Integration by Substitution Type 1¶
Proposition¶
Let be continuously differentiable, and let be continuous on an interval containing the range of Then
Interpretation¶
Substitution of type 1 is the chain rule read backwards. When the integrand has the form , the inner function is renamed , and the integral becomes in the new variable. It works best when the derivative factor already appears in the integrand.
The colours in the formula show the matching. The red part becomes , and the blue part becomes . As runs from to , runs from to , so the limits change too and there is no need to return to at the end.
The equality concerns Riemann integrals under the stated continuity assumptions. The differential relation records the derivative factor, and gives the transformed endpoints. The hypotheses make both sides ordinary integrals of continuous functions, and has an antiderivative with . The function may go back and forth: for on , , so for every continuous .
A common slip is to substitute when the factor is missing. The substitution turns into , but it does not help with . Another is to change the integrand but keep the old limits .
Key Results¶
- The function need not be invertible; the formula follows from the chain rule and the fundamental theorem of calculus.
- The limits of integration must be transformed together with the integrand, from to
- If then the corresponding indefinite identity is
Examples¶
- can be simplified by proposing
- can be evaluated using
Prerequisites¶
Related Concepts¶
Sources¶
- Math I: Calculus · Lecture 12
Aliases: u-substitution Keywords: change of variables, substitution rule Symbols: alpha, beta, element of, integral, pi, real numbers
Last updated: 27 October 2026 11:52
Integration by Substitution Type 1Transformation of a Continuous Random VariableRiemann IntegralDifferentiability ClassContinuityChain RuleDifferentialIntegration by Substitution Type 2Indefinite IntegralIntegration by Parts