Mathematically Modelling the Post-Mortem Interval (PMI) | Sample IB Math Internal Assessment | Real-Life Application of Logarithms
Introduction
Post
Mortem Interval (PMI) is referred as the time that has elapsed after a person
has expired[1]. PMI is a very reliable source of information that
criminologists can use in order to solve or investigate a particular crime
case. There are number of ways to estimate PMI, such as looking at the changes
in the intestinal content, stage of invasion, blow fly larval development and
so on[2]. These methods give more accurate estimation of PMI
as it is useful in cases with both short PMI and long PMI[1]. But other methods such as Henssge-nomogram and the electrical or mechanical
stimulation of skeletal muscles are only useful for short PMI because at one
point of time the corps will attain the ambient temperature (room temperature)
and stops cooling[1]. This method purely relies on the temperature
factor, the cooling of the corpse. This method of death time estimation is
based on the cooling of the corpse. From my prior knowledge I knew that the
cooling of any object follows an exponential decrease. And so, it was clear
that post mortem interval could be mathematically modeled using exponential
functions. Through this model I aim at arriving at an equation which will help
in estimating the time of death.
This method of estimating PMI is no more in action
due to its limitations mentioned above. However, it is very fascinating to know
how man has been able to translate a real life issue into a mathematical
language and further mathematically model the problem and find a solution for
it. Yet another interesting part which fascinates me the most is the
exponential function and the real world. Right from the very common radioactive
decay, charging and discharging of capacitors, analyzing the population growth,
bacterial growth, predicting cost and revenue in economics, there are number of
applications of exponential function to solve real life problems. Initially I
didn’t have any idea how to go about with this because there were number of
applications based on exponent functions and majority of them were commonly
know and discussed ones. However, my objective of this exploration was to apply
the concept that was learnt in class to a real life scenario and to show how
mathematics as a language expressed in terms of equations, symbols and numbers
has got significance in understanding the world.
Data Collection
To obtain the data and graph for the study, I had
to gather secondary data from authenticated journals since I had no scope of
conducting the experiment at lab. The gathered data shown below is obtained
from ‘Journal of Criminal Law and Criminology’[4]. This data represents the change in rectal
temperature of a corpse with respect to time. This data was recorded on 28th
January 1953 and it is a very old data.
TABLE 1
|
Rectal Temperatures at (°F) |
||||||||||
|
10 am |
11 am |
12 pm |
1 pm |
2 pm |
3 pm |
4 pm |
5 pm |
6 pm |
7 pm |
8 pm |
|
97.7 |
96.8 |
95.8 |
94.8 |
94.1 |
93.3 |
92.7 |
91.9 |
91.1 |
90.4 |
89.9 |
TABLE
2
|
Room Temperature in
Laboratory(°F) |
||
|
Min. |
Max. |
Avg. |
|
79.0 |
82.0 |
80.3 |
From the data shown in TABLE 1, it’s
understood that the temperature of the corpse was recorded at consecutive hours
and the temperature is expressed in terms of Fahrenheit (°F). But for my
convenience, I will be using Celsius (°C) to express the temperature. The
conversion of Fahrenheit to Celsius can be done using the equation:
TABLE
3
|
Rectal Temperature of
the corpse (°C) |
|||||||||||
|
Time (Hours) |
0 |
1 |
2 |
3 |
4 |
5 |
6 |
7 |
8 |
9 |
10 |
|
Temperature (°C) |
36.5 |
36.0 |
35.4 |
34.9 |
34.5 |
34.1 |
33.7 |
33.3 |
32.8 |
32.4 |
32.2 |
Average room temperature: 26.8°C
Methodology
This
graph represents the cooling of a corpse according to the data provided in TABLE
3. I used logger pro to produce the graph with x-axis representing the time
t in hours and y-axis representing temperature in °C. Curve fitting was
added into the graph in order to get a proper visualization of the data since
the available wasn’t enough for further analysis.
It
was surprising to see that the plotted graph was very similar to the curve fit
with RMSE (Root-Mean-Square-Error) value of just 0.06327°C. RMSE basically
means the deviation of values from the true value (in this case the best fit). The
applied curve fit was of the general equation:
Here,
B represents the horizontal asymptote of the function, which I assume it to be
a value close to the ambient temperature. Plugging in the obtained values of A,
C and B from the graph, the curve can be expressed in the form of an
exponential function:
Using
the above equation, the time at which the corpse attains the ambient
temperature can be determined by solving for t. The ambient temperature is
considered to be the average room temperature where the data collection was
taken place and according to TABLE 2, the average room temperature is
26.8°C. Plugging this into the equation, we
get:
This
shows us that, approximately after 39 hours the corpse will attain the ambient
temperature and further there won’t be any major reduction in the body
temperature. Since we know that the function of the curve is:
Graph 2 now gives more visual clarity about the exponential nature of the cooling of a corpse. It can be seen that it follows an exponential decrease and thus the power of exponential being negative. This graph validates the fact that the body will stop cooling when it attains the ambient temperature. In the graph, it can be observed that between 20°C and 30°C on y-axis, the curve becomes a straight line indicating that the body has reached the ambient temperature of around 28.6°C and it cannot decrease way beyond the ambient temperature. The (e.q.1) shows
24.94°C
as the horizontal asymptote carrying an uncertainty of ±1.95. This supports my
assumption that the asymptote will be a value closer to the ambient temperature.
Let’s look upon to a different scenario where in there is no ‘Logger pro’ software determining the function of the graph plotted by providing with appropriate curve fits. It is known that the average body temperature of a normal living human being is around 37°C and from the obtained secondary data (shown in TABLE 3), it can be inferred that the person has just recently expired since the initial rectal temperature reading (36.5°C) is almost near to the average human body temperature (37°C). Taking this into consideration, I will be modeling a hypothetical situation and finding time elapsed since the death of a man.
Situation: An unknown man’s dead body was happened to be found in an abandoned place at 12 pm. The police officers were informed about this by the people who saw the lying dead body. Within in no time an ambulance arrived and the body was taken to a nearby hospital. The man’s body was taken for further medical examination to learn how the person has actually died and when did he die. The rectal temperature of the body was recorded as 34.1°C at 12.30 pm. The rectal temperature was recorded at every hour for 5 hours and the data is shown below. The average room temperature was 26.8°C. (Note that the values shown below are obtained from TABLE 3).
TABLE 4
|
Time (hrs) |
0 |
1 |
2 |
3 |
4 |
5 |
|
Temp (°C) |
34.1 |
33.7 |
33.3 |
32.8 |
32.4 |
32.2 |
From
the data set provided, let’s try to determine the time when the person died. We
don’t have sufficient data set to plot a graph and check whether the cooling of
the corpse has an exponential nature. Therefore, we assume the decrease in
temperature to have an exponential nature and at one point of time the body
stops cooling i.e.it has attained the room temperature.
Assuming the cooling will
follow an exponential nature, further assumptions can be made that:
·
The power of the
exponential will carry a negative value since it’s an exponential decrease
· According to the law of nature, the temperature of the body cannot go down beyond the ambient temperature 26.8°C to a greater extent. Therefore, the horizontal asymptote of this function can be defined as y=26.8.
Based on my 1st assumption, I can mathematically write it as:
Where, T represents
temperature and t representing time.
Based on my 2nd assumption, the graph will be translated 26.8 units up on y-axis because we know that the corpse can’t cool down beyond the ambient temperature and so the graph should converge at y = 26.8. Adding the translation constant Ta which represents the ambient temperature, we get:
Still, we see that the equation is not complete because at t =
0, the temperature T should be equal to 34.1°C. But, when t = 0
is plugged in into the (e.q.2), the temperature is, T = 27.8°C. Also,
graphically we can tell it as incorrect. Plotting (e.q.2) on a graphic
calculator gives us a curve:
Therefore I assumed
multiplying the function e-t from (e.q.2) by 34.1
would give the y-intercept 34.1 at x = 0. But I understood that the vertical
translation constant Tb (ambient temperature, horizontal
asymptote) would change my y value. This made me realize that, in order to get
y-intercept as 34.1 at x = 0, the graph should undergo both vertical and horizontal
stretch or compression
In
order for this, (e.q.2) should be re-written as:
The
general equation can be written as:
Here,
the k represents the vertical stretch or compression along with the y values
and ‘a’ represents the horizontal stretch or compression along the
x-axis.
So, using (e.q.4) let’s solve for k and a, then determine the translation constant along the y-axis and the horizontal translation constant along x-axis.
Now, values should be plugged into (e.q.5). We can algebraically solve the equation by producing 2 different equations and solving them. The values should be taken from the data set provided on TABLE 4.
This
shows that the produced function matches with data set of TABLE 4. So,
let’s estimate the time when the person had actually died. We know that the
average human body temperature is around 37°C. Let’s substitute T= 36.5
(such that we can reflect back onto e.q.1 and check to what extent the
calculating values matches with these values) and find at what value for x does
the value of y becomes 36.5°C in (e.q.8)
This
shows us that the man was dead approximately 5 hours before the body was found.
That is, the person died around 7 in the morning. Comparing this answer with TABLE
3 also confirms the answer to be correct. Using (e.q.8) and
(e.q.1) let’s find the temperature value (function value) of the
body for 10 hours by substituting values for t from 0-10 and compare them with
the original data set provided in TABLE 3.
TABLE 5
|
Time
(hrs) |
0 |
1 |
2 |
3 |
4 |
5 |
6 |
7 |
8 |
9 |
10 |
|
Difference between the temperature values obtained from e.q.1 and
Expt.data |
0 |
0 |
-0.1 |
-0.1 |
-0.1 |
0 |
+1 |
+1 |
-1 |
-1 |
0 |
|
Difference between the temperature values obtained from e.q.8 and
Expt.data |
-0.2 |
-0.1 |
-0.1 |
-0.1 |
0 |
0 |
0 |
0 |
-0.1 |
-0.1 |
0 |
Conclusion
Graphically
analysing, both (e.q.1) and (e.q.8) gave out identical graphs
without any major difference (Graph 7) except for the y-intercept being
different. It was good to see that the logically produced equation (e.q.8)
suited with (e.q.1) produced by the software by applying a best fit curve.
However, a reference graph of the experimental data could have been used for
comparison and check to what extend did the graphs produced from (e.q.1)
and (e.q.8) deviate from the original graph. But sufficient data wasn’t
available to plot such a graph because cooling of a corpse is a very slow
process and so, it takes lots of time to record sufficient data in order to
produce such a graph for comparison. Yet another limiting factor is that, these
dead bodies must not be kept out for a long period of time as the human organs
starts to decompose and produces virtually intolerable smell and so they are
refrigerated. However, with the available data of 10 hours, (e.q.1), (e.q.8)
and the experimental values are plotted on the same axes for comparison. It is
observed that there isn’t any major deviation of values from the experimental
value. Determining the mean error for each equation shown on TABLE 5, it
can be deduced that (e.q.1) lies more closer to the experimental value
than (e.q.8) signifying that values of (e.q.1) being more
accurate.
The justification for why (e.q.1) gave out
comparatively a bit more accurate data is because, (e.q.1) was produced
using a best fit curve approach and so the best fit line would have taken
account of the slight variations in the temperature. According to the original
data, the average room temperature was recorded as 26.8°C and so the vertical
translation constant, Tb in the equation should have been 26.8.
But then we find in (e.q.1) that the value for Tb
is given as 24.94°C. This shows that the rate in change in temperature
shown in TABLE 3 was not due to the average ambient temperature being
26.8°C alone but due to 24.94°C with an uncertainty of ±1.95°C. From this, it
can be understood that ambient temperature came around in the range 26.8°C -
23°C. In case of the hypothetical situation, it was determined that the man was
happened to be dead 5 hours before his body was found. But in
reality, this value needn’t be true as the ambient temperature needn’t be the
same every time since the time the person has expired and temperature is most
likely to be lesser than 26.8°C in the morning, so at that point of time, the
rate at which the body cools will also vary from what we have generalized. This
shows the discrepancy involved in this particular mathematical modeling. In
order to overcome this, multiple parameters must be included into the modeling
which makes the equation more and more complex.
However,
I was able to solve the hypothetical scenario using this model even though
there existed slight anomalies in the data produced. So rather than
’determining’ post-mortem interval, it would be accurate to say, ‘estimating’
the post-mortem interval. After all, this has made me more curious to explore
real life problems and how the mathematic concepts learnt in class can be
applied solve real life situations.
Bibliography
[1] H. T. Gelderman, L. Boer, T. Naujocks, A.
C. M. Ijzermans, and W. L. J. M. Duijst, “The development of a post-mortem
interval estimation for human remains found on land in the Netherlands,” Int.
J. Legal Med., vol. 132, no. 3, pp. 863–873, 2018.
[2] R. Sharma, R.
Kumar Garg, and J. R. Gaur, “Various methods for the estimation of the post
mortem interval from Calliphoridae: A review,” Egypt. J. Forensic Sci.,
vol. 5, no. 1, pp. 1–12, 2015.
[3] C. Henßge and
B. Madea, “Estimation of the time since death in the early post-mortem period,”
Forensic Sci. Int., vol. 144, no. 2–3, pp. 167–175, 2004.
[4] G. Webster and N. Kathirgamatamby,
“Post-Mortem Temperature and the Time of Death,” vol. 46, no. 4, 1956.
















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