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Integral Properties and Estimates · Tutorial 993 of 1495

Odd Functions On Symmetric Intervals

Use the defining symmetry of an odd function to prove and apply the zero-integral rule on intervals symmetric about zero.

Intermediate 9 min read

What You'll Learn

  • Define an odd function on a domain symmetric about zero.
  • State the conditions for the zero-integral rule.
  • Prove the rule by pairing terms in symmetric Riemann sums.
  • Check oddness for polynomial and trigonometric functions.
  • Apply cancellation and verify results by evaluating antiderivatives.
  • Recognize why symmetry of the interval alone is not enough.

Why Oddness Produces Cancellation

A definite integral records signed accumulation. Contributions above the horizontal axis count positively, and contributions below it count negatively. When a function is odd, values at points equally far to the left and right of zero have equal magnitudes and opposite signs. On a symmetric interval, these paired contributions cancel.

The symmetry of the interval matters, but it is not enough by itself. The function must have the matching sign symmetry. This tutorial defines that condition, proves the resulting zero-integral rule, and applies it to polynomial and trigonometric functions.

Odd Functions and Symmetric Intervals

Definition: A function \(f\) is odd on a domain symmetric about zero if, for every \(x\) in that domain, \(f(-x)=-f(x)\). An interval is symmetric about zero if it has the form \([-a,a]\) for some \(a\geq 0\).

The equation \(f(-x)=-f(x)\) says that reflecting the input across zero reverses the output's sign. In particular, if zero is in the domain, then setting \(x=0\) gives \(f(0)=-f(0)\), so \(f(0)=0\).

For the integral rule, we also need integrability. Throughout, integrability means Riemann integrability on the stated closed interval. The theorem does not require \(f\) to be continuous, but it does require the integral to exist and the oddness condition to hold throughout the interval.

Theorem: If \(f\) is Riemann integrable on \([-a,a]\) and is odd there, then $$ \int_{-a}^{a} f(x)\,dx=0. $$ This includes \(a=0\), for which the interval has length zero.

Proof by Pairing Riemann-Sum Terms

The cancellation can be seen directly in Riemann sums, without assuming a general formula for reflecting integrals. Assume first that \(a>0\). Divide \([0,a]\) into \(n\) equal subintervals, each of width \(h=a/n\). For each subinterval choose a tag \(\xi_k\), where \(k=1,\ldots,n\). Pair that subinterval with its reflection on the negative side, and choose the reflected tag \(-\xi_k\).

Each positive-side term and its paired negative-side term add to zero:

$$ h f(\xi_k)+h f(-\xi_k) = h\bigl(f(\xi_k)+f(-\xi_k)\bigr) = h\bigl(f(\xi_k)-f(\xi_k)\bigr) = 0. $$

The paired subintervals cover \([-a,a]\). Therefore, the entire tagged Riemann sum is

$$ \sum_{k=1}^{n} h f(\xi_k) + \sum_{k=1}^{n} h f(-\xi_k) = 0. $$

The width of every subinterval is \(h=a/n\), which tends to zero as \(n\) increases. Because \(f\) is Riemann integrable, these tagged sums converge to its integral on \([-a,a]\). Every sum in this sequence is zero, so its limit is zero. This proves the theorem for \(a>0\). When \(a=0\), the integral over the interval of length zero is zero by the definition of the definite integral. Thus the result holds for every \(a\geq 0\).

The proof relies on two distinct facts: oddness makes each reflected pair cancel, and integrability ensures the Riemann sums converge to the integral. If either condition is missing, this argument does not establish the conclusion.

Worked Example: An Odd Polynomial

Worked Example: An Odd Polynomial

Evaluate \(\int_{-1}^{1}(x^5-2x^3+4x)\,dx\) using symmetry, and verify the result directly.

Let \(f(x)=x^5-2x^3+4x\). Replacing \(x\) by \(-x\) gives

$$ f(-x)=(-x)^5-2(-x)^3+4(-x) =-x^5+2x^3-4x =-(x^5-2x^3+4x) =-f(x). $$

Thus \(f\) is odd. It is a polynomial, so it is Riemann integrable on \([-1,1]\). The interval is symmetric about zero, and the theorem gives

$$ \int_{-1}^{1}(x^5-2x^3+4x)\,dx=0. $$

To check by direct evaluation, an antiderivative is

$$ F(x)=\frac{x^6}{6}-\frac{x^4}{2}+2x^2. $$

Differentiating verifies the antiderivative:

$$ F'(x)=x^5-2x^3+4x. $$

At both endpoints,

$$ F(1)=\frac{1}{6}-\frac{1}{2}+2 =\frac{1-3+12}{6} =\frac{10}{6} =\frac{5}{3}, $$
$$ F(-1)=\frac{(-1)^6}{6}-\frac{(-1)^4}{2}+2(-1)^2 =\frac{1}{6}-\frac{1}{2}+2 =\frac{5}{3}. $$

Therefore the definite integral is \(F(1)-F(-1)=\frac{5}{3}-\frac{5}{3}=0\), agreeing with the symmetry argument.

Worked Example: A Trigonometric Function

Worked Example: A Trigonometric Function

Evaluate \(\int_{-\pi/2}^{\pi/2}\sin(2x)\,dx\) by checking its symmetry, then verify by antiderivative.

Since sine is odd, \(\sin(-u)=-\sin(u)\). Taking \(u=2x\) gives

$$ \sin(2(-x))=\sin(-2x)=-\sin(2x). $$

Thus \(f(x)=\sin(2x)\) is odd. It is continuous, hence integrable, on the symmetric interval \([-\pi/2,\pi/2]\). The theorem therefore gives an integral of zero.

For a direct check, an antiderivative is \(F(x)=-\frac{1}{2}\cos(2x)\), since

$$ F'(x)=-\frac{1}{2}\bigl(-2\sin(2x)\bigr)=\sin(2x). $$

The endpoint values are

$$ F\left(\frac{\pi}{2}\right) =-\frac{1}{2}\cos(\pi) =\frac{1}{2}, \qquad F\left(-\frac{\pi}{2}\right) =-\frac{1}{2}\cos(-\pi) =\frac{1}{2}, $$

because \(\cos(\pi)=\cos(-\pi)=-1\). Hence

$$ \int_{-\pi/2}^{\pi/2}\sin(2x)\,dx = F\left(\frac{\pi}{2}\right)-F\left(-\frac{\pi}{2}\right) = \frac{1}{2}-\frac{1}{2} = 0. $$

Worked Example: A Sum of Odd Terms

Worked Example: A Sum of Odd Terms

Evaluate \(\int_{-\pi}^{\pi}(x\cos x+\sin x)\,dx\) by identifying the symmetry, and check it directly.

Cosine is even, so \(\cos(-x)=\cos x\). Therefore

$$ (-x)\cos(-x)=-x\cos x=-(x\cos x). $$

Thus \(x\cos x\) is odd. Sine is odd as well, so

$$ \sin(-x)=-\sin x. $$

Adding these equalities shows that \(f(x)=x\cos x+\sin x\) is odd. The function is continuous on \([-\pi,\pi]\), so the theorem gives an integral of zero.

For a direct check, \(F(x)=x\sin x\) is an antiderivative:

$$ F'(x)=\sin x+x\cos x. $$

Using \(\sin(\pi)=\sin(-\pi)=0\), the endpoint values are

$$ F(\pi)=\pi\sin(\pi)=0, \qquad F(-\pi)=(-\pi)\sin(-\pi)=0. $$

Consequently,

$$ \int_{-\pi}^{\pi}(x\cos x+\sin x)\,dx =F(\pi)-F(-\pi)=0-0=0, $$

which confirms the result.

Common Mistake: Confusing an Even Function with an Odd One

A symmetric interval does not make every integral zero. For example, \(x^2\) is not odd:

$$ (-x)^2=x^2, $$

so it is even. A mistaken argument might call \(x^2\) odd because its interval \([-1,1]\) is symmetric, then conclude that its integral vanishes. The function's symmetry must be checked separately. In fact,

$$ \int_{-1}^{1}x^2\,dx = \left[\frac{x^3}{3}\right]_{-1}^{1} = \frac{1}{3}-\left(-\frac{1}{3}\right) = \frac{2}{3}, $$

not zero. The correction is to verify \(f(-x)=-f(x)\) before applying the odd-function theorem. Here \(f(-x)=f(x)\), so the zero-integral result does not apply.

Another useful check is the interval: oddness alone does not force an integral over a nonsymmetric interval to vanish. For instance, \(f(x)=x\) is odd, but

$$ \int_{0}^{1}x\,dx = \left[\frac{x^2}{2}\right]_{0}^{1} = \frac{1}{2}-0 = \frac{1}{2}. $$

The cancellation theorem applies when both requirements are met: the function is odd and the interval is symmetric about zero.

Why the Rule Is Useful

When an integrand is odd and its interval is symmetric, the theorem can give the exact value without finding an antiderivative. This is especially useful when an expression has several terms: check each term's behavior under \(x\mapsto -x\), then determine whether the whole integrand is odd. The third example used this approach for a sum of two odd terms.

The geometric interpretation is signed area. The portions on opposite sides of zero have equal magnitude and opposite sign, so they cancel in the definite integral. This does not say that the total area without signs is zero; it says that the signed contributions sum to zero. The distinction matters whenever a graph crosses the horizontal axis.

Key takeaway: If \(f\) is integrable and odd on \([-a,a]\), then its signed integral over that interval is zero. Check the function's parity and the interval separately before using the result.

Check Your Understanding

For each question, identify the symmetry and the conditions that justify your conclusion.

  1. What equation defines an odd function on a domain symmetric about zero?
  2. Why do paired terms in the proof's Riemann sums add to zero?
  3. Does the theorem apply to \(f(x)=x^3+x\) on \([-2,2]\)? Explain which conditions hold.
  4. Is \(f(x)=x^2\) odd or even, and what is \(\int_{-1}^{1}x^2\,dx\)?
  5. Why does oddness alone not imply that the integral over \([0,1]\) is zero?

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