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The purpose of this lab is to familiarize you with some applications from real life involving exponential and logarithmic functions. The diversity of the processes which are described by the natural exponential function appears amazing. In this lab, you will encounter to three very different applications and try to use Maple to simplify computations and visualize behaviors of the processes in time.
The lab consists of Background including both the relevant theoretical notes and description of the use of appropriate Maple commands. There are four problems, each of which has separate preliminary remarks (discussion of equations, introduction of terms, etc.) and an exercise to do.
Theoretical notes. In many natural processes the rate of change of physical quantity (temperature, velocity amount of money, electric current, whatever) is proportional to the current amount of the quantity. If we also know the amount present at time t=0, call it y0, we can find y as a function of t by solving the following initial value problem:
Differential equation: is a constant. (1)
Initial conditions: y = y0 when t = 0 .
If y is positive and increasing, then k is positive, and we use Eq. (1) to say that the rate of growth is proportional to what has already been accumulated. If y is positive and decreasing, then k is negative, and Eq. (1) is used to say that the rate of decay is proportional to the amount still left.
It is seen that the constant function y = 0 is a solution of Eq. (1). To find
the non-zero solutions, the equation is solved in accordance with the known
technique of separating variables and integrating. The solution
involves the natural exponential function (whose derivatives is the
function itself) and is expressed as
The constant k is called the growth rate in exponential growth (k >0) and the decay rate in exponential decay (k < 0). In a process that can be modeled by exponential functions, the rate constant k depends only on the process and the conditions under which it is carried out.
Some processes are described by differential equations similar to (1) but containing two or more constants characterizing some other circumstances in which these processes are carried out. Also, the initial conditions might be specified by more complicated expressions. The corresponding initial value problems lead to the solution having slightly different form, e.g., like (2) including a combination of additive and multiplicative constants. You will meet illustrations of that in the problems below.
In some applications, a physical quantity varies on a huge range. To make this quantity more convenient to handle, special scales involving logarithms are used. This allows one to deal with the corresponding powers instead of actual values of y .
Relevant Maple Means. In order to enter the exponential and natural logarithmic functions, use the exp and ln command. The syntax of these commands is similar to that of sin and cos. For example, below it is shown how to enter the function f(x) = ex and then evaluate it at x = 0.8.
> f:=exp(x);
> evalf(subs(x=0.8, f));
In the same manner, the function is entered and
calculated. Try the following commands:
> g := ln(x);
> evalf(subs(x=0.8, g));
To simplify expression involving logarithms, use command simplify; it works as
follows:
> simplify(exp(a+ln(b*exp(c))));
The common logarithm is defined by function log10 = log[10], but log10 must be defined with the command readlib(log10) before use:
> readlib(log10): log10(10000);
Maple manipulates with common logarithms the same way but may return expressions including natural logarithms.
The solve command is usually sufficient for solving most problems encountered in your Calculus courses. This command comes in a couple of varieties, as shown below.
> solve (y=n*(x+1)-m(x-1),x);
> solve (5+7*x=39-10*x,x);
Plotting the two functions f(x) = ex and on the same coordinate
system illustrates an idea of the symmetry around the line y=x. All the three
graphs can be plotted by the use of the following command:
> plot({f,g,x}, x=-4..4, y=-4..4);Responding this command, Maple returns the figure as shown in Figure 1.
In order to get a graph of a left-hand/right-hand side of an equation obtained
after symbolic transformations and/or computations, first use commands lhs and
rhs respectively. The example:
> eq1 := A=b+c*exp(k*t): eq2 := subs(b=2.5,c=3,k=0.8,eq1):
> rh2 := rhs(eq2):
> plot(rh2, t=0..3);
When analyzing graphs obtained as the result of your computation, you
may need to plot supplementary or auxiliary straight lines in the same
figure. The following format of the plot command illustrates how the
line y = 60 from x = 0 to x = 20 can be displayed:
> plot({[0,60], [20,60]});
Radioactive decay is a typical example to which the exponential decay model can be applied. In Eq. (2), y represents the mass (in grams) of an isotope, y0 and k are constants determining from initial conditions: y0 is the mass present originally, and k is the decay constant.
k is often specified in terms of an empirical parameter, the half-life of the
isotope. The half-life of a sample of a radioactive isotope is the time
required for half of the atoms of that sample to decay. The half-lives of some
common radioactive isotopes are as follows:
Uranium (U-238) | 4,510,000,000 years | |
Plutonium (Pu-239) | 24,360 years | |
Carbon (C-14) | 5,730 years | |
Einsteinium (Es-254) | 270 days | |
Nobelium (No-257) | 23 sec |
The relationship between k and is set up from
the condition saying that the sample of y0 grams will
contain only
grams after the time
, so that, referring to equation (2):
and therefore:
The worst nuclear accident in history happened on April 26, 1986 at
01:23 a.m. (GMT +03:00) at the Chernobyl nuclear
plant 60 miles north of Kiev in the Ukraine. An explosion destroyed one of the plant's four
reactors, releasing large amount of radioactive isotopes into the
atmosphere. For almost two weeks the radiation continued to escape
and clouds settled onto villages, towns, and forests across wide
stretches of Ukraine, Belarus, and neighboring parts of Russia. About
300,000 people were evacuated from the fallout areas. The estimate of
the accident's ultimate death toll varies from several thousand to
half a million deaths. (For more information, see `The Chernobyl
Nuclear Accident'* site at Geocities.com)
* www.geocities.com/RainForest/Canopy/3643/chern.html
Consider 20 grams of the plutonium isotope Pu-239 released in the Chernobyl nuclear accident.
Base 10 logarithms, often called common logarithms, appear in many scientific and applied formulas.
For example, earthquake intensity is often reported on the logarithmic Richter
scale. Here the formula is
where a is the amplitude of the ground motion in microns at the receiving
station, T is the period of the seismic wave in seconds, and B is an
empirical factor that allows for the weakening of the seismic wave with
increasing distance from the epicenter of the earthquake. For an earthquake
10,000 km from the receiving station, B = 6.8. Thus if the recorded vertical
ground motion is a = 10 microns and the period is T = 1 sec, the
earthquake's magnitude, following (7), is R = 7.8. An earthquake of this
magnitude does great damage near its epicenter.
Another example of the use of common logarithms is the decibel scale using,
particularly, for measuring loudness. (The decibel unit is named in honor of
Alexander G. Bell (1847-1922), inventor of the telephone.) If I is the
intensity of sound in watts per square meter, the decibel level of the sound
is
where I0 is an intensity of 10-12 watts per square meter corresponding
roughly to the faintest sound that can be heard.
When tuning the rock band's equipment before the concert in a big concert hall, an audio engineer finds that in order to maintain appropriate loudness in this hall, he needs to increase the power of the amplifiers compared with the level used for the previous concert in a smaller hall. Use formula (8)
An aluminum beam brought from the outside cold into a machine shop where the regular normal temperature is maintained warms up to the temperature of the surrounding air. A hot silver ingot immersed in water cools to the temperature of the surrounding water.
In situations like these, the rate at which an object's temperature is changing at any given time is approximately proportional to the difference between its temperature and the temperature of the surrounding medium. This observation is sometimes called the Newton's Law of Cooling, although, as in the case with the aluminum beam, it applies to warming as well.
An equation representing this law is derived from a corresponding
differential equation and can be written as
where T is the temperature of the object at time is the surrounding
temperature, T0 is the value of T when t = 0.
Thomas Robert Malthus (1766-1834), English economist and sociologist, was a pioneer in modern world population study. In An Essay on the Principle of Population (1798; rev. ed. 1803) he suggested that populations tend to increase exponentially, whereas resources which support populations (e.g., food) tend to grow only linearly. So poverty, distress, wars, famine are unavoidable because population increases faster than the means of subsistence.
The differential equation (1) may be regarded as a mathematical model of the
changing population according to Malthus. Thus population P(t) with constant
birth rate and constant death rate
is given by
where P0 = P(0) and is called the Malthusian parameter.
If t is measured in years, it represents the annual growth rate, which,
depending on the relationship between
and
, can be positive,
negative, or zero.
However, equation (3) describes only the simplest ideal situation, in which
the inner impulse of the population to expand is given a completely free rein;
it does not take into account any of the inhibiting factors that put a ceiling
on the possible size of a real population. It is obvious, for example, that
the human population of the earth can never expand to the stage where there
will be only a small fraction of an acre of usable land per person. Long
before the point is reached at which the whole surface of the earth becomes
teeming slum, the rate of population growth will be forced down; social,
psycological, and economic effects will depress the birth rate and
increase the death rate
.
In about 1840 the Belgian mathematician Pierre-Francoise Verhulst proposed a population growth model which takes into account the possible limitation of population size due to limited resources. It is called logistic model. When the population P(t) is small, it tends to grow at a rate proportional to itself; but when it becomes larger, P(t) grows at a smaller rate. If L is the largest population beyond which the population cannot grow, the rate of growth of the population is assumed to be proportional to P and to (L - P), so that
The solution of equation (4) subject to the condition that P = P0 when t = 0 is obtained by separation of variables and eventually yields
Since and
depend on time, parameter k in (5) is
interpreted as not their difference but rather as the maximum possible
rate of population growth which is the net effect of birth and death rates.
In accordance with some environmental and demographic studies, the earth will not support a population of more than 16 billion. It is also known that there were 2 billion people in 1925 and 4 billion people in 1975.
Christine Marie Bonini