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Integration rules

Properties of Definite Integrals: Rules, Symmetry and Examples

The properties of definite integrals: reversing limits, zero width, additivity over intervals, odd and even symmetry and comparison bounds, with examples.

Integration rules Updated 3 min read

At a glance

\int_a^b f(x)\,dx + \int_b^c f(x)\,dx = \int_a^c f(x)\,dx
Zero width
\int_a^a f(x)\,dx = 0
Reversed limits
\int_b^a f(x)\,dx = -\int_a^b f(x)\,dx
Constant
\int_a^b k\,dx = k(b - a)
Odd function
\int_{-a}^{a} f(x)\,dx = 0
Even function
\int_{-a}^{a} f(x)\,dx = 2\int_0^a f(x)\,dx
Comparison
If f(x) \le g(x) on [a, b], then \int_a^b f\,dx \le \int_a^b g\,dx
On this page
  1. The properties
  2. Why they hold
  3. Symmetry: odd and even functions
  4. Worked examples
  5. Common mistakes

The properties of definite integrals are the rules for manipulating \int_a^b f(x)\,dx without computing it from scratch: flipping limits, splitting intervals, using symmetry and estimating size. They all follow from viewing the integral as signed area, or from the Fundamental Theorem of Calculus.

The properties

Assume f and g are integrable on the intervals involved.

Property Statement
Zero width \int_a^a f(x)\,dx = 0
Reversed limits \int_b^a f(x)\,dx = -\int_a^b f(x)\,dx
Constant \int_a^b k\,dx = k(b-a)
Linearity \int_a^b [\alpha f + \beta g]\,dx = \alpha\int_a^b f\,dx + \beta\int_a^b g\,dx
Additivity \int_a^b f\,dx + \int_b^c f\,dx = \int_a^c f\,dx
Comparison f \le g on [a,b] \Rightarrow \int_a^b f\,dx \le \int_a^b g\,dx
Bounds m \le f \le M on [a,b] \Rightarrow m(b-a) \le \int_a^b f\,dx \le M(b-a)
Odd symmetry f(-x) = -f(x) \Rightarrow \int_{-a}^{a} f\,dx = 0
Even symmetry f(-x) = f(x) \Rightarrow \int_{-a}^{a} f\,dx = 2\int_0^a f\,dx

The comparison and bounds properties assume a < b. Additivity holds for any order of a, b and c, as long as f is integrable on the intervals, thanks to the reversed-limits rule.

Why they hold

If F is an antiderivative of f, then \int_a^b f\,dx = F(b) - F(a). Each property is a line of algebra from there:

  • zero width: F(a) - F(a) = 0;
  • reversed limits: F(a) - F(b) = -\left(F(b) - F(a)\right);
  • additivity: \left(F(b) - F(a)\right) + \left(F(c) - F(b)\right) = F(c) - F(a).

Linearity is covered on its own page: integral linearity rules.

Symmetry: odd and even functions

Signed area of the odd function y = x³ − 2x on [−1.5, 1.5]
The area on the left is the mirror image of the area on the right with the opposite sign, so \int_{-1.5}^{1.5} (x^3 - 2x)\,dx = 0.

An odd function is symmetric about the origin, so every bit of positive area has a matching bit of negative area. An even function is symmetric about the y-axis, so the two halves are equal and you can double one of them. Checking symmetry first can turn a long calculation into one line.

Worked examples

Example 1: odd symmetry. x^5 - 4x^3 + \sin x is odd, so

\int_{-3}^{3} \left(x^5 - 4x^3 + \sin x\right)dx = 0

Example 2: even symmetry. x^2 is even, so

\int_{-1}^{1} x^2\,dx = 2\int_0^1 x^2\,dx = 2\cdot\frac{1}{3} = \frac{2}{3}

Example 3: additivity and reversed limits. Given \int_0^5 f(x)\,dx = 10 and \int_0^2 f(x)\,dx = 3:

\int_2^5 f(x)\,dx = 10 - 3 = 7, \qquad \int_5^2 f(x)\,dx = -7

Example 4: an absolute value. Split where the inside changes sign. On [-1, 0], \lvert x\rvert = -x; on [0, 2], \lvert x\rvert = x:

\int_{-1}^{2} \lvert x\rvert\,dx = \int_{-1}^{0} (-x)\,dx + \int_0^2 x\,dx = \frac{1}{2} + 2 = \frac{5}{2}

Example 5: estimating with bounds. On [0, 1], e^{-1} \le e^{-x^2} \le 1, so

0.37 \approx e^{-1} \le \int_0^1 e^{-x^2}\,dx \le 1

This integral has no elementary antiderivative, yet the bounds pin it down. Its actual value is about 0.747.

Common mistakes

  1. Using symmetry on a non-symmetric interval. \int_{-1}^{2} x^3\,dx is not 0. The interval must be [-a, a].
  2. Calling a function odd without checking. x^3 + 1 is neither odd nor even, so \int_{-1}^{1} (x^3 + 1)\,dx = 2, not 0.
  3. Forgetting the sign flip when reversing limits.
  4. Confusing signed area with total area. \int_{-1}^{1} x\,dx = 0, but the total shaded area is 1. For area, integrate \lvert f(x)\rvert, as in area between curves.

For how these properties connect to Riemann sums and evaluating integrals, see the guides to Riemann sums and the Fundamental Theorem of Calculus.

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The definite integral as area

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Frequently asked questions

What happens when you switch the limits of a definite integral?

The integral changes sign: \int_b^a f(x)\,dx = -\int_a^b f(x)\,dx. This follows directly from evaluating F(a) - F(b) instead of F(b) - F(a).

What is the integral of an odd function from -a to a?

It is 0, because the signed area on the left exactly cancels the signed area on the right. For example \int_{-2}^{2} x^3\,dx = 0.

Can you split a definite integral into two?

Yes. For any b, \int_a^c f\,dx = \int_a^b f\,dx + \int_b^c f\,dx. This is how you integrate piecewise functions and absolute values.

Is the integral from a to a always zero?

Yes. An interval of width zero has no area, so \int_a^a f(x)\,dx = 0 for any function f defined at a.

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