08 Antiderivatives and Indefinite Integrals

A progressive guide to antiderivatives, indefinite integrals, integration rules, initial-value problems, motion, and substitution.

Understanding Antiderivatives

An reverses the process of differentiation. A function FF is an of ff on an interval when

F′(x)=f(x).F'(x)=f(x).

For example, because

ddx(x3)=3x2,\frac{d}{dx}(x^3)=3x^2,

one of 3x23x^2 is x3x^3. However, it is not the only one. Adding any constant does not change the derivative:

ddx(x3+C)=3x2.\frac{d}{dx}\bigl(x^3+C\bigr)=3x^2.

Thus, all antiderivatives of 3x23x^2 can be written as x3+Cx^3+C. More generally, any two antiderivatives of the same function differ by a constant on an interval.

For f(x)=6x−4f(x)=6x-4, integrate each term:

∫(6x−4) dx=3x2−4x+C.\int(6x-4)\,dx=3x^2-4x+C.

Differentiating gives

ddx(3x2−4x+C)=6x−4,\frac{d}{dx}(3x^2-4x+C)=6x-4,

which verifies the result.

Takeaway: Differentiation removes constants, so reversing differentiation requires including an arbitrary constant.

Reading Integral Notation

An is notation for the complete family of antiderivatives:

∫f(x) dx=F(x)+C,\int f(x)\,dx=F(x)+C,

where F′(x)=f(x)F'(x)=f(x). The parts of the notation have specific roles:

  • ∫\int is the integral sign.

  • f(x)f(x) is the .

  • dxdx identifies xx as the variable of integration.

  • CC is the arbitrary constant.

For example,

∫4x3 dx=x4+C.\int 4x^3\,dx=x^4+C.

This expression represents infinitely many functions, including x4x^4, x4+5x^4+5, and x4−12x^4-12. All have derivative 4x34x^3.

Do not confuse an with a . An expression such as

∫abf(x) dx\int_a^b f(x)\,dx

has bounds and produces a number when evaluated, whereas an produces a function family.

Takeaway: The absence of bounds signals a family of antiderivatives and therefore requires +C+C.

Core Integration Rules

Integration rules are obtained by reversing familiar differentiation rules. The constant rule is

∫k dx=kx+C,\int k\,dx=kx+C,

where kk is constant. The is

∫xn dx=xn+1n+1+C,n≠−1.\int x^n\,dx=\frac{x^{n+1}}{n+1}+C,\qquad n\ne -1.

The exponent increases by one, and the result is divided by the new exponent. The exceptional case n=−1n=-1 must be handled separately:

∫1x dx=ln⁡∣x∣+C.\int\frac{1}{x}\,dx=\ln|x|+C.

The absolute value is required because the derivative of ln⁡∣x∣\ln|x| is 1/x1/x for every x≠0x\ne0.

Constants can be factored out, and sums or differences can be integrated term by term:

∫kf(x) dx=k∫f(x) dx,\int kf(x)\,dx=k\int f(x)\,dx,
∫[f(x)±g(x)]dx=∫f(x) dx±∫g(x) dx.\int\bigl[f(x)\pm g(x)\bigr]dx=\int f(x)\,dx\pm\int g(x)\,dx.

Useful formulas include

  • ∫ex dx=ex+C\int e^x\,dx=e^x+C

  • ∫cos⁡x dx=sin⁡x+C\int\cos x\,dx=\sin x+C

  • ∫sin⁡x dx=−cos⁡x+C\int\sin x\,dx=-\cos x+C

  • ∫sec⁡2x dx=tan⁡x+C\int\sec^2x\,dx=\tan x+C

  • ∫csc⁡2x dx=−cot⁡x+C\int\csc^2x\,dx=-\cot x+C

  • ∫sec⁡xtan⁡x dx=sec⁡x+C\int\sec x\tan x\,dx=\sec x+C

  • ∫csc⁡xcot⁡x dx=−csc⁡x+C\int\csc x\cot x\,dx=-\csc x+C

  • ∫11+x2 dx=arctan⁡x+C\int\frac{1}{1+x^2}\,dx=\arctan x+C

  • ∫11−x2 dx=arcsin⁡x+C\int\frac{1}{\sqrt{1-x^2}}\,dx=\arcsin x+C

For a polynomial, integrate each term:

∫(5x4−2x3+7x−9) dx=x5−x42+7x22−9x+C.\begin{aligned} \int(5x^4-2x^3+7x-9)\,dx &=x^5-\frac{x^4}{2}+\frac{7x^2}{2}-9x+C. \end{aligned}

Differentiate the result to check every coefficient and exponent.

Takeaway: Apply linearity first, then use the appropriate basic formula, paying special attention to the 1/x1/x exception.

Solving Initial-Value Problems

An supplies both a differential equation and a value of the unknown function. A typical form is

dydx=f(x),y(x0)=y0.\frac{dy}{dx}=f(x),\qquad y(x_0)=y_0.

First find the general solution by integrating:

y=F(x)+C.y=F(x)+C.

Then substitute the given input and output to determine CC.

For

dydx=4x3−2x,y(1)=5,\frac{dy}{dx}=4x^3-2x,\qquad y(1)=5,

integration gives

y=x4−x2+C.y=x^4-x^2+C.

Applying the condition produces

5=14−12+C=C,5=1^4-1^2+C=C,

so the particular solution is

y=x4−x2+5.y=x^4-x^2+5.

Verify both parts: its derivative is 4x3−2x4x^3-2x, and its value at x=1x=1 is 55.

Takeaway: Integration gives a family of solutions; the initial condition selects one member of that family.

Motion from Velocity and Acceleration

In one-dimensional motion, position, velocity, and acceleration are linked by differentiation:

v(t)=s′(t),a(t)=v′(t)=s′′(t).v(t)=s'(t),\qquad a(t)=v'(t)=s''(t).

Integration reverses these relationships. If velocity is known, integrate once to find position. If acceleration is known, integrate once to find velocity and a second time to find position. Each integration introduces a constant, which must be determined from an initial position or velocity.

Suppose

v(t)=6t−4,s(0)=3.v(t)=6t-4,\qquad s(0)=3.

Since s′(t)=v(t)s'(t)=v(t),

s(t)=∫(6t−4) dt=3t2−4t+C.s(t)=\int(6t-4)\,dt=3t^2-4t+C.

Using s(0)=3s(0)=3 gives C=3C=3, so

s(t)=3t2−4t+3.s(t)=3t^2-4t+3.

If instead

a(t)=4,v(0)=7,s(0)=2,a(t)=4,\qquad v(0)=7,\qquad s(0)=2,

first integrate acceleration:

v(t)=4t+C1.v(t)=4t+C_1.

The velocity condition gives C1=7C_1=7, so v(t)=4t+7v(t)=4t+7. Integrating again,

s(t)=2t2+7t+C2.s(t)=2t^2+7t+C_2.

The position condition gives C2=2C_2=2, so

s(t)=2t2+7t+2.s(t)=2t^2+7t+2.

A final check is

s′(t)=4t+7=v(t),s′′(t)=4=a(t).s'(t)=4t+7=v(t),\qquad s''(t)=4=a(t).

A negative velocity means motion in the negative direction relative to the chosen positive direction.

Takeaway: Keep the order clear: acceleration integrates to velocity, and velocity integrates to position.

Substitution and the Reverse

Substitution, also called , reverses the . The has the form

ddxF(g(x))=F′(g(x))g′(x).\frac{d}{dx}F(g(x))=F'(g(x))g'(x).

Therefore, when an contains an inner expression and its derivative, set

u=g(x),du=g′(x) dx.u=g(x),\qquad du=g'(x)\,dx.

The integral then becomes an integral in uu. Use this sequence:

  1. Identify the inner expression g(x)g(x).

  2. Set u=g(x)u=g(x).

  3. Compute du=g′(x) dxdu=g'(x)\,dx.

  4. Rewrite the entire integral using uu and dudu.

  5. Integrate with respect to uu.

  6. Substitute back for uu.

  7. Differentiate the result to verify it.

For example,

∫6x(3x2+4)4 dx\int6x(3x^2+4)^4\,dx

has inner expression u=3x2+4u=3x^2+4, with du=6x dxdu=6x\,dx. Thus,

∫6x(3x2+4)4 dx=∫u4 du=u55+C.\int6x(3x^2+4)^4\,dx=\int u^4\,du=\frac{u^5}{5}+C.

Substituting back gives

∫6x(3x2+4)4 dx=(3x2+4)55+C.\int6x(3x^2+4)^4\,dx=\frac{(3x^2+4)^5}{5}+C.

When the derivative appears only up to a constant factor, adjust for that factor. For

∫xx2+1 dx,\int x\sqrt{x^2+1}\,dx,

let u=x2+1u=x^2+1. Since du=2x dxdu=2x\,dx, we have x dx=du/2x\,dx=du/2. Therefore,

∫xx2+1 dx=12∫u1/2 du=u3/23+C=(x2+1)3/23+C.\begin{aligned} \int x\sqrt{x^2+1}\,dx &=\frac12\int u^{1/2}\,du\\ &=\frac{u^{3/2}}{3}+C\\ &=\frac{(x^2+1)^{3/2}}{3}+C. \end{aligned}

Takeaway: Successful substitution replaces the inner expression and its differential completely, then returns to the original variable at the end.

Checking Work and Avoiding Errors

Several mistakes recur in problems:

  • Omitting the constant: Every needs +C+C.

  • Applying the to 1/x1/x: Because the exponent is −1-1, use ln⁡∣x∣+C\ln|x|+C instead.

  • Ignoring a missing factor: If du=2x dxdu=2x\,dx, then x dx=du/2x\,dx=du/2.

  • Leaving the answer in terms of uu: For an , substitute back into the original variable.

  • Confusing motion quantities: Integrate acceleration to obtain velocity before integrating velocity to obtain position.

  • Skipping verification: Differentiate the final expression whenever possible.

A useful general check is to compare the derivative of the proposed answer with the original :

ddx(proposed antiderivative)=original integrand.\frac{d}{dx}\bigl(\text{proposed antiderivative}\bigr)=\text{original integrand}.

For an , also substitute the specified input into the final function and confirm the required value.

Takeaway: Constants, exceptional formulas, variable changes, physical quantities, and differentiation checks are the main points requiring deliberate attention.