Antiderivatives and Indefinite Integration

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4.1 Antiderivatives and Indefinite Integration
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Presentation transcript:

Antiderivatives and Indefinite Integration MATH 1910 Chapter 4 Section 1 Antiderivatives and Indefinite Integration

Objectives Write the general solution of a differential equation and use indefinite integral notation for antiderivatives. Use basic integration rules to find antiderivatives. Find a particular solution of a differential equation.

Antiderivatives To find a function F whose derivative is f(x) = 3x2, you might use your knowledge of derivatives to conclude that The function F is an antiderivative of f .

Antiderivatives Note that F is called an antiderivative of f, rather than the antiderivative of f. To see why, observe that are all derivatives of f (x) = 3x2. In fact, for any constant C, the function F(x)= x3 + C is an antiderivative of f.

Antiderivatives Using Theorem 4.1, you can represent the entire family of antiderivatives of a function by adding a constant to a known antiderivative. For example, knowing that Dx [x2] = 2x, you can represent the family of all antiderivatives of f(x) = 2x by G(x) = x2 + C Family of all antiderivatives of f(x) = 2x where C is a constant. The constant C is called the constant of integration.

Antiderivatives The family of functions represented by G is the general antiderivative of f, and G(x) = x2 + C is the general solution of the differential equation G'(x) = 2x. Differential equation A differential equation in x and y is an equation that involves x, y, and derivatives of y. For instance, y' = 3x and y' = x2 + 1 are examples of differential equations.

Example 1 – Solving a Differential Equation Find the general solution of the differential equation y' = 2. Solution: To begin, you need to find a function whose derivative is 2. One such function is y = 2x. 2x is an antiderivative of 2. Now, you can use Theorem 4.1 to conclude that the general solution of the differential equation is y = 2x + C. General solution

Example 1 – Solution cont’d The graphs of several functions of the form y = 2x + C are shown in Figure 4.1. Figure 4.1

Notation for Antiderivatives When solving a differential equation of the form it is convenient to write it in the equivalent differential form The operation of finding all solutions of this equation is called antidifferentiation (or indefinite integration) and is denoted by an integral sign ∫.

Notation for Antiderivatives The general solution is denoted by The expression ∫f(x)dx is read as the antiderivative of f with respect to x. So, the differential dx serves to identify x as the variable of integration. The term indefinite integral is a synonym for antiderivative.

Basic Integration Rules The inverse nature of integration and differentiation can be verified by substituting F'(x) for f(x) in the indefinite integration definition to obtain Moreover, if ∫f(x)dx = F(x) + C, then

Basic Integration Rules These two equations allow you to obtain integration formulas directly from differentiation formulas, as shown in the following summary.

Basic Integration Rules cont’d

Example 2 – Applying the Basic Integration Rules Describe the antiderivatives of 3x. Solution: So, the antiderivatives of 3x are of the form where C is any constant.

Basic Integration Rules In Example 2, note that the general pattern of integration is similar to that of differentiation.

Initial Conditions and Particular Solutions You have already seen that the equation y = ∫f(x)dx has many solutions (each differing from the others by a constant). This means that the graphs of any two antiderivatives of f are vertical translations of each other.

Initial Conditions and Particular Solutions For example, Figure 4.2 shows the graphs of several antiderivatives of the form for various integer values of C. Each of these antiderivatives is a solution of the differential equation Figure 4.2

Initial Conditions and Particular Solutions In many applications of integration, you are given enough information to determine a particular solution. To do this, you need only know the value of y = F(x) for one value of x. This information is called an initial condition. For example, in Figure 4.2, only one curve passes through the point (2, 4). To find this curve, you can use the general solution F(x) = x3 – x + C General solution and the initial condition F(2) = 4 Initial condition

Initial Conditions and Particular Solutions By using the initial condition in the general solution, you can determine that F(2) = 8 – 2 + C = 4 which implies that C = –2. So, you obtain F(x) = x3 – x – 2. Particular solution

Example 8 – Finding a Particular Solution Find the general solution of and find the particular solution that satisfies the initial condition F(1) = 0. Solution: To find the general solution, integrate to obtain

Example 8 – Solution Using the initial condition F(1) = 0, you cont’d Using the initial condition F(1) = 0, you can solve for C as follows. So, the particular solution, as shown in Figure 4.3, is Figure 4.3