/*! 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 25 Find the lengths of the curves. ... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the lengths of the curves. The curve \(r=\cos ^{3}(\theta / 3), \quad 0 \leq \theta \leq \pi / 4\)

Short Answer

Expert verified
The length of the curve is \( \frac{4\pi + 3}{32} \).

Step by step solution

01

Identify the formula for arc length in polar coordinates

The formula for the length of a curve in polar coordinates is given by \[ L = \int_{a}^{b} \sqrt{ \left( \frac{dr}{d\theta} \right)^2 + r^2 } d\theta \]where \( r = f(\theta) \).
02

Differentiate the function r with respect to θ

Given \( r = \cos^3(\theta/3) \), we need to find \( \frac{dr}{d\theta} \).Using the chain rule:1. \( u = \theta/3 \), so \( \frac{du}{d\theta} = 1/3 \).2. \( r = \cos^3(u) \), so \( \frac{dr}{du} = 3 \cos^2(u) \cdot (-\sin(u)) = -3 \cos^2(u) \sin(u) \).Using the chain rule, \( \frac{dr}{d\theta} = \frac{dr}{du} \cdot \frac{du}{d\theta} = -\cos^2(\theta/3) \sin(\theta/3) \).
03

Substitute into the arc length formula

Substitute \( r = \cos^3(\theta/3) \) and \( \frac{dr}{d\theta} = -\cos^2(\theta/3) \sin(\theta/3) \) into the arc length formula:\[ L = \int_{0}^{\pi/4} \sqrt{ \left( -\cos^2(\theta/3) \sin(\theta/3) \right)^2 + \cos^6(\theta/3) } d\theta \]Simplify the expression under the square root:\[ L = \int_{0}^{\pi/4} \sqrt{ \cos^4(\theta/3) \sin^2(\theta/3) + \cos^6(\theta/3) } d\theta \]\[ L = \int_{0}^{\pi/4} \cos^2(\theta/3) \sqrt{ \sin^2(\theta/3) + \cos^2(\theta/3) } d\theta \]Using \( \sin^2(x) + \cos^2(x) = 1 \), further simplifies to\[ L = \int_{0}^{\pi/4} \cos^2(\theta/3) d\theta \].
04

Evaluate the integral

To evaluate \( L = \int_{0}^{\pi/4} \cos^2(\theta/3) d\theta \), use the identity:\[ \cos^2(x) = \frac{1 + \cos(2x)}{2} \].Substituting and changing limits:\[ L = \int_{0}^{\pi/4} \frac{1 + \cos(2\theta/3)}{2} d\theta \].Separate into two integrals:\[ L = \frac{1}{2} \int_{0}^{\pi/4} d\theta + \frac{1}{2} \int_{0}^{\pi/4} \cos(2\theta/3) d\theta \].The first integral is straightforward:\[ \frac{1}{2} \int_{0}^{\pi/4} d\theta = \frac{\pi}{8} \].For the second,\[ \frac{1}{2} \int_{0}^{\pi/4} \cos(2\theta/3) d\theta \], let \( u = 2\theta/3 \), \( du = 2/3 \, d\theta \), then \( d\theta = \frac{3}{2} du \).Change of limits: when \( \theta = 0, u = 0 \) and when \( \theta = \pi/4, u = \pi/6 \).The second term becomes:\[ \int_{0}^{\pi/6} \cos(u) du = \sin(u) \bigg|_{0}^{\pi/6} = \frac{1}{2} \sin\left(\frac{\pi}{6}\right) = \frac{1}{2} \times \frac{1}{2} = \frac{1}{4} \].Thus, adding them together:\[ L = \frac{\pi}{8} + \frac{3}{8} \times \frac{1}{4} = \frac{\pi}{8} + \frac{3}{32} \].
05

Calculate the final result

Simplify and find a common denominator:\[ L = \frac{4\pi}{32} + \frac{3}{32} = \frac{4\pi + 3}{32} \].

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Key Concepts

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

polar coordinates
Polar coordinates provide a different way of representing points in a plane compared to Cartesian coordinates. Instead of using the standard x and y axes, polar coordinates use a distance from a reference point (radius, \( r \)) and an angle from a reference direction (angle, \( \theta \)). This system is particularly useful for curves that naturally involve circular patterns or rotational symmetry.

In polar coordinates, the position of a point is given by \( (r, \theta) \). The angle \( \theta \) is measured in radians or degrees from the positive x-axis, and the distance \( r \) denotes how far the point is from the origin.

For curves defined in polar coordinates, such as \( r = \cos^{3}(\theta / 3) \), the parameters \( \theta \) and \( r \) help to describe how the curve wraps or loops around the origin as \( \theta \) changes. In this exercise, you calculated the arc length of such a curve over a specific range of \( \theta \).

To find lengths of curves in polar coordinates, it is essential to grasp how these coordinates work relative to standard Cartesian processes.
calculus integration
In calculus, integration is a method of adding up small quantities to calculate the whole. Practically, this means finding areas, total amounts, or lengths of curves.

When dealing with arc length in polar coordinates, integration becomes useful. In our exercise, you computed how long a curve is by integrating a particular function over a certain range. Here, the integration process involved taking the square root of a function derived from the polar function.

This process captures the small lengths of each infinitesimal segment of the curve, adding them up to find the total arc length. Understanding integration in this context means recognizing how it sums up continuous variables, sometimes needing substitution or identities to simplify the integration.

We used the integral \( \int_{a}^{b} \sqrt{ \left( \frac{dr}{d\theta} \right)^2 + r^2 } d\theta \) to find the length of the curve. Each tiny slice of the curve contributes to the total length, and integration efficiently tallies these to deliver the complete arc length.
differentiation in calculus
Differentiation is all about finding how a function changes at a point. It's the process of determining the derivative, which represents how a function's output varies as its input changes.

In this exercise, you differentiated \( r = \cos^3(\theta/3) \) with respect to \( \theta \). By determining \( \frac{dr}{d\theta} \), you understand how the radial distance changes with the angle. Differentiation is crucial because it allows us to calculate the slope or rate of change of the curve at each point.

This rate of change informs how sharp or smooth the curve is, which then influences our integration step when finding the arc length. Without differentiation, we wouldn't have the integrand needed for the arc length formula.

Understanding differentiation includes grasping basic derivative rules and recognizing when to apply them, such as in our formula for arc length in polar coordinates.
chain rule in calculus
The chain rule is a fundamental rule in calculus for differentiating composed functions. It states that to differentiate a composite function, you first differentiate the outer function, then multiply it by the derivative of the inner function.

In the arc length problem, you applied the chain rule to differentiate \( r = \cos^3(\theta/3) \). This involved finding the derivative of the outer function \( \cos^3(u) \) with respect to the inner function \( u = \theta/3 \), and then differentiating \( u \) with respect to \( \theta \).

The chain rule simplifies complex differentiation tasks and ensures accurate results when functions are nested within each other.

Applying the chain rule, you transformed the original function step-by-step, keeping track of each differentiation task to arrive at \( \frac{dr}{d\theta} = -\cos^2(\theta/3) \sin(\theta/3) \). Utilizing the chain rule effectively often requires practice, but it is crucial for solving advanced calculus problems.

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Most popular questions from this chapter

\(r=f(\boldsymbol{\theta})\) vs. \(\boldsymbol{r}=2 \boldsymbol{f}(\boldsymbol{\theta}) \quad\) The curves \(r=f(\theta), \alpha \leq \theta \leq \beta,\) and \(r=2 f(\theta), \alpha \leq \theta \leq \beta,\) are revolved about the \(x\) -axis to generate surfaces. Can anything be said about the relative areas of these surfaces? Give reasons for your answer.

A rose within a rose Graph the equation \(r=1-2 \sin 3 \theta\)

The reflective property of parabolas The figure here shows a typical point \(P\left(x_{0}, y_{0}\right)\) on the parabola \(y^{2}=4 p x .\) The line \(L\) is tangent to the parabola at \(P .\) The parabola's focus lies at \(F(p, 0) .\) The ray \(L^{\prime}\) extending from \(P\) to the right is parallel to the \(x\) -axis. We show that light from \(F\) to \(P\) will be reflected out along \(L^{\prime}\) by showing that \(\beta\) equals \(\alpha\) . Establish this equality by taking the following steps. a. Show that \(\tan \beta=2 p / y_{0}\) . b. Show that \(\tan \phi=y_{0} /\left(x_{0}-p\right)\) c. Use the identity $$\tan \alpha=\frac{\tan \phi-\tan \beta}{1+\tan \phi \tan \beta}$$ to show that \(\tan \alpha=2 p / y_{0}\) since \(\alpha\) and \(\beta\) are both acute, \(\tan \beta=\tan \alpha\) implies \(\beta=\alpha\)

Graph the lines and conic sections in Exercises \(47-56\) $$ r=4 \sin \theta $$

Exercises \(29-36\) give the eccentricities of conic sections with one focus at the origin, along with the directrix corresponding to that focus. Find a polar equation for each conic section. $$ e=1 / 2, \quad x=1 $$

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