Worked examples · Sheet 1
Basic integrals and integrals in composite form
Theory used: Indefinite integralBasic integralsBasic integrals in composite formAntiderivatives of the same function
Go to: Exercise 1Exercise 2Exercise 3Exercise 4
Exercise 1
Compute
By the linearity of the indefinite integral, each term is integrated separately, bringing the multiplicative constants outside. The powers and are integrated with the formula , the constant has antiderivative , and the term , which is the only power excluded from that formula, has antiderivative . The constants of the individual integrals are combined into a single constant . As a check, the derivative of the result is , that is, the integrand.
Exercise 2
Compute, for ,
The quotient does not have a basic antiderivative, so it is first transformed into a sum of powers. We expand the square of the binomial and divide each term by , subtracting from the exponents. Each power has exponent different from , therefore it is integrated with the power formula, and dividing by , , is equivalent to multiplying by , , . The last term is rewritten as .
Exercise 3
Compute
In the first integral the numerator is exactly the derivative of the denominator, so the integral has the composite form with . The discriminant of is and the coefficient of is positive, therefore for every and the absolute value can be omitted.
In the second integral the power appears with , whose derivative is . The factor present in the integrand is the derivative up to the factor , so we multiply and divide by and apply the composite form with . Differentiating the result gives , as it must be.
Exercise 4
Find the antiderivative of
such that .
The derivative of is , so the first term has the composite form and has antiderivative , without absolute value because . The second term has the form with up to the factor , therefore its antiderivative is . By the theorem on antiderivatives of the same function, all the antiderivatives of are obtained by adding a constant , and the condition singles out only one of them. Since and , the condition becomes , so .