Intefinite integrals

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Primitives

Differentiation assigns to each function a unique derivative by definition. The inverse process asks whether, for a given function $f(x)$, there exists a function $F(x)$ whose derivative is exactly $f(x)$. Such a function is called a primitive of $f$. Formally, $F(x)$ is a primitive of $f(x)$ on the interval $[a, b]$ if $F$ is differentiable throughout $[a, b]$ and:

F'(x) = f(x), \quad \forall x \in [a, b]

Not every function admits a primitive on a given interval. A sufficient condition is continuity: every continuous function on a closed interval $[a, b]$ admits a primitive there. The converse does not hold in general. As an example, if $f(x) = 3x^2$, a primitive is $F(x) = x^3$, since:

\frac{d}{dx} x^3 = 3x^2

Unlike derivatives, primitives are not unique. Since the derivative of any constant is zero, the functions $x^3$, $x^3 + 5$, and $x^3 - \frac{1}{2}$ are all primitives of $3x^2$. More generally, if $F(x)$ is a primitive of $f(x)$, then so is $F(x) + c$ for any $c \in \mathbb{R}$, since:

\frac{d}{dx}[F(x) + c] = F'(x) = f(x)

Conversely, any two primitives of the same function differ by a constant. If $F_1(x)$ and $F_2(x)$ are both primitives of $f(x)$, then:

\frac{d}{dx}[F_1(x) - F_2(x)] = F_1'(x) - F_2'(x) = f(x) - f(x) = 0

which implies $F_1(x) - F_2(x) = c$ for some constant $c \in \mathbb{R}$.


What is the indefinite integral

The indefinite integral of a function $f(x)$ is the set of all its primitives. Since any two primitives differ by a constant, the entire family is expressed as $F(x) + c$ for $c \in \mathbb{R}$, and is denoted:

\int f(x) \, dx = F(x) + c, \quad c \in \mathbb{R}

From this definition it follows directly that:

\frac{d}{dx}\left[ \int f(x) \, dx \right] = f(x)

Differentiating an indefinite integral returns the original function. This relationship is made precise by the Fundamental Theorem of Calculus, which establishes the formal connection between differentiation and integration.


Example 1

Find the primitive of $f(x) = 3x$ that passes through the point $(2, 1)$. The general primitive is obtained by integrating:

F(x) = \int 3x \, dx = \frac{3}{2}x^2 + c

To determine the constant, the condition $F(2) = 1$ is imposed:

\begin{align} \frac{3}{2}(2)^2 + c &= 1 \\[6pt] 6 + c &= 1 \\[6pt] c &= -5 \end{align}

The unique primitive satisfying the given a is $F(x) = \frac{3}{2}x^2 - 5$.


Linearity properties

The indefinite integral is a linear operator. The integral of a sum of integrable functions equals the sum of their integrals:

\int \left[ f(x) + g(x) \right] \, dx = \int f(x) \, dx + \int g(x) \, dx \tag{1}

A constant factor can be moved outside the integral sign:

\int k f(x) \, dx = k \int f(x) \, dx, \quad \forall k \in \mathbb{R} \tag{2}

Example 2

Compute the integral of $f(x) = 3x^2 + 2x$. Applying property $1$, the integral splits into two terms, each of which falls under the power rule:

\int (3x^2 + 2x) \, dx = \int 3x^2 \, dx + \int 2x \, dx

The two integration constants arising from each term combine into a single arbitrary constant, giving $x^3 + x^2 + c$ with $c \in \mathbb{R}$.


Example 3

Compute the integral of $f(x) = 5\sin(x)$. Applying property $2$, the constant factor is moved outside the integral:

\int 5\sin(x) \, dx = 5 \int \sin(x) \, dx

Since the integral of $\sin(x)$ is $-\cos(x)$, the result is $-5\cos(x) + c$ with $c \in \mathbb{R}$.


Integral of a power function

The integral of a power function $x^a$ with $a \in \mathbb{R}$ and $a \neq -1$ is given by:

\int x^a \, dx = \frac{x^{a+1}}{a+1} + c

The case $a = -1$ requires a separate treatment and is discussed in the next section.


Example 4

Compute the following integral:

\int (3x^4 + 5x^2) \, dx

Applying linearity, the constant factors are moved outside and the power rule is applied to each term:

\int (3x^4 + 5x^2) \, dx = 3 \int x^4 \, dx + 5 \int x^2 \, dx = 3 \cdot \frac{x^5}{5} + 5 \cdot \frac{x^3}{3} + c

The result is $\dfrac{3}{5}x^5 + \dfrac{5}{3}x^3 + c$ with $c \in \mathbb{R}$.


Example 5

Compute the following integral:

\int \left( 4x^3 - \frac{3}{\sqrt{x}} + 2\cos x \right) \, dx

Applying linearity, the integral splits into three terms:

\int 4x^3 \, dx - \int 3x^{-1/2} \, dx + \int 2\cos x \, dx

The first term follows directly from the power rule: $\int 4x^3 \, dx = x^4$. For the second, rewriting $\frac{1}{\sqrt{x}}$ as $x^{-1/2}$ and applying the power rule with $a = -\frac{1}{2}$ gives $\int 3x^{-1/2} \, dx = 6\sqrt{x}$. The third term follows from the standard integral of the cosine: $\int 2\cos x \, dx = 2\sin x$.

Assembling the three contributions:

\int \left( 4x^3 - \frac{3}{\sqrt{x}} + 2\cos x \right) \, dx = x^4 - 6\sqrt{x} + 2\sin x + c

The result can be verified by differentiating $x^4 - 6\sqrt{x} + 2\sin x + c$ term by term, which returns the original integrand.


The logarithmic integral

When $a = -1$, the power rule formula produces a zero denominator and does not apply. The integral in this case is:

\int \frac{1}{x} \, dx = \ln |x| + c

This follows from the fact that $\frac{d}{dx} \ln |x| = \frac{1}{x}$, which holds for all $x \neq 0$. The absolute value is necessary because $\ln$ is defined only for positive arguments, while $\frac{1}{x}$ is defined on both $(-\infty, 0)$ and $(0, +\infty)$.

The identity $\int \frac{1}{x} \, dx = \ln |x| + c$ holds separately on $(-\infty, 0)$ and on $(0, +\infty)$. On each interval the arbitrary constant may take a different value, so the most general antiderivative of $\frac{1}{x}$ on its full domain is not a single expression $\ln |x| + c$ with one constant, but a piecewise family with independent constants on the two components.


Fundamental integration rules

Linearity\[ \int \left( f(x) + g(x)\right)\, dx = \int f(x)\, dx + \int g(x)\, dx \]
Linearity\[ \int k\, f(x)\, dx = k \int f(x)\, dx \]
Power rule\[ \int x^a\, dx = \dfrac{x^{a+1}}{a+1} + c \quad a \neq -1 \]
Logarithmic case\[ \int \dfrac{1}{x} \,dx = \ln|x| + c \]

Common Integrals

Below is a summary of the most common basic integrals, useful in calculus and for transforming complex expressions into simpler, well-known forms.

These identities hold on any interval where the integrand is defined and continuous.