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Mathematics · Ch 11 — Definite Integration

Properties of Definite Integrals

11.2.1

Properties of Definite Integrals

These eight properties let a definite integral be simplified — often to zero, or to twice a simpler integral, or to another definite integral that is easier to handle — purely by symmetry or by a change of variable, without ever writing down the antiderivative explicitly. In every proof below, gg denotes any primitive of ff, i.e. ∫f(x) dx=g(x)+c\int f(x)\,dx=g(x)+c, and the Fundamental Theorem (Section 4.2) is used to convert each bracketed evaluation.

Property I. ∫aaf(x) dx=0\displaystyle\int_a^a f(x)\,dx = 0.

Proof: ∫aaf(x) dx=[g(x)+c]aa=(g(a)+c)−(g(a)+c)=0\int_a^a f(x)\,dx=[g(x)+c]_a^a=(g(a)+c)-(g(a)+c)=0 — the upper and lower limit are the same point, so the bracket has nothing to measure.

Property II. ∫abf(x) dx=−∫baf(x) dx\displaystyle\int_a^b f(x)\,dx = -\int_b^a f(x)\,dx.

Proof: ∫abf(x) dx=g(b)−g(a)=−(g(a)−g(b))=−∫baf(x) dx\int_a^b f(x)\,dx=g(b)-g(a)=-\big(g(a)-g(b)\big)=-\int_b^a f(x)\,dx. Swapping the limits of a definite integral flips its sign.

Worked examples: ∫31x dx=[x22]31=12−92=−4\int_3^1 x\,dx=\left[\frac{x^2}2\right]_3^1=\frac12-\frac92=-4, while ∫13x dx=[x22]13=92−12=4\int_1^3 x\,dx=\left[\frac{x^2}2\right]_1^3=\frac92-\frac12=4 — exactly the negative of each other, confirming the property.

Property III. ∫abf(x) dx=∫abf(t) dt\displaystyle\int_a^b f(x)\,dx = \int_a^b f(t)\,dt.

Proof: both sides reduce, via the Fundamental Theorem, to g(b)−g(a)g(b)-g(a) regardless of whether the dummy integration variable is called xx or tt. This says definite integration is independent of the name given to the variable — the definite integral is a fixed number determined only by ff, aa, and bb, not by the symbol used inside. Worked example: both ∫π/6π/3cos⁡x dx\int_{\pi/6}^{\pi/3}\cos x\,dx and ∫π/6π/3cos⁡t dt\int_{\pi/6}^{\pi/3}\cos t\,dt evaluate to [sin⁡(⋅)]π/6π/3=sin⁡π3−sin⁡π6=32−12=3−12[\sin(\cdot)]_{\pi/6}^{\pi/3}=\sin\frac\pi3-\sin\frac\pi6=\frac{\sqrt3}2-\frac12=\frac{\sqrt3-1}2.

Property IV (additivity over sub-intervals). ∫abf(x) dx=∫acf(x) dx+∫cbf(x) dx\displaystyle\int_a^b f(x)\,dx = \int_a^c f(x)\,dx+\int_c^b f(x)\,dx, for any c∈[a,b]c\in[a,b].

Proof: the right side is (g(c)−g(a))+(g(b)−g(c))=g(b)−g(a)\big(g(c)-g(a)\big)+\big(g(b)-g(c)\big)=g(b)-g(a), which is exactly the left side. Worked example: for ∫−15(2x+3) dx\int_{-1}^5(2x+3)\,dx with c=3c=3, both the direct evaluation [x2+3x]−15=(25+15)−(1−3)=42[x^2+3x]_{-1}^5=(25+15)-(1-3)=42 and the split evaluation [x2+3x]−13+[x2+3x]35=[(9+9)−(1−3)]+[(25+15)−(9+9)]=20+22=42[x^2+3x]_{-1}^3+[x^2+3x]_3^5=\big[(9+9)-(1-3)\big]+\big[(25+15)-(9+9)\big]=20+22=42 agree.

Property V. ∫abf(x) dx=∫abf(a+b−x) dx\displaystyle\int_a^b f(x)\,dx = \int_a^b f(a+b-x)\,dx.

Proof: substitute t=a+b−xt=a+b-x in the right side, so x=a+b−tx=a+b-t, dx=−dtdx=-dt; as xx runs from aa to bb, tt runs from bb down to aa. So ∫abf(a+b−x) dx=∫baf(t)(−dt)=−∫baf(t) dt=∫abf(t) dt\int_a^b f(a+b-x)\,dx=\int_b^a f(t)(-dt)=-\int_b^a f(t)\,dt=\int_a^b f(t)\,dt (using Property II), which by Property III equals ∫abf(x) dx\int_a^b f(x)\,dx. This is the single most useful property in the chapter: reflecting xx about the midpoint of [a,b][a,b] never changes the value of the integral.

Worked example: for I=∫π/6π/3sin⁡2x dxI=\int_{\pi/6}^{\pi/3}\sin^2x\,dx, reflecting via x→π6+π3−x=π2−xx\to\frac\pi6+\frac\pi3-x=\frac\pi2-x turns sin⁡2x\sin^2x into sin⁡2 ⁣(π2−x)=cos⁡2x\sin^2\!\big(\frac\pi2-x\big)=\cos^2x, so I=∫π/6π/3cos⁡2x dxI=\int_{\pi/6}^{\pi/3}\cos^2x\,dx too. Adding the two expressions for II: 2I=∫π/6π/3(sin⁡2x+cos⁡2x) dx=∫π/6π/31 dx=π3−π6=π62I=\int_{\pi/6}^{\pi/3}(\sin^2x+\cos^2x)\,dx=\int_{\pi/6}^{\pi/3}1\,dx=\frac\pi3-\frac\pi6=\frac\pi6, so I=π12I=\frac\pi{12}.

Property VI. ∫0af(x) dx=∫0af(a−x) dx\displaystyle\int_0^a f(x)\,dx = \int_0^a f(a-x)\,dx — the special case of Property V when the lower limit is 00 (so a+b−xa+b-x becomes a−xa-x).

Worked example: for I=∫0π/4log⁡(1+tan⁡x) dxI=\int_0^{\pi/4}\log(1+\tan x)\,dx, reflecting via x→π4−xx\to\frac\pi4-x and using tan⁡ ⁣(π4−x)=1−tan⁡x1+tan⁡x\tan\!\big(\frac\pi4-x\big)=\dfrac{1-\tan x}{1+\tan x} gives 1+tan⁡ ⁣(π4−x)=21+tan⁡x1+\tan\!\big(\frac\pi4-x\big)=\dfrac{2}{1+\tan x}, so I=∫0π/4[log⁡2−log⁡(1+tan⁡x)]dx=(log⁡2)⋅π4−II=\int_0^{\pi/4}\big[\log2-\log(1+\tan x)\big]dx=\big(\log2\big)\cdot\frac\pi4-I. Solving, 2I=π4log⁡22I=\frac\pi4\log2, so I=π8log⁡2I=\frac\pi8\log2.

Property VII. ∫02af(x) dx=∫0af(x) dx+∫0af(2a−x) dx\displaystyle\int_0^{2a} f(x)\,dx = \int_0^a f(x)\,dx+\int_0^a f(2a-x)\,dx.

Proof: in the second term on the right, substitute t=2a−xt=2a-x (dx=−dtdx=-dt; x:0→ax:0\to a gives t:2a→at:2a\to a), so ∫0af(2a−x) dx=∫2aaf(t)(−dt)=∫a2af(t) dt\int_0^a f(2a-x)\,dx=\int_{2a}^a f(t)(-dt)=\int_a^{2a}f(t)\,dt. Adding ∫0af(x) dx+∫a2af(x) dx\int_0^a f(x)\,dx+\int_a^{2a}f(x)\,dx gives exactly ∫02af(x) dx\int_0^{2a}f(x)\,dx by Property IV. This is the tool used whenever the upper limit is twice the useful reflection point.

Property VIII (odd/even functions).

∫−aaf(x) dx={2∫0af(x) dx,f even (f(−x)=f(x))0,f odd (f(−x)=−f(x))\int_{-a}^a f(x)\,dx = \begin{cases} 2\displaystyle\int_0^a f(x)\,dx, & f \text{ even } (f(-x)=f(x))\\[4pt] 0, & f \text{ odd } (f(-x)=-f(x)) \end{cases} …