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Calculus I Supplements · Foundational

Supplement: Common Antiderivatives

Build a reliable antiderivative reference from derivative checks, including powers, exponentials, logarithms, trigonometric functions, and constants of integration.

Formula reference. Differentiate any proposed antiderivative to check it. Each formula holds on an interval where its integrand is defined.

Common antiderivatives

∫xn dx=xn+1n+1+C (n≠−1),∫1x dx=ln⁡∣x∣+C,∫ex dx=ex+C.\int x^n\,dx=\frac{x^{n+1}}{n+1}+C\ (n\ne-1),\qquad \int\frac1x\,dx=\ln|x|+C,\qquad \int e^x\,dx=e^x+C.

∫ax dx=axln⁡a+C (a>0, a≠1),∫cos⁡x dx=sin⁡x+C,∫sin⁡x dx=−cos⁡x+C.\int a^x\,dx=\frac{a^x}{\ln a}+C\ (a>0,\ a\ne1),\qquad \int\cos x\,dx=\sin x+C,\qquad \int\sin x\,dx=-\cos x+C.

∫sec⁡2x dx=tan⁡x+C,∫csc⁡2x dx=−cot⁡x+C,∫sec⁡xtan⁡x dx=sec⁡x+C.\int\sec^2x\,dx=\tan x+C,\qquad \int\csc^2x\,dx=-\cot x+C,\qquad \int\sec x\tan x\,dx=\sec x+C.

∫csc⁡xcot⁡x dx=−csc⁡x+C,∫11+x2 dx=arctan⁡x+C,∫11−x2 dx=arcsin⁡x+C.\int\csc x\cot x\,dx=-\csc x+C,\qquad \int\frac1{1+x^2}\,dx=\arctan x+C,\qquad \int\frac1{\sqrt{1-x^2}}\,dx=\arcsin x+C.

An antiderivative is best remembered as a function whose derivative returns the integrand. That definition turns every reference entry into something you can check. If you claim that an expression is an antiderivative of f(x)f(x), differentiate your claim. The check is quick, local, and more reliable than recall alone.

Imagine reconstructing a train’s position from a recorded velocity. Many position functions can have the same velocity because adding a constant vertical shift does not change a derivative. The initial position selects one member of that family. This story explains why indefinite integrals require +C+C and why a definite integral does not.

Recover powers, exponentials, and logarithms

For n≠−1n\ne-1, ∫xn dx=xn+1n+1+C\int x^n\,dx=\frac{x^{n+1}}{n+1}+C. Differentiate xn+1n+1\frac{x^{n+1}}{n+1} to see the coefficient and exponent cancel correctly. The exception is ∫1x dx=ln⁡∣x∣+C\int\frac1x\,dx=\ln|x|+C on intervals that avoid zero. The absolute value is needed because both positive and negative nonzero inputs have derivative 1x\frac1x after the logarithmic form is interpreted on its interval.

Exponential families reverse cleanly: ∫ex dx=ex+C\int e^x\,dx=e^x+C, while ∫ax dx=axln⁡a+C\int a^x\,dx=\frac{a^x}{\ln a}+C for a>0a>0 and a≠1a\ne1. The denominator appears because (ax)′=(ln⁡a)ax(a^x)'=(\ln a)a^x. A missing ln⁡a\ln a is a derivative-check failure, not a minor formatting error.

An antiderivative family diagram distinguishes a whole family of functions from one initial-condition-selected member.

Recover trigonometric functions with signs

Because (sin⁡x)′=cos⁡x(\sin x)'=\cos x, ∫cos⁡x dx=sin⁡x+C\int\cos x\,dx=\sin x+C. Because (cos⁡x)′=−sin⁡x(\cos x)'=-\sin x, ∫sin⁡x dx=−cos⁡x+C\int\sin x\,dx=-\cos x+C. The minus sign is a consequence of differentiation, and it is worth checking rather than memorizing as an exception.

For secant-squared and cosecant-squared, ∫sec⁡2x dx=tan⁡x+C\int\sec^2x\,dx=\tan x+C and ∫csc⁡2x dx=−cot⁡x+C\int\csc^2x\,dx=-\cot x+C on intervals where the expressions are defined. These statements inherit the trig functions’ discontinuities. Choose an interval before treating one antiderivative family as a global formula.

A unit-circle-to-sine graph provides the geometric context for sine and cosine derivative and antiderivative pairs.

Connect the reference to a model

If a train has velocity v(t)=3t2−4 msv(t)=3t^2-4\,\frac{\mathrm{m}}{\mathrm{s}}, then an antiderivative is s(t)=t3−4t+Cs(t)=t^3-4t+C meters. The units are consistent because integrating velocity with respect to seconds yields meters. Given s(0)=12 ms(0)=12\,\mathrm{m}, the constant is 1212, producing a particular position model.

Do not confuse that antiderivative with distance traveled. The difference s(b)−s(a)s(b)-s(a) gives displacement, which may cancel when velocity changes sign. Total distance requires integrating ∣v(t)∣|v(t)| or splitting at sign changes. A reference table provides forms; the model determines what the form means.

A motion antiderivative ladder connects position, velocity, acceleration, and the direction of differentiation or accumulation.

Narrative challenge: reconstruct the train position

A train has velocity v(t)=6t−8 msv(t)=6t-8\,\frac{\mathrm{m}}{\mathrm{s}} and position s(0)=15 ms(0)=15\,\mathrm{m}. Before opening the solution, find a position function and explain why the constant cannot be omitted. Then identify the time at which velocity is zero and state why that time may matter for distance.

Show a solution path

An antiderivative is s(t)=3t2−8t+Cs(t)=3t^2-8t+C. The initial condition gives C=15C=15, so s(t)=3t2−8t+15s(t)=3t^2-8t+15 meters. Velocity is zero when 6t−8=06t-8=0, or t=43 st=\frac43\,\mathrm{s}. A sign change there would make it a necessary split point when computing total distance.

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Prerequisites

Calculus I SupplementsRules of Integration and Method Choice

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Connections

Related lessons

Unit 5 - Accumulation, Integrals, and the Fundamental TheoremAntiderivatives and Simple Differential EquationsCalculus I SupplementsSupplement: Rules of Integration and Method Choice

Applications

  • reconstructing quantities
  • motion
  • differential equations