/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 30 Evaluate the integral and check ... [FREE SOLUTION] | 91Ó°ÊÓ

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Evaluate the integral and check your answer by differentiating. $$ \int\left[\phi+\frac{2}{\sin ^{2} \phi}\right] d \phi $$

Short Answer

Expert verified
The integral evaluates to \( \frac{\phi^2}{2} - 2 \cot \phi + C \).

Step by step solution

01

Integrate the First Term

We start by integrating each term separately. The integral of the first term, \( \phi \), with respect to \( \phi \), is straightforward. \[ \int \phi \, d\phi = \frac{\phi^2}{2}. \]
02

Integrate the Second Term

For the second term \( \frac{2}{\sin^2 \phi} \), we recognize that \( \frac{1}{\sin^2 \phi} \) is equal to \( \csc^2 \phi \), whose integral is \( -\cot \phi \). Thus,\[ \int \frac{2}{\sin^2 \phi} \, d\phi = 2 \int \csc^2 \phi \, d\phi = -2 \cot \phi. \]
03

Combine the Integrals

Add the results of the previous steps to find the indefinite integral of the entire expression:\[ \int \left[ \phi + \frac{2}{\sin^2 \phi} \right] \, d\phi = \frac{\phi^2}{2} - 2 \cot \phi + C, \]where \( C \) is the constant of integration.
04

Differentiate to Check the Solution

Differentiate the result to ensure it matches the original integrand. The derivative of \( \frac{\phi^2}{2} \) is \( \phi \), and the derivative of \( -2 \cot \phi \) is \( \frac{2}{\sin^2 \phi} \). Thus, differentiating:\[ \frac{d}{d\phi} \left( \frac{\phi^2}{2} - 2 \cot \phi + C \right) = \phi + \frac{2}{\sin^2 \phi}. \]This matches the original integrand, confirming that our integration is correct.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Integrals
The concept of integrals is a cornerstone of calculus. Integration is essentially the process of finding the accumulated sum over an interval. In simpler terms, it's like adding up slices to find the whole area under a curve. For indefinite integrals, like the one in our exercise, we find a function whose derivative gives us the original function we started with.

To tackle the integral \[ \int\left[\phi+\frac{2}{\sin ^{2} \phi}\right] d \phi \] we separated it into two terms. First, the simple term \( \phi \), which integrates to \( \frac{\phi^2}{2} \).
  • An integral simplifies a lot when it deals with a polynomial term like \( \phi \).
The second term \( \frac{2}{\sin^2 \phi} \) is a bit more complex as it involves a trigonometric function. However, recognizing that \( \frac{1}{\sin^2 \phi} \) translates to \( \csc^2 \phi \) helps us solve it.

Integrals often have this creative component where identifying equivalent expressions can make solving them easier. The complete integral solution includes an arbitrary constant \( C \), since indefinite integrals represent a family of functions.
Differentiation
Differentiation is the process of finding the rate at which things change. It tells you how a function's output value changes as its input changes. In our problem, differentiation serves another important purpose: verifying the integration.

Once we have the integral \[ \frac{\phi^2}{2} - 2 \cot \phi + C \]we use differentiation to check our work. Start by taking the derivative of each term:
  • The derivative of \( \frac{\phi^2}{2} \) is simply \( \phi \).
  • For \( -2 \cot \phi \), using the rule that the derivative of \( \cot \phi \) is \( -\csc^2 \phi \), gives us \( \frac{2}{\sin^2 \phi} \).
Adding these results gives us back the original function from our integral \( \phi+\frac{2}{\sin ^{2} \phi} \). The fact that we return to the original function verifies that our integration was done correctly. Differentiation, therefore, acts like a double-check, providing confidence in our solution.
Trigonometric Functions
Trigonometric functions, like sine, cosine, and tangent, relate the angles of a triangle to the lengths of its sides. In calculus, they frequently appear in problems involving periodic phenomena or in specific substitution techniques.

In our exercise, recognizing \( \frac{2}{\sin^2 \phi} \) as \( 2 \csc^2 \phi \) is a crucial step. The csc function, or cosecant, is simply \( 1/\sin \phi \). It shows how interchangeable trigonometric identities can simplify problems.
  • The function \( \csc^2 \phi \) has a particularly useful integral: it equals \( -\cot \phi \).
  • Recognizing these patterns or identities can simplify integration or differentiation problems significantly.
So, understanding these functions and their derivatives is key. Trigonometry in calculus often involves switching between equivalent forms to make solving easier. The ability to spot these transformations will greatly enhance problem-solving efficiency.

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Most popular questions from this chapter

Electricity is supplied to homes in the form of alternating current, which means that the voltage has a sinusoidal waveform described by an equation of the form $$ V=V_{p} \sin (2 \pi f t) $$ (see the accompanying figure). In this equation, \(V_{p}\) is called the peak voltage or amplitude of the current, \(f\) is called its frequency, and \(1 / f\) is called its period. The voltages \(V\) and \(V_{p}\) are measured in volts \((\mathrm{V})\), the time \(t\) is measured in seconds (s), and the frequency is measured in hertz (Hz). \((1 \mathrm{~Hz}=1\) cycle per second; a cycle is the electrical term for one period of the waveform.) Most alternating-current voltmeters read what is called the \(\boldsymbol{r m s}\) or root-mean-square value of \(V\). By definition, this is the square root of the average value of \(V^{2}\) over one period. (a) Show that $$ V_{\mathrm{rms}}=\frac{V_{p}}{\sqrt{2}} $$ [Hint: Compute the average over the cycle from \(t=0\) to \(t=1 / f\), and use the identity \(\sin ^{2} \theta=\frac{1}{2}(1-\cos 2 \theta)\) to help evaluate the integral.] (b) In the United States, electrical outlets supply alternating current with an rms voltage of \(120 \mathrm{~V}\) at a frequency of \(60 \mathrm{~Hz}\). What is the peak voltage at such an outlet?

$$ \int x^{2} e^{-2 x^{3}} d x $$

By writing out the sums, determine whether the following are valid identities. (a) \(\int\left[\sum_{i=1}^{n} f_{i}(x)\right] d x=\sum_{i=1}^{n}\left[\int f_{i}(x) d x\right]\) (b) \(\frac{d}{d x}\left[\sum_{i=1}^{n} f_{i}(x)\right]=\sum_{i=1}^{n}\left[\frac{d}{d x}\left[f_{i}(x)\right]\right]\)

$$ \begin{aligned} &\begin{aligned} &\hline \end{aligned}\\\ &\int \sec ^{4} 3 \theta d \theta[\text { Hint: Apply a trigonometric identity.] } \end{aligned} $$

Let $$ I=\int_{-1}^{1} \frac{1}{1+x^{2}} d x $$ (a) Explain why \(I>0\). (b) Show that the substitution \(x=1 / u\) results in $$ I=-\int_{-1}^{1} \frac{1}{1+x^{2}} d x=-I $$ Thus, \(2 I=0\), which implies that \(I=0 .\) But this contradicts part (a). What is the error?

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