PERTEMUAN VII A p l i k a si PD Linear & PD Bernoulli IV-1 IV-2 Example : 2 IV-3 Example : 3 Example 4 : A radioactive isotope has a half-life of 16 days. You wish to have 30 g at the end of 30 days. How much radioisotope should you start with? IV-4 Solution: Since the half-life is given in days we will measure time in days. Let Q(t) be the amount present at time t and looking for (the initial the amount we are amount). We know that , where r is a constant. We use the half-life T to determine r. Indeed, we have Hence, since , we get Newton's Law of Cooling Example 5 From experimental observations it is known that (up to a ``satisfactory'' approximation) the surface temperature of an object changes at a rate proportional to its relative temperature. That is, the difference between its temperature and the temperature of the surrounding environment. This is what is known as Newton's law of cooling. Thus, if is the temperature of the object at time t, then we have IV-5 where S is the temperature of the surrounding environment. A qualitative study of this phenomena will show that k >0. This is a first order linear differential equation. The solution, under the initial condition , is given by Hence, , which implies This equation makes it possible to find k if the interval of time and vice-versa. is known Example 6 : Time of Death Suppose that a corpse was discovered in a motel room at midnight and its temperature was room is kept constant at dropped to . The temperature of the . Two hours later the temperature of the corpse . Find the time of death. Solution: First we use the observed temperatures of the corpse to find the constant k. We have . In order to find the time of death we need to remember that the temperature of a corpse at time of death is (assuming the dead person was not sick!). Then we have IV-6 which means that the death happened around 7:26 P.M. One of our interested readers, E.P. Esterle, wrote a program that helps find the time of death based on the above notes. Click HERE to download it. Have fun with it. Population Dynamics Here are some natural questions related to population problems: What will the population of a certain country be in ten years? How are we protecting the resources from extinction? More can be said about the problem but, in this little review we will not discuss them in detail. In order to illustrate the use of differential equations with regard to this problem we consider the easiest mathematical model offered to govern the population dynamics of a certain species. It is commonly called the exponential model, that is, the rate of change of the population is proportional to the existing population. In other words, if P(t) measures the population, we have , where the rate k is constant. It is fairly easy to see that if k > 0, we have growth, and if k <0, we have decay. This is a linear equation which solves into IV-7 , where is the initial population, i.e. . Therefore, we conclude the following: if k>0, then the population grows and continues to expand to infinity, that is, if k < 0, then the population will shrink and tend to 0. In other words we are facing extinction. Clearly, the first case, k > 0, is not adequate and the model can be dropped. The main argument for this has to do with environmental limitations. The complication is that population growth is eventually limited by some factor, usually one from among many essential resources. When a population is far from its limits of growth it can grow exponentially. However, when nearing its limits the population size can fluctuate, even chaotically. Another model was proposed to remedy this flaw in the exponential model. It is called the logistic model (also called Verhulst-Pearl model). The differential equation for this model is , where M is a limiting size for the population (also called the carrying capacity). Clearly, when P is small compared to M, the equation reduces to the exponential one. In order to solve this equation we recognize a nonlinear IV-8 equation which is separable. The constant solutions are P=0 and P=M. The non-constant solutions may obtained by separating the variables , and integration The partial fraction techniques gives , which gives Easy algebraic manipulations give where C is a constant. Solving for P, we get If we consider the initial condition IV-9 (assuming that P0 is not equal to both 0 or M), we get , which, once substituted into the expression for P(t) and simplified, we find It is easy to see that However, this is still not satisfactory because this model does not tell us when a population is facing extinction since it never implies that. Even starting with a small population it will always tend to the carrying capacity M. Population Dynamics : Example: 7 Let P(t) be the population of a certain animal species. Assume that P(t) satisfies the logistic growth equation 1. Is the above differential equation separable? 2. Is the differential equation autonomous? IV-10 3. Is the differential equation linear? 4. Without solving the differential equation, give a sketch of the graph of P(t). 5. What is the long-term behavior of the population P(t)? 6. Show that the solution is of the form Find A and B. Hint: Use the initial condition and the result of 5. 7. Where is the solution's inflection point? Hint: This can be done without using the answer of 6. 8. What is special about the growth rate of the population P(t) at the inflection point (found in 7)? Answer: 1. This differential equation is autonomous, i.e. the variable t is missing. Therefore, this equation is indeed separable. 2. The answer is Yes! (see 1.) Every autonomous differential equation is separable. 3. The equation is not linear because of the presence of . 4. The graph of the solution P(t) is as follows: IV-11 5. Clearly, because of the initial condition (see the graph of the solution below), we have , 200 being the carrying capacity. 6. Let us solve this equation (use the technique for solving separable equations). First, we look for the constant solutions (equilibrium points or critical points). We have Then, the non-constant solutions can be generated by separating the variables , and the integration IV-12 . Next, the left hand-side can be handled by using the technique of integration of rational functions. We get , which gives Hence, we have . Easy algebraic manipulations give , where . Therefore, all the solutions are where C is a constant parameter. Remark: We may rewrite the non-constant solutions as , IV-13 where a and B are two parameters. If we use the conditions we will be able to get the desired solution. Indeed, we have Thus, and consequently . 7. From the graph (see 4.), the graph of P(t) has an inflection point between 0 and 200. Let us find it. Since we must have P''(t) = 0, we get , where we used the chain rule and the fact that . Since our solution is not one of the two constant solutions we are only left with the equation This simplifies to , which gives P=100 (half-way between 0 and 200). IV-14 Remark: You still need to convince yourself that t=100 is indeed the inflection point, that is the second derivative changes sign at that point. 8. The growth rate at t=100 is maximal. Population Dynamics: Example: 8 The fox squirrel is a small mammal native to the Rocky Mountains. These squirrels are very territorial. Note the following observations: if the population is large, their rate of growth decreases or even becomes negative; if the population is too small, fertile adults run the risk of not being able to find suitable mates, so again the rate of growth is negative The carrying capacity N indicates when the population is too big, and the sparsity parameter M indicates when the population is too small. A mathematical model which agrees with the above assumptions is the modified logistic model: . 1. Find the equilibrium (critical) points. Classify them as : source, sink or node. Justify your answers. 2. Sketch the slope-field . IV-15 3. Assume N=100 and M=1 and k = 1. Sketch the graph of the solution which satisfies the initial condition y(0)=20. 4. Assume that squirrels are emigrating (from a certain region) with a fixed rate E. Write down the new differential equation. Also, discuss the equilibrium (critical) points under the parameter E. When do you observe a bifurcation? Answer: 1. The equilibrium (or critical) points are the roots of the equation Clearly, we have P=0, P=N, and P=M. Using the graph of , we get the phase-line of the equilibrium points, IV-16 We conclude that P=0 and P=N are sinks, while P=M is a source. 2. The Slope-Field is given by the following graph: IV-17 3. From the Slope-Field, we get the graph of the particular solution satisfying the condition P(0) = 20. 4. First, the new equation is , where E > 0. Clearly, the graph of the function can be obtained by shifting the graph of IV-18 down E-unit along the vertical axis. Clearly we have three cases according to the value of E and the value of f at the local maximum : If 0 < E < f(h), then we have similar behavior as for E=0: If E=f(h), we have two critical points: IV-19 If E > f(h), we have only one critical point: Note that IV-20 Clearly, the bifurcation is happening when E = f (h ). Perkiraan penyebaran AID The HIV Virus invades a white blood cell... Populations usually grow in an exponential fashion at first: IV-21 However, populations do not continue to grow forever, because food, water and other resources get used up over time. Differential equations are used to predict populations of people, animals, bacteria and viruses that are being affected by external events. The logistic equation (developed in the mid-19th century) allows for a growth term AND an inhibition term and it is predicted that the AIDS epidemic will follow the pattern of the logistic equation. If A = number of people affected by the virus at time t, P = the total population (a constant), and c is a constant, then the rate of growth of the virus at time t is given by the differential equation: The term cPA is the growth term and - cA2 is the inhibition term. AIDS Example 9 AIDS is spreading through a city of 50.000 people who take no precautions. The virus was brought to the town by 100 people and it was found that 1000 people were infected after 10 weeks. How long will it take for half of the population to be infected? Solution. Here, P = 50.000 . So our differential equation becomes: Solving using SN gives: IV-22 Exact solution is: Now, we are told that A(10) = 1000 . So now we solve for c: , Solution is: c = 4. 6416 × 10 -6 . So We see in the graph the S-shaped curve which the logistic equation can take. Now to find how long it takes for half the population ( ) to be infected: , Solution is: So we conclude that half of the population will be infected after about 27 weeks. IV-23 Newly Reported AIDS Cases in Australia Year Cumulative Totals 1982 1 1985 50 1988 413 1991 1100 1993 2426 1995 4179 1996 4836 1998 5525 1999 5721 Men: 5439 Women: 282 Total: 5721 We see that the data roughly follows the expected S-shaped logistic equation curve. The decrease in growth in the late 1990s is largely due to suppressant drugs and education. Reported AIDS Cases - Australia NOTE: This data is from several sources and some of it is conflicting. Some sources include "HIV/AIDS" while others "AIDS". TERIMA KASIH IV-24
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