PERTEMUAN VIII (Aplikasi Persamaan Differensial ) Population Dynamics: Example: 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? 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)? VII-1 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 . 3. The graph of the solution P(t) is as follows: 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 VII-2 Then, the non-constant solutions can be generated by separating the variables , and the integration . 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 VII-3 where C is a constant parameter. Remark: We may rewrite the non-constant solutions as , 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 , VII-4 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). 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. Example: SOLUTIONS TO SOME OF THE APPLICATION PROBLEMS VII-5 Example: Example: A tank holds 100 gallons of liquid. The tank is half full with a salt water solution that contains 0.1 lb of salt per gallon. Pure water is added to the container at the rate of 2 gallons per minute and at the same time one gallon of salt water per minute is removed from the tank. Assume that the concentration of salt in the water in the tank remains uniform throughout. When the tank becomes full it begins to overflow and at that time a total of 2 gallons per minute of salt water will be leaving the tank. Construct a piecewise continuous function S(t) that gives the amount of salt in the tank as a function of time t where t = 0 represents the time when the 2 gallons per minute of pure water began being added to the tank and the 1 gallon per minute of "well-stirred, uniform" mixture began exiting VII-6 the tank. The picture at the right shows the amount of salt in the tank as a function of time. VII-7 Example: Here is an example of the logistic equation which describes growth with a natural population ceiling: The solutions of this logistic equation have the following form: VII-8 Equilibria of Autonomous Equations Example. Draw some solutions for the equation Answer. Note that this equation models the logistic growth with threshold. The equilibria or constant solutions are given by or y = 0, y = 2, and y = 5. The graph of the function f(y) = .2y(5-y)(y-2) is given in the next picture So we have: the solution which satisfies the initial condition is increasing. Moreover we have , with , VII-9 the solution which satisfies the initial condition decreasing. Moreover we have , with , is the solution which satisfies the initial condition increasing. Moreover we have , with , is the solution which satisfies the initial condition decreasing. Moreover we have , with , is In the picture below we draw some solutions Phase Line VII-10 Let us reconsider the above example. Let us focus our attention on the solutions which satisfy the initial condition already know that and . We It is somehow amazing that this conclusion is valid regardless whether is close to 5 or close to 2. In this case we say that the equilibrium point 5 is attractive from below. In fact, in this example, this equilibrium point is attractive from below and above. On the other hand, the solutions get away from the equilibrium point 2 from below and above. We will say that the equilibrium point 2 is repelling. Note that there is no general agreement on the words used to describe these phenomena. Example. Classify the equilibrium points of the equation as source, sink, or node. Answer. The equilibrium points are 0, 2, and 5. Using the above results, we see that 0 and 5 are sinks while 2 is a source. Example. Find and classify the equilibrium points of the equation as source, sink, or node. Answer. It is easy to see that the only equilibrium point is 0. Since VII-11 is always positive, then the solutions will always be increasing. Using previous results, we conclude: if y(t) is a solution satisfying y(0) < 0, then we have if y(t) is a solution satisfying y(0) > 0, then we have Hence, the equilibrium point 0 is a node. In the picture below we draw some solutions. There is a very nice way to put all this information together. Indeed, draw a vertical line (where the variable describing it is y) and start by marking the equilibrium points of the equation VII-12 on the y-axis. Then using the sign of f(y), we draw arrows pointing upward in a region where f(y) is positive, and downward in a region where f(y) is negative. This vertical line is called the phase line of the equation. An equilibrium point is a sink, if the arrows on both sides point towards the equilibrium point, and it is a source, if both arrows point away from it. TERIMA KASIH VII-13 VII-14
© Copyright 2026 Paperzz