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The power rule of integration yields antiderivatives: raise the exponent by 1 and divide by the new exponent.
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Formula
Dimensionless (calculus)
| Symbol | Meaning | Unit |
|---|---|---|
| Variable of integration | dimensionless | |
| Exponent | dimensionless | |
| Constant of integration (any real number) | dimensionless |
\int x^{n} \, dx = \frac{x^{n+1}}{n+1} + C \quad (n \neq -1)Original schematic by Quanta
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Integration reverses differentiation: F is called an antiderivative of f if . The power rule of integration mirrors the power rule of differentiation. Important basic integrals: , (the special case n = −1), , . Since constants vanish when differentiating, every antiderivative is determined only up to +C.
The power rule of integration holds for all real ; for the antiderivative is ln|x| + C. Antiderivatives are unique only up to a constant C.
Integration reverses differentiation: differentiate the candidate and compare.
Special case \(n = -1\)
The power rule would divide by 0; the logarithm steps in.
Exponential and trigonometry
The basic exam integrals; watch the sign for sin.
Linear substitution
Inner linear function: divide by a instead of multiplying.
Find all antiderivatives of .
Term by term: .
Check: F′ ✓.
Find the antiderivative of through the point (0|1).
.
, so .
Result: .
Lowering the exponent when integrating, as in differentiating.
Integration raises: .
Dropping the +C.
Without C infinitely many antiderivatives are missing; initial conditions fix C.
Integrating with the power rule.
is the special case: ln|x| + C.
Writing .
Correct: −cos x + C; differentiate to check.
Formula cluster
Basic integrals, fundamental theorem and area calculation build on each other.
. Check by differentiating: ✓. Likewise: , since .
Area and volume calculation, reconstructing totals from rates of change, physics (distance from velocity), probability densities
Here is how to work through a typical Antiderivatives and Basic Integrals (∫xⁿ dx = xⁿ⁺¹/(n+1) + C) task step by step:
Task
Find all antiderivatives of .
Solution path
Term by term: .
Check: F′ ✓.
Task
Find the antiderivative of through the point (0|1).
Solution path
.
, so .
Result: .
Reverse the power rule of differentiation: raise the exponent by 1, then divide by the new exponent. becomes , valid for all . Constant factors stay, sums are handled term by term. Example: has antiderivatives . The rule also works for negative and fractional exponents: and . Safest check: differentiate the result, it must give exactly the integrand. Only the case drops out; there the antiderivative is ln|x| + C.
Because the derivative of every constant is zero. If F is an antiderivative of f, then so are F + 7 or F − 123, since the constant vanishes without trace when differentiating. The set of all antiderivatives is therefore a whole family of vertically shifted graphs, and the +C stands for these infinitely many possibilities. C is pinned down only by an extra condition, such as "the graph passes through (0|1)": for , , and forces . In a definite integral, however, C cancels in F(b) − F(a), so there you may drop it.
The core set is short: the power rule for , the special case , the exponential ∫eˣ dx = eˣ + C with the variant , and the trigonometric pair and . Add the structural rules: integrate term by term, pull constant factors out front, and for an inner linear function f(ax + b) divide by a. With this toolbox you cover almost all mandatory-part integrals; more complicated products are handled by integration by parts. Regular self-check: differentiate backwards.
In German classrooms "aufleiten" is student slang for finding an antiderivative, i.e. reversing differentiation; the proper term is indefinite integration. Mathematics distinguishes two things precisely: the indefinite integral ∫f(x) dx denotes the set of all antiderivatives F + C. The definite integral ∫aᵇ f(x) dx, by contrast, is a number, defined as a limit of rectangle sums, measuring signed areas. The fundamental theorem connects both worlds: you obtain the number by evaluating any antiderivative at the limits, F(b) − F(a). In exams use the term antiderivative; "aufleiten" is understood by everyone but counts as colloquial.
Use the linear substitution rule: if F is an antiderivative of f, then . The inner linear function stays, and you divide by its slope a instead of multiplying by it as in differentiation. Examples: , , . Checking by differentiating shows why: the chain rule produces the factor a, which the cancels again. Caution: this convenient rule holds ONLY for linear inner functions; for it fails, such an integral has no elementary antiderivative.
Quanta exam set
Curated exam set for "Antiderivatives and Basic Integrals":
Question (front)
Which formula describes Antiderivatives and Basic Integrals?
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Question (front)
How do you rearrange Antiderivatives and Basic Integrals for Special case \(n = -1\)?
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Question (front)
Which common mistake happens with Antiderivatives and Basic Integrals?
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