# 2 A Differential Equations Primer

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1 A Differential Equations Primer Homer: Keep your head down, follow through. [Bart putts and misses] Okay, that didn't work. This time, move your head and don't follow through. From: The Simpsons.1 Introduction An ordinary differential equation (ODE) is an equation involving the derivative of an unknown function of a single variable. In working with such equations our objective is to understand something about the function(s) that satisfy the equation. The most obvious goal might be to find eplicit formulas for the solutions. We have alrea tackled that problem for the simplest ODEs in Chapter 1, although from a slightly different perspective. Eample.1: Find all functions y that satisfy the differential equation 1 d = +. In effect, the differential equation provides a formula for the derivative of the unknown function. We have to find all functions with the given derivative. This is just the antidifferentiation problem 3 we addressed in Chapter 1. Integrating the right side of the ODE we obtain that y = + + C.! 3 Eample.1 was particularly simple because the ODE epressed the derivative of the unknown function in terms of the independent variable. In general, the differential equations we will encounter will not be of such a simple form. A more typical and important eample is Eample.: Find all solutions of the differential equation y d =. (.1)! In words, this equation says that differentiating the unknown function returns the original function. From our differentiation review in Chapter 1 we know that y = e has this property since ( e ) = e. So y = e is certainly a solution of this differential equation. However, in Eample.1 we found infinitely many solutions of the ODE as the constant C in the solution formula varies. We would like to find a similar family of solutions to (.1). Trying the obvious, we consider y = e + C and ask whether or not this satisfies (.1). To test whether an epression y satisfies a differential equation we find and see if it is equal to the right side of the differential d equation, when the latter is epressed in terms of the independent variable. 17

2 Differential Equations d Here we find that ( e C ) e = + = and since the right side is just y = e + C, the differential d d equation is not satisfied ecept when C =. However, if we instead consider y = Ce then we d find that = ( Ce ) = Ce = y, so that these functions are solutions of the differential d d equation.! These two eamples illustrate two characteristics of ODEs. First, the equation will epress d in terms of either the independent or dependent variable or both. Second, the equation will usually have an infinite number of solutions epressible by varying some arbitrary constant. This family of solutions is called the general solution of the differential equation. To single out a unique solution we must specify some additional information, as in the net eample. Eample.3: Find the solution of = y that satisfies () 1 d y =. We use the general solution y = Ce found in Eample. (a systematic method for finding these solutions will be discussed in the net section). Since when = we are supposed to have y = 1, we can substitute this information into the general solution to determine C : 1 () = y = Ce = C. Thus, the specific solution we want is y = 1e.! The data consisting of a differential equation together with a numerical value of the unknown function is called an initial value problem. Quite often, as in Eample.3, the function value will be the value of y at =, but a value at some other value may be given instead. This piece of information is referred to as the initial condition. For most problems there is a unique solution of the differential equation that satisfies the given initial condition.. Separation of Variables At this point the only type of ODE we can solve is one of the form y = f( ), provided we can compute the antiderivative of f( ). In this section we develop a technique that can be used to solve many differential equations. The method applies to what are called separable equations - those for which the right side can be factored into a product or quotient of epressions, each of which involves only the independent or dependent variable. 18

3 Eample.4: Determine which of the following differential equations is separable. a) y d = + b) y 1 d = c) yy ( 1) d = + d) d = + y Differential Equations a) The right side may be factored as y+ ( 1), which meets the condition for separability. b) The right side is the quotient of a function of y divided by a function of. Therefore, this equation is separable. c) The right side can be thought of as a product yy+ ( 1) 1, where the constant factor 1 can be viewed as a function of. Therefore, the equation is separable. d) The right side cannot be factored as a product of a function of and a function of y. Therefore, this equation is not separable.! The idea behind the method of separation of variables is to multiply or divide both sides of the separable differential equation by suitable factors so that all the y terms wind up on the left side, together with the unknown derivative, and all the terms wind up on the right side. Following that step, we then have two big hurdles to overcome. First, we must be able to integrate both sides of the transformed equation. Second, even after integrating, we will not usually have an eplicit formula for the solution but rather an implicit one. Some tricky algebra may be needed to obtain an eplicit solution. Often, an eplicit solution cannot be found. We illustrate with some eamples, beginning with a reprise of Eample.. Eample.5: Use the method of separation of variables to find the general solution of y d =.! Although we will eventually work with the differential notation, to understand the method it is better to write the equation as y = y. Following the instructions in the previous paragraph, we divide both side of the equation by y. (It is worth emphasizing that division and/or multiplication must be used to move factors from one side to the other, never addition or subtraction.) We then obtain y = 1. y 19

4 Differential Equations Now we integrate both sides of the latter equation with respect to, the independent variable. This gives y d = 1 d y. Although we don't know the function y that appears in the integrand on the left side, we can use the general integration formula discussed in Chapter 1 for functions u of, u / ud= ln u + C, to evaluate the left side. The right side can be eplicitly integrated. We get ln y + C = + D. Since C and D are arbitrary constants, we combine them on the right side as D C obtaining the so-called implicit solution of the differential equation, ln y = + D C. (.) The constant D C on the right is again an arbitrary constant. In order to avoid a proliferation of letters, we will simply call this C again, as we have no interest in keeping track of the original value of all the constants. In general, in these types of manipulations, if an arbitrary constant is modified to produce a constant of a slightly different form, we will usually continue labeling the new variant with the same letter. Note that here we could have avoided this notational annoyance had we only used a single constant of integration in deriving (.). In the future we shall include only one constant, on the right side of the integrated equation. We must now solve the implicit equation (.) for y. In order to etract the y term on the left we use the identity e ln w = w, valid for any positive w. This identity is simply a restatement of the inverse function relationship that holds between the eponential and logarithm functions. Thus from (.) (with D C replaced by C ) we get ln y + C C y = e = e = e e. C C Since y =± y, we can write the last equation as y =± e e. The quantity ± e is just a constant, so following the convention mentioned earlier, we again denote its value by C. Thus we obtain the final solution y = Ce.! We can simplify the mechanics of the solution process by using the / d form of the differential equation. In this procedure we not only separate the and y terms, but we also separate the d and differentials, placing each with the corresponding variable. This method of doing separation of variables is similar in spirit to using the differential to do substitutions in integration problems. The manipulations are easier to carry out, though the mathematical reasoning behind them is somewhat obscured.

5 Eample.6: Solve the initial value problem = ( y+ 1), and () 4 d y =. Differential Equations The first step is to produce the general solution of the differential equation. The ODE has separable variables. We separate the variables by dividing both sides by y + 1 and multiplying by d. This leads to = d. y + 1 We now integrate both sides, treating each side as if the variable on that side were an independent variable. = d = + C y + 1. The integral /( y + 1) is evaluated using the substitution u = y+ 1 and yields ln y + 1 the constant of integration. From this we obtain the implicit form of the solution. ln y+ 1 = + C. We solve for y by eponentiation of both sides. This yields, (after writing C for C e ), ignoring / y+ 1 = Ce. The solution y is unwrapped from the absolute value as we did in Eample.5, producing the general solution / y = Ce 1. Having found the general solution, we can solve the initial value problem. Substituting = and y = 4 in the last equation gives 4= Ce 1= C 1, so C = 5 and the solution of the initial value / problem is y = 5e 1.! Eample.7: Find the general solution of y (1) = 4. d y + 1 = and determine the solution for which 1

6 Differential Equations We can separate the variables yielding We now integrate both sides. On the left side of (.3) we have = y + 1 = y + 1 d d. (.3) 1/ = (y+ 1). y + 1 Making the substitution u = y + 1, du = the last integral becomes (ignoring the constant of integration). Therefore (.3) evaluates to 1 = = + 1 1/ 1/ u du u y y+ 1= ln + C, (.4) which is the implicit solution for y. To solve for y we square both sides of (.4). This gives + = + or y 1 (ln C) (ln + C) 1 y =. Note that constants such as 1 and that appear in the final formula are not arbitrary. They are specific pieces of the general solution and must not be omitted or changed. To find the value of C it is more convenient to substitute the initial conditions into (.4) rather than into the final epression for y. When we set = 1 and y = 4 in (.4) we get C = 3 (assuming the square root is the positive one). The solution of the initial value problem is therefore y = ((ln + 3) 1) /.!.3 Money What is the derivative of a function y = f( )? In Chapter 1 we discussed how to compute derivatives and in this chapter we learned some methods for finding a function from information about its derivative. However, to understand how differential equations arise we need to review the fundamental idea of a derivative as an instantaneous rate of change. You may recall the standard definition of the derivative in calculus:

7 Differential Equations f( + h) f( ) f ( ) = lim. (.5) h h This definition is useful for doing algebraic eercises and proving the various differentiation rules, but there is an older, less fashionable notation that captures more of the flavor of the concept. Instead of using h for the increment in the independent variable, we use (read delta ). The symbol represents a single number, not a product. You can think of as an abbreviation for the difference in. The numerator in (.5) can then be written as f( + ) f( ) = y and represents the difference y in the y value when changes from to +. Using the differential notation for the derivative we can rewrite (.5) as y = lim d. (.6) The fraction on the right side of (.6) represents the average rate of change of the function y = f( ) over the interval from to +. The derivative is the limit of this average rate of change as the increment approaches zero. Therefore, it is often referred to as the instantaneous rate of change of y. Differential equations arise when we know something about the rate at which a function changes and want to deduce the behavior of the function itself. In physics, because of Newton's law relating force to acceleration (which is the rate of change of velocity), differential equations are at the core of the subject. We will see in Chapters 5and 6 that many problems concerning biological populations can be given reasonable formulations as differential equations. Here we want to consider a different sort of aggregate, but variable quantity, - money. Unlike populations, for which our mathematical descriptions represent a simplification of reality, an eact mathematical process is usually at the bottom of many financial transactions. We consider the question of continuous compounding of interest and show how equation (.6) leads us to a description of this process as a differential equation. Eample.8: Suppose you have \$1 in a bank account paying 1% annual interest, compounded daily. After 3 days what would be your total accumulation? The daily compounding of interest means that on any day the interest rate would be 1/365 th of the annual rate or.1/365. The amount of interest earned in a day, I, is the current principal P old multiplied by this daily rate. The new principal is then given by Pnew = Pold + I from which we can derive the net day's interest. The table below shows the results obtained at the beginning and end of the 3-day period. The interest is rounded to three decimal places. The change in principal from one day to the net is just the interest earned during the day in question. Notice that the daily interest does change, though it only increases slightly over the entire 3-day period. 3

8 Differential Equations Day Principal (\$) Interest (\$) Day Principal (\$) Interest (\$) 1 1, , , , , , , , , , , , After 3 days the total principal would be \$1, \$1,8.6.! What will happen if we compound the interest even more frequently? We can work out the framework of Eample.8 in abstract terms. If r is the annual interest rate and the time period is represented as a fraction of the year, t (which is 1/ 365 in the eample), then the interest rate during that time period will be r t. If P denotes the principal at time t then the interest earned during the time t from t to t+ t will be P r t. This interest accounts for the change in the principal P, so we have P= P( r t). (.7) We want to let t. Of course, this says that the time period goes to zero. Hence, so does the rate and therefore also the interest earned - not very surprising in view of the interest listed in the table above. In such situations we can learn something by considering the rate at which the interest goes to zero, namely the ratio P/ t. By (.7) this ratio is rp. However according to (.6), as t the ratio P/ t approaches the derivative, the instantaneous rate of change of the function Pt ( ). Thus we arrive at the differential equation dp rp dt =, (.8) which we take as the definition of continuous compounding of interest. Definition.1: Money earns interest at an annual rate r compounded continuously if the principal satisfies equation (.8).! Although we can't physically compound the interest continuously, we can solve the differential equation (.8) and thereby figure out what the principal would be if that idealized process could be achieved. The formula turns out to be quite simple and can be used to directly compute the principal. Eample.9: Find the general formula for the principal Pt () when money is compounded continuously at an annual interest rate r, assuming an initial principal of P. 4

9 Differential Equations We must solve (.8) with initial condition P() = P. The method of separation of variables can be applied. Separating the variables gives Integrating both sides of the latter equation yields dp rdt P =. ln P = rt+ C. Solving for P by eponentiation (see Eample.5) we get P rt = Ce. Substituting P = P() and putting t = we have becomes P Ce C = = so the formula for the principal! rt Pt () = Pe. (.9) There are a number of interesting financial lessons that can be learned from (.9). Eample.1: a) What is the effective annual interest rate if money is compounded continuously at an annual rate r? b) How many years are needed to double any starting principal if money earns interest at an annual rate r compounded continuously? a) By definition, the effective annual interest rate is the relative change in the principal in one year. In other words, it is the quantity r P(1) P() Pe P r = = e 1. P() P When r is small (as it usually is when we are dealing with interest rates) this quantity is just slightly larger than the nominal rate r. The increase is due to the compounding. The table below shows this for some representative interest rates. For eample, at 7% annual interest you would actually earn 7.5% over the course of a year. 5

10 r Differential Equations Effective Annual Rate Doubling Time(years) Table.1 b) We need to find how long it takes for the principal to reach double its initial amount. We must rt find the time t for which P = Pe. Canceling the term P, we are left with the equation rt = e. To solve this equation we take the natural logarithm of both sides obtaining ln = rt ln e = rt, since ln e = 1. Denoting the solution by t, we have t ln =. (.1) r Some representative values of the doubling time are given in Table.1. We can derive a useful rule of thumb to estimate the doubling time. Observe first that ln Therefore, multiplying the numerator and denominator in (.1) by 1 we have t ln 1 7 =. r 1 % interest rate For eample, if the interest rate is r =.7 = 7 %, the estimate gives 7 / 7 = 1 years for the doubling time, compared to the more eact value of 9.9. In finance tets, this rule is often called the Rule of 7.! Money might seem far removed from biology. Yet the same mathematical arguments that allow us to analyze the growth of money in the bank can be used to model the growth of populations. In eercises 18 to 1 we describe how the continuous interest model we have described in this section can be etended to quantify a variety of common financial transactions. In Chapter 5 we will see that the same differential equations are related to problems of harvesting and conservation in population biology..4 Summary A differential equation epresses a relation between the derivative of an unknown function d and values of the independent variable and dependent variable y. The collection of all solutions to the differential equation is called the general solution. This family of solutions will usually contain an arbitrary constant C, whose value may be determined by giving additional information about the unknown function. Quite often this etra information is in the form of an initial condition, y() = y, specifying the value of the unknown function at =. 6

11 Differential Equations Differential equations are solved using integration, but the equation may have to be manipulated algebraically before this can be done. In a separable differential equation, we can separate the dependent and independent variables on either side of the equation and solve the equation by integrating each side. An important eample of this type with many applications is the equation y d = or more generally ry d =, where r is a constant. The solution of the latter is given by r y = y e..5 Eercises 1. By computing d verify that for any constant C the epression y = e + Ce is a solution of the differential equation = e + y. (See Eample..) d. Verify that for any constant C the epression 1 equation =. d y y C = + is a solution of the differential 3. a) Verify that for any constant C the epression y = 1+ Ce is a solution of the differential equation y d =. b) Find the solution of the differential equation in 3a) that satisfies y () =. 4. a) Verify that for any constant C the epression equation 1+ y =. d 1 + Ce 1 y = is a solution of the differential 1+ b) Find the solution of the differential equation in 4a)that satisfies y (1) =. 5. a) Verify that for any constant C the epression differential equation = y. d + y y C = + + is a solution of the b) Find the solution of the differential equation in 5a) that satisfies y (1) = Which, if any, of the differential equations in eercises 1-5 are separable? 7. Which, if any, of the following differential equations are separable? 7

12 Differential Equations a) c) y = d 1 + b) (3y 1) d = + d) y = d y + 1 y d = Use separation of variables to solve each of the differential equations in eercises 8-16 below: 8. y d =, y () =. 9. y d =, y () = 1. dt = t y + 1, y (1) = 3 t 11. =, y () = 1. y dt e 1. 3y 1 dt = +, y (1) =. 13. y = y ( + 1), y () = y =, y () = d y d = ( t + 1) y =, y () =. y 17. After 5 years, which of the following accounts will have a larger principal? After 1 years? Justify your answers. a) An account earning 5% annual interest compounded continuously and starting out with \$1. b) An account earning 4% annual interest compounded continuously and starting out with \$ a) Suppose you want to put away a certain amount of money so that in 1 years the principal will be \$1,. If you can invest at 6% annual interest compounded continuously, what must be your initial principal to meet your 1-year objective? b) Referring to18a), if the best investment available to you will only pay 5% annual interest, show that your initial principal must be increased by more than 1% over the answer to a) in order to reach the \$1, objective in 1 years. 19. a) If you deposit \$5 in an account earning 5% annual interest compounded continuously, how long will it take for the principal to reach \$75? b) If the deposit of \$5 earns 1% interest, how long will it take for the principal to reach \$75? 8

13 9 Differential Equations. A 5-year investment of \$1, begins at 6% annual interest compounded continuously. The investment agreement calls for the interest rate to be evaluated after ½ years, when it can move up or down by at most % for the remaining ½ years. Determine the minimum and maimum principal you can receive at the end of 5 years. 1. For each of the interest rates listed in Table.1, find the number of years for an initial principal to triple.. a) Suppose you deposit an initial principal of \$1 in an account paying 6% annual interest compounded continuously. Every year, including the first, you make additional deposits of \$5 spread out uniformly throughout the year. By repeating the arguments that led to (.8), show that the principal Pt ( ) satisfies the ODE dp.6p 5 dt = +. (.11) b) Find the solution of (.11) satisfying the initial condition P () = 1. c) After 1 years what will be the total principal in the account as described in a)? How much of this total has come from deposits? How much from interest? 3. a) Consider the investment scenario described ina), ecept that your initial principal is zero. Each year you want to make a deposit of K dollars spread out uniformly throughout the year, so that at the end of 5 years the account will have a principal of \$5,. By repeating the arguments that led to equation (.8), show that the principal Pt () satisfies the ODE dp.6p K dt = +. (.1) b) Find the solution of (.1) satisfying P () =. (The as yet unknown constant K will appear in your formula) c) Using the formula in b) find the value of K that will meet your objective as stated in a). How much of the final \$5, consists of deposits and how much consists of interest? 4. a) A woman retires and receives a lump sum of \$, from her company's retirement account. Suppose she deposits this in an account paying 7% continuously compounded annual interest and withdraws \$, a year spread out uniformly throughout the year. By repeating the arguments that led to equation (.8), show that the principal Pt () satisfies the ODE dp.7p dt =, (.13) where we have used units of \$1. b) Find the solution of (.13) satisfying the initial condition P () =.

14 Differential Equations c) For how many years can the woman continue withdrawing the \$, (usually referred to as an annuity)? 5. a) A man wants to retire at age 65 and be able to draw \$1, a year from retirement savings to supplement his Social Security income and employee retirement benefits. At retirement he anticipates investing his savings in government securities that should return 5% a year compounded continuously. By repeating the arguments that led to equation (.8), show that after retirement the principal Pt ( ) in his account satisfies the ODE dp.5p 1 dt =, (.14) where we have used units of \$1. b) Determine the general solution of (.14) and find a formula for the solution with, as yet undetermined, initial value P. c) How large must the man's initial retirement savings be so that he can continue drawing his \$1, income (annuity) for years? 6. Eercises - 5 dealt with ODEs of the form dp = rp + b. Find a formula for the solution of dt this equation with initial condition P() = P. Check that when b = your answer reduces to (.9). 3

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