The pattern that motivates this section. Every standard antiderivative on the table in §11.3 was built for a bare variable x. What happens when the argument is not x itself but a linear expression ax+b — for instance sin(2x+4) or (4x+5)6 instead of sinx or x6?
Constants added/subtracted change nothing. From dxd[10(x−a)10]=(x−a)9 we recover ∫(x−a)9dx=10(x−a)10+c; likewise dxd[sin(x+k)]=cos(x+k) gives ∫cos(x+k)dx=sin(x+k)+c. So whenever a constant is merely added to or subtracted from x inside the argument, the fundamental antiderivative formula carries straight over unchanged — no correction factor needed.
A coefficient of x DOES introduce a correction factor. But when x is scaled — the argument is ax+b rather than just x+b — an extra factor appears. Differentiating l1elx+m by the chain rule gives elx+m, so ∫elx+mdx=l1elx+m+c; similarly dxd[a1sin(ax+b)]=cos(ax+b) gives ∫cos(ax+b)dx=a1sin(ax+b)+c. In both cases the extra factor is exactly a1 — the reciprocal of the coefficient of x — because the chain rule multiplies the derivative of the outer function by the derivative of the inner linear argument, which is the constant a; integrating undoes that multiplication by dividing by a.
Note
The general rule. If ∫f(x)dx=g(x)+c, then
∫f(ax+b)dx=a1g(ax+b)+c.
In words: integrate as if the argument were a bare x using the ordinary standard formula, then divide the whole result by the coefficient of x 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)6dx=41⋅7(4x+5)7+c=28(4x+5)7+c. A negative or fractional exponent works identically: ∫15−2xdx=∫(15−2x)1/2dx=(−21)3/2(15−2x)3/2+c=−3(15−2x)3/2+c, and ∫(3x+7)4dx=∫(3x+7)−4dx=31⋅−3(3x+7)−3+c=−9(3x+7)31+c.
Trigonometric arguments.∫sin(2x+4)dx=21(−cos(2x+4))+c=−21cos(2x+4)+c; ∫sec2(3+4x)dx=41tan(3+4x)+c; and ∫cosec(ax+b)cot(ax+b)dx=−a1cosec(ax+b)+c.
Exponential arguments.∫e3xdx=31e3x+c, and with a negative coefficient ∫e5−4xdx=−41e5−4x+c (the sign of a simply carries through the a1 factor).
Reciprocal-linear (log) arguments.∫3x−2dx=31log∣3x−2∣+c, and ∫5−4xdx=−41log∣5−4x∣+c. …