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multivariable_17_Differential_Equations_4up

multivariable_17_Differential_Equations_4up - 426 Chapter...

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17 Differential Equations Many physical phenomena can be modeled using the language of calculus. For example, observational evidence suggests that the temperature of a cup of tea (or some other liquid) in a room of constant temperature will cool over time at a rate proportional to the difference between the room temperature and the temperature of the tea. In symbols, if t is the time, M is the room temperature, and f ( t ) is the temperature of the tea at time t then f ( t ) = k ( M f ( t )) where k > 0 is a constant which will depend on the kind of tea (or more generally the kind of liquid) but not on the room temperature or the temperature of the tea. This is Newton’s law of cooling and the equation that we just wrote down is an example of a differential equation . Ideally we would like to solve this equation, namely, find the function f ( t ) that describes the temperature over time, though this often turns out to be impossible, in which case various approximation techniques must be used. The use and solution of differential equations is an important field of mathematics; here we see how to solve some simple but useful types of differential equation. Informally, a differential equation is an equation in which one or more of the derivatives of some function appear. Typically, a scientific theory will produce a differential equation (or a system of differential equations) that describes or governs some physical process, but the theory will not produce the desired function or functions directly. Recall from section 6.2 that when the variable is time the derivative of a function y ( t ) is sometimes written as ˙ y instead of y ; this is quite common in the study of differential equations. 425 426 Chapter 17 Differential Equations We start by considering equations in which only the first derivative of the function appears. DEFINITION 17.1 A first order differential equation is an equation of the form F ( t, y, ˙ y ) = 0. A solution of a first order differential equation is a function f ( t ) that makes F ( t, f ( t ) , f ( t )) = 0 for every value of t . Here, F is a function of three variables which we label t , y , and ˙ y . It is understood that ˙ y will explicitly appear in the equation although t and y need not. The term “first order” means that the first derivative of y appears, but no higher order derivatives do. EXAMPLE 17.2 The equation from Newton’s law of cooling, ˙ y = k ( M y ) is a first order differential equation; F ( t, y, ˙ y ) = k ( M y ) ˙ y . EXAMPLE 17.3 ˙ y = t 2 +1 is a first order differential equation; F ( t, y, ˙ y ) = ˙ y t 2 1. All solutions to this equation are of the form t 3 / 3 + t + C . DEFINITION 17.4 A first order initial value problem is a system of equations of the form F ( t, y, ˙ y ) = 0, y ( t 0 ) = y 0 . Here t 0 is a fixed time and y 0 is a number. A solution of an initial value problem is a solution f ( t ) of the differential equation that also satisfies the initial condition f ( t 0 ) = y 0 .

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