Examples of integrand in the following topics:
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- Trigonometric functions can be substituted for other expressions to change the form of integrands.
- If the integrand contains $a^2+x^2$, let $x = a \tan(\theta)$ and use the identity:
- If the integrand contains $x^2-a^2$, let $x = a \sec(\theta)$ and use the identity:
- Example 1: Integrals where the integrand contains $a^2 − x^2$ (where $a$ is positive)
- Example 2: Integrals where the integrand contains $a^2 − x^2$ (where $a$ is not zero)
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- The integrand $f(x)$ may be known only at certain points, such as obtained by sampling.
- A formula for the integrand may be known, but it may be difficult or impossible to find an antiderivative which is an elementary function.
- Numerical integration methods can generally be described as combining evaluations of the integrand to get an approximation to the integral.
- Also, each evaluation takes time, and the integrand may be arbitrarily complicated.
- A 'brute force' kind of numerical integration can be done, if the integrand is reasonably well-behaved (i.e. piecewise continuous and of bounded variation), by evaluating the integrand with very small increments.
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- The integrand $f(x)$ may be known only at certain points, such as when obtained by sampling.
- A formula for the integrand may be known, but it may be difficult or impossible to find an antiderivative which is an elementary function.
- An example of such an integrand $f(x)=\exp(-x^2)$, the antiderivative of which (the error function, times a constant) cannot be written in elementary form.
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- Integrals are also improper if the integrand is undefined at an interior point of the domain of integration, or at multiple such points.
- The problem here is that the integrand is unbounded in the domain of integration (the definition requires that both the domain of integration and the integrand be bounded).
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- In the integrand, the factor $x$ represents the radius of the cylindrical shell under consideration, while is equal to the height of the shell.
- Therefore, the entire integrand, $2\pi x \left | f(x) - g(x) \right | \,dx$, is nothing but the volume of the cylindrical shell.
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- $f(x)$, the function being integrated, is known as the integrand.
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- Depending on the value of $E_f/E_0$ this integral may vanish.Specifically the integrand is non-zero only if $\mu_f$ lies in the range
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- Similarly, an improper integral of a function, $\textstyle\int_0^\infty f(x)\,dx$, is said to converge absolutely if the integral of the absolute value of the integrand is finite—that is, if $\int_0^\infty \left|f(x)\right|dx = L$.
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- If $\omega \tau \gg\ 1$, the integrand will oscillate rapidly so the integral will be small.