Skip to content

Mathematics · Ch 11 — Integral Calculus

Integrals of the Form $\int f(ax+b)\,dx$

11.4

Integrals of the Form $\int f(ax+b)\,dx$

The pattern that motivates this section. Every standard antiderivative on the table in §11.3 was built for a bare variable xx. What happens when the argument is not xx itself but a linear expression ax+bax+b — for instance sin⁡(2x+4)\sin(2x+4) or (4x+5)6(4x+5)^6 instead of sin⁡x\sin x or x6x^6?

Constants added/subtracted change nothing. From ddx ⁣[(x−a)1010]=(x−a)9\dfrac{d}{dx}\!\left[\dfrac{(x-a)^{10}}{10}\right]=(x-a)^9 we recover ∫(x−a)9 dx=(x−a)1010+c\displaystyle\int (x-a)^9\,dx=\dfrac{(x-a)^{10}}{10}+c; likewise ddx[sin⁡(x+k)]=cos⁡(x+k)\dfrac{d}{dx}[\sin(x+k)]=\cos(x+k) gives ∫cos⁡(x+k) dx=sin⁡(x+k)+c\displaystyle\int\cos(x+k)\,dx=\sin(x+k)+c. So whenever a constant is merely added to or subtracted from xx inside the argument, the fundamental antiderivative formula carries straight over unchanged — no correction factor needed.

A coefficient of xx DOES introduce a correction factor. But when xx is scaled — the argument is ax+bax+b rather than just x+bx+b — an extra factor appears. Differentiating 1lelx+m\dfrac1l e^{lx+m} by the chain rule gives elx+me^{lx+m}, so ∫elx+m dx=1lelx+m+c\displaystyle\int e^{lx+m}\,dx=\dfrac1l e^{lx+m}+c; similarly ddx ⁣[1asin⁡(ax+b)]=cos⁡(ax+b)\dfrac{d}{dx}\!\left[\dfrac1a\sin(ax+b)\right]=\cos(ax+b) gives ∫cos⁡(ax+b) dx=1asin⁡(ax+b)+c\displaystyle\int \cos(ax+b)\,dx=\dfrac1a\sin(ax+b)+c. In both cases the extra factor is exactly 1a\dfrac1a — the reciprocal of the coefficient of xx — because the chain rule multiplies the derivative of the outer function by the derivative of the inner linear argument, which is the constant aa; integrating undoes that multiplication by dividing by aa.

Note

The general rule. If ∫f(x) dx=g(x)+c\displaystyle\int f(x)\,dx = g(x)+c, then

∫f(ax+b) dx=1a g(ax+b)+c.\int f(ax+b)\,dx = \frac1a\,g(ax+b) + c.

In words: integrate as if the argument were a bare xx using the ordinary standard formula, then divide the whole result by the coefficient of xx inside the linear argument. (This shortcut can also be derived rigorously via the substitution method, taken up in higher study.)

Applying the rule across function families.

  • Powers of a linear argument. ∫(4x+5)6 dx=14⋅(4x+5)77+c=(4x+5)728+c\displaystyle\int (4x+5)^6\,dx = \frac14\cdot\frac{(4x+5)^7}{7}+c=\frac{(4x+5)^7}{28}+c. A negative or fractional exponent works identically: ∫15−2x dx=∫(15−2x)1/2dx=(1−2)(15−2x)3/23/2+c=−(15−2x)3/23+c\displaystyle\int \sqrt{15-2x}\,dx=\int(15-2x)^{1/2}dx=\left(\frac{1}{-2}\right)\frac{(15-2x)^{3/2}}{3/2}+c=-\frac{(15-2x)^{3/2}}{3}+c, and ∫dx(3x+7)4=∫(3x+7)−4dx=13⋅(3x+7)−3−3+c=−19(3x+7)3+c\displaystyle\int \frac{dx}{(3x+7)^4}=\int(3x+7)^{-4}dx=\frac13\cdot\frac{(3x+7)^{-3}}{-3}+c=-\frac{1}{9(3x+7)^3}+c.
  • Trigonometric arguments. ∫sin⁡(2x+4) dx=12(−cos⁡(2x+4))+c=−12cos⁡(2x+4)+c\displaystyle\int \sin(2x+4)\,dx=\frac12\big(-\cos(2x+4)\big)+c=-\frac12\cos(2x+4)+c; ∫sec⁡2(3+4x) dx=14tan⁡(3+4x)+c\displaystyle\int \sec^2(3+4x)\,dx=\frac14\tan(3+4x)+c; and ∫cosec(ax+b)cot⁡(ax+b) dx=−1a cosec(ax+b)+c\displaystyle\int \text{cosec}(ax+b)\cot(ax+b)\,dx=-\frac1a\,\text{cosec}(ax+b)+c.
  • Exponential arguments. ∫e3x dx=13e3x+c\displaystyle\int e^{3x}\,dx=\frac13e^{3x}+c, and with a negative coefficient ∫e5−4x dx=−14e5−4x+c\displaystyle\int e^{5-4x}\,dx=-\frac14e^{5-4x}+c (the sign of aa simply carries through the 1a\tfrac1a factor).
  • Reciprocal-linear (log⁡\log) arguments. ∫dx3x−2=13log⁡∣3x−2∣+c\displaystyle\int \frac{dx}{3x-2}=\frac13\log|3x-2|+c, and ∫dx5−4x=−14log⁡∣5−4x∣+c\displaystyle\int \frac{dx}{5-4x}=-\frac14\log|5-4x|+c. …