Unit 6 · Topic 6.6 Beta

Properties of Definite Integrals

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A definite integral is the limit of Riemann sums, and sums obey simple rules: you can split them, reorder them and pull out common factors. Those rules carry over to integrals. They let you compute new integrals from ones you already know, without ever finding a formula.

Adjacent intervals add

A positive curve y = f(x) over points a, b and c on the x-axis. The region under the curve from a to b is shaded crimson and from b to c blue. The equation reads: the integral of f from a to c equals the integral from a to b plus the integral from b to c.
Figure 1. The area from a to c is the area from a to b plus the area from b to c. LevlPrep original diagram.

If you accumulate from aa to bb and then from bb to cc, you have accumulated from aa to cc:

∫abf(x)dx+∫bcf(x)dx=∫acf(x)dx.\int_a^b f(x)\,dx + \int_b^c f(x)\,dx = \int_a^c f(x)\,dx.

This additivity is the property used most. It works in reverse too: ∫37f\int_3^7 f=∫07f−∫03f= \int_0^7 f - \int_0^3 f.

Worked example 1. Given ∫03f(x)dx\int_0^3 f(x)\,dx=5= 5 and ∫07f(x)dx\int_0^7 f(x)\,dx=12= 12, find ∫37f(x)dx\int_3^7 f(x)\,dx.

∫03f\int_0^3 f+∫37f+ \int_3^7 f=∫07f= \int_0^7 f, so 5+∫37f5 + \int_3^7 f=12= 12 and ∫37f(x)dx\int_3^7 f(x)\,dx=7= 7.

Reversed limits and equal limits

∫ab\int_a^b runs from aa to bb. Writing the limits the other way runs the interval backward, so every width Δx\Delta x is negative and the value changes sign:

∫baf(x)dx=−∫abf(x)dx,∫aaf(x)dx=0.\int_b^a f(x)\,dx = -\int_a^b f(x)\,dx, \qquad \int_a^a f(x)\,dx = 0.

With reversal, additivity holds for any order of aa, bb and cc. This matters for accumulation functions. If g(x)g(x)=∫2xf(t)dt= \int_2^x f(t)\,dt and x=0x = 0 is to the left of the lower limit, then g(0)g(0)=∫20f(t)dt= \int_2^0 f(t)\,dt=−∫02f(t)dt= -\int_0^2 f(t)\,dt. A positive ff there gives a negative g(0)g(0). The exam tests this every few years.

Constants and sums

A constant factor and a sum pass through every Riemann sum, so they pass through the integral:

∫ab(kf(x)+g(x))dx=k∫abf(x)dx+∫abg(x)dx.\int_a^b \left(kf(x) + g(x)\right)dx = k\int_a^b f(x)\,dx + \int_a^b g(x)\,dx.

A constant by itself is a rectangle: ∫abkdx\int_a^b k\,dx=k(b−a)= k(b - a).

Worked example 2. Also given ∫37g(x)dx\int_3^7 g(x)\,dx=−2= -2. Find ∫73(2f(x)−g(x))dx\int_7^3 \left(2f(x) - g(x)\right)dx and ∫37(f(x)+4)dx\int_3^7 \left(f(x) + 4\right)dx.

First, the integral from 3 to 7: 2(7)−(−2)=162(7) - (-2) = 16. The limits are reversed, so ∫73(2f−g)dx\int_7^3 (2f - g)\,dx=−16= -16.

Second: ∫37f(x)dx\int_3^7 f(x)\,dx+∫374dx+ \int_3^7 4\,dx=7= 7+4⋅4+ 4 \cdot 4=23= 23. The constant is integrated over the interval of width 4; writing 7+4=117 + 4 = 11 is the classic slip.

Products do not split: ∫abf(x)g(x)dx\int_a^b f(x)g(x)\,dx is not the product of the two integrals. Try f=g=1f = g = 1 on [0,2][0, 2]: the integral of the product is 2, the product of the integrals is 4.

Integrals from geometry, including breaks

When the graph is made of segments and circular arcs, split the interval where the pieces change, find each signed area, and add. Half a disc of radius rr has area 12πr2\frac{1}{2}\pi r^2; a quarter disc, 14πr2\frac{1}{4}\pi r^2.

A function with a jump or a removable discontinuity can still be integrated, as long as it stays bounded: split at the break. A single point has no width, so the value of the function at the jump does not change the integral. For p(x)=xp(x) = x when x<2x < 2 and p(x)=5p(x) = 5 when x≥2x \ge 2:

∫04p(x)dx=∫02xdx+∫245dx=2+10=12.\int_0^4 p(x)\,dx = \int_0^2 x\,dx + \int_2^4 5\,dx = 2 + 10 = 12.

The rules at a glance

RuleFormula
zero width∫aaf(x)dx\int_a^a f(x)\,dx=0= 0
reversed limits∫baf(x)dx\int_b^a f(x)\,dx=−∫abf(x)dx= -\int_a^b f(x)\,dx
additivity∫abf(x)dx\int_a^b f(x)\,dx+∫bcf(x)dx+ \int_b^c f(x)\,dx=∫acf(x)dx= \int_a^c f(x)\,dx
constant multiple∫abkf(x)dx\int_a^b kf(x)\,dx=k∫abf(x)dx= k\int_a^b f(x)\,dx
sum∫ab(f(x)+g(x))dx\int_a^b (f(x) + g(x))\,dx=∫abf(x)dx= \int_a^b f(x)\,dx+∫abg(x)dx+ \int_a^b g(x)\,dx
constant∫abkdx\int_a^b k\,dx=k(b−a)= k(b - a)

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