## Techniques of Indefinite Integration

Integration by substitution. This section opens with integration by substitution, the most widely used integration technique, illustrated by several examples. The idea is simple: Simplify an integral by letting a single symbol (say the letter u) stand for some complicated expression in the integrand. If the differential of u is left over in the integrand, the process will be a success.

Example 1: Determine Let u = x 2 + 1 (this is the substitution); then du = 2 x dx, and the given integral is transformed into which transforms back to ⅓( x 2 + 1) 3/2; + c.

Example 2: Integrate Let u = sin x; then du = cos x dx, and the given integral becomes Example 3: Evalute First, rewrite tan x as sin x/cos x; then let u = cos x, du = − sin x dx: Example 4: Evaluate Let u = x 2; then du = 2 x dx, and the integral is transformed into Example 5: Determine Let u = sec x; then du = sec x dx, and the integral is transformed into Integration by parts. The product rule for differentiation says d( uv) = u dv + v du. Integrating both sides of this equation gives uv = ∫ u dv + ∫ v du, or equivalently This is the formula for integration by parts. It is used to evaluate integrals whose integrand is the product of one function ( u) and the differential of another ( dv). Several examples follow.

Example 6: Integrate Compare this problem with Example 4. A simple substitution made that integral trivial; unfortunately, such a simple substitution would be useless here. This is a prime candidate for integration by parts, since the integrand is the product of a function ( x) and the differential ( e x dx) of another, and when the formula for integration by parts is used, the integral that is left is easier to evaluate (or, in general, at least not more difficult to integrate) than the original.

Let u = x and dv = e x dx; then and the formula for integration by parts yields Example 7: Integrate Let u = x and dv = cos x dx; then The formula for integration by parts gives Example 8: Evaluate Let u = In x and dv = dx; then and the formula for integration by parts yields 