation damage at certain phases than at others, and they are more prone to delays in the cell-cycle velocity at some stages than others. The properties of these phases relevant to radiation biophysics are as follows.
Phase | Symbol | Timespan | Defining Activity | Radiation Sensitivity |
Radiation-induced Cycle Delay |
Mitotic | M | 5-10% | Cell Division |
Sensitive | |
Presynthetic | G1 | 10-50% | Preparation for DNA synthesis | Moderate | Minimal |
Synthetic | S | 30-50% | DNA Synthesis | Insensitive | Substantial |
Postsynthetic | G2 | 15-25% | Preparation for mitosis | Sensitive | Substantial |
Thus the least sensitive cells are those in the synthetic phase, particularly the later part of the S phase. The most sensitive are those in the G2 and M phases. It is likely that the radio-resistance is strong in the S phase because the DNA repair enzymes that allow radiation-induced damage to appear in DNA are at full activity during S phase and less so at other stages. During G2 and M the DNA is packaged in chromosomes, where the repair enzymes would have difficulty operating. The mechanisms by which cell progression is delayed by radiation are less well understood. There are several protein kinases involved in regulating the cell cycle, and it may be that radiation-induced degradation of the these kinases slows the cycle.
The first physical or chemical effector of the sensitivity of tissue to radiation that we will discuss is water. We recall that much of the damage from radiation is mediated through free radicals derived from water (OH., H., O2-.) and energetic ions produced in water. The radicals and high-energy ions are responsible for damage to DNA and other biomolecules, so the less water we have in a system, the less damage will occur-- all other things being equal, which they rarely are.
This dependence on water availability, i.e. on the concentration of
water, is almost irrelevant to biology. The molarity of pure water is
ρM, where ρ is
the density of water and M is its molecular weight. Thus water is
(1 kg/L) / [ (18 g/mole) * (0.001 kg / g) ] = 55.5M.
Even in biological systems that contain high concentrations of salts
and other solutes the water activity will be only slightly lower than this
maximum value of 55.5M, so variations based on differences in water
availability matter little.
Temperature
Another physical effector is temperature. Most chemical reactions
proceed more rapidly at high temperature than at low; typically
the log of the reaction rate is linearly related to the inverse of
the Kelvin temperature, with a negative slope.
The slope is equal to -ΔG / R,
i.e. the activation energy of the reaction divided by the gas-law constant:
Thus any chemical reaction will display a temperature dependence that
is relatively easy to characterize. Among the reactions that constitute
the interaction between radiation and biological systems are covalent bond
breakages, restitutions of radicals, and enzymatic repair of damages.
Each of these processes proceeds through a different mechanism, and there
is no reason to expect any two of them to have the same activation energy.
So the overall temperature dependence of some chemical endpoint associated
with irradiation of biological samples will be complex.
The reality is that temperature will rarely matter.
Activation energies associated with biological reactions are small enough
that the difference in rate between, say, 25°C = 298K and
37°C = 310K will be small. Alpen characterizes various categories
of radiation-related reactions in three ranges of temperatures--T <. 100K,
100K < T < 170K, and 170 < T < 420K. Studies in these
first two ranges have little relevance to real biological systems,
and the variability in temperature in the last range is small.
One could use thermal kinetics--that is, the temperature dependence of
reaction rates-- as a way of sorting out the differences between
direct action of radiation, viz.
R-H + hν -> R-H.+ + e-
and indirect action, viz.
R-H + .OH -> R.
+ H2O
since the thermal implications of these two approaches will be different.
But in reality temperature effects are of minor influence on the
biological response to radiation.
Oxygen
A more significant chemical effector is oxygen, based on the following facts:
One of the mechanisms by which oxygen influences radiation response
is damage fixation by oxygen. In this instance a macromolecular
or small-molecule reactant reacts with molecular oxygen, and a peroxyl
radical results:
R. + O2 ->
R-O2.
which is a semi-stable free radical (T1/2 = 10-7 to
10-3), capable of remaining in the
neighborhood of the tissue where it was produced and causing further
damage over the long haul. This oxygen-related mechanism is called
"damage fixation by oxygen". We say that the free radical becomes
"fixed", i.e. stabilized enough so that further damage may arise.
Note that this definition of "fixed" differs almost 180° from the
conventional usage, where "fixed" means "repaired." Reactions like
the one just mentioned can compete with the organism's built-in
mechanisms for scavenging free radicals. An example of these scavenger
mechanisms are the reactions of radicals with sulfhydryl reagents:
R. + R'-SH ->
R-H + R'S.
R'S. +
R'S. ->
R'-S-S-R'
where we show that the most common restitution event with the resulting
organic sulfur free radicals is dimerization.
A series of cell-culture experiments on the influence of oxygen were
conducted in the 1950's.
It was found that survival was diminished in oxygen relative to the results
obtained in nitrogen. Thus the survival curves look like this:
In fact, it is possible to plot the relative sensitivity of a set
of cells to oxygen as a function of the oxygen partial pressure, as shown:
From these considerations we seek a quantitative characterization for the
influence of oxygen on a cell culture. The definition we use is of the
oxygen enhancement ratio or OER, as such:
OER = (dose in N2 for surviving fraction, S / S0) /
(dose in O2 for surviving fraction, S / S0)
That is, we choose a particular survival fraction, say S = S0 / 10,
and determine the radiation dose necessary to reach S both under oxic
and anoxic conditions. Since the cells are more sensitive to radiation under
oxic than oxic conditions, the dose in nitrogen necessary to bring the
survival fraction down to S0 / 10 will be larger than it
is in oxygen. Thus in this figure,
we can define OER = DN2 / DO2:
We wish to fit the data from the plot of relative sensitivity against
partial pressure. Over a reasonable range of oxygen concentrations
a good match to data is obtained from the Howard-Flanders & Alper equation:
S/SN = (m[O2] + K) / ([O2] + K)
where we note that K is in concentration units, i.e. the same units as
[O2], and m must be unitless.
The value m is known as the maximum relative sensitivity, because
if [O2] >> K,
(S / SN) = m[O2] / [O2] = m.
We can also examine plots of S vs. [O2] to obtain K.
We do this by saying that if K == [O2],
then at that particular S value, SK, we find that
SK / SN = (mK + K) / (K + K) = (m+1) / 2.
Some actual values for m and K for three organisms are given below:
Organism | m | K,µM |
Shigella | 2.9 | 4.0 |
E.coli | 3.1 | 4.7 |
S.cerevisiae | 2.4 | 5.8 |
We have already mentioned the role of thiols in protecting cells
from free-radical damage from radiation.
The most important type of thiol present is reduced glutathione,
which is reasonably plentiful in tissues.
It can react with macromolecular free radicals,
[macro]-R. + R'-SH ->
[macro]-R-H + R'-S.,
i.e. a hydrogen atom is transferred from the thiol (glutathione or its
equivalent) to the macromolecule
so that the thiol becomes the free-radical species and the macromolecule
becomes unreactive. The other mechanism by which glutathione exerts its
protecive action is through interactions with small-molecule radicals
that might otherwise react with macromolecules to cause damage.
Formally this is almost an identical reaction:
[small]-. + R'-SH ->
[small]-H + R'-S..
In either case the resulting quasi-stable glutathione (or other sulfhyrdryl)
radical finds a mate and dimerizes:
R'-S. +
R'-S. -> R'-S-S-R'
As a final topic for this week we consider whether there might be
ways to increase the radiation-sensivity of cells in a tumor. If we are
using radiation to kill a tumor, we would like it (the tumor) to be as
sensitive as possible to the tumor, so that we will be able kill it with
minimal damage to the surrounding non-tumorous tissue. Since tumors are
sometimes poorly supplied with oxygen, they are often less
radiation-sensitive than are neighboring non-tumor cells that are dividing
as fast as they are.
The challenge, then, is to devise a way to make the cells in the rapidly
growing tumor as radiation-sensitive at it would be if the partial pressure
of oxygen around the tumor were as high as in healthy tissue.
It is found that certain nitroaromatic compounds, including metronidazole,
,
increase the radiation sensitivity of cells
to levels similar to that of fully oxygenated tissue--provided that
large doses (several millimolar) are used. Toxicity limits the
utility of this method, but if the metronidazole can be administered in
the tumor mass without acute toxicity, it could become an important
adjoint to radiation therapy.