Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Arc length using technology Use a calculator to find the approximate length of the following curves. $$\text { The lemniscate } r^{2}=6 \sin 2 \theta$$

Short Answer

Expert verified
Answer: The approximate length of the curve is 9.688.

Step by step solution

01

Calculate the derivatives of $$r^2$$ with respect to $$\theta$$.

We are given the polar equation $$r^2 = 6 \sin 2 \theta$$, and we need to find $$\frac{dr}{d\theta}$$. First, we differentiate both sides of the equation with respect to $$\theta$$: $$2r\frac{dr}{d\theta} = 12\cos 2\theta$$ Now, we need to isolate $$\frac{dr}{d\theta}$$: $$\frac{dr}{d\theta} = \frac{6\cos 2\theta}{r}$$
02

Plug our derivatives and our polar equation into the arc length formula.

We will substitute the expression for $$r^2$$ and $$\frac{dr}{d\theta}$$ into the arc length formula: $$L = \int_{\alpha}^{\beta} \sqrt{6 \sin 2 \theta + \Big(\frac{6\cos 2\theta}{\sqrt{6 \sin 2 \theta}}\Big)^2} d\theta$$
03

Determine the appropriate integration bounds.

A lemniscate has symmetry in both the x and y axes. We can take advantage of this symmetry and just find the arc length of one loop and then multiply it by 2. To do this, we will find the arc length between points where $$\theta = 0$$ and $$\theta = \frac{\pi}{2}$$, since the lemniscate intersects the x-axis at these points: $$L = 2\int_{0}^{\frac{\pi}{2}} \sqrt{6 \sin 2 \theta + \Big(\frac{6\cos 2\theta}{\sqrt{6 \sin 2 \theta}}\Big)^2} d\theta$$
04

Use a calculator to evaluate the integral and get the approximate arc length.

Now, using a calculator to evaluate the integral, we find the approximate arc length of the lemniscate: $$L \approx 2\int_{0}^{\frac{\pi}{2}} \sqrt{6 \sin(2 \theta) + \Big(\frac{6\cos(2 \theta)}{\sqrt{6 \sin(2 \theta)}}\Big)^2} d\theta \approx 9.688$$ So, the approximate length of the curve is 9.688.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Lemniscate
The lemniscate is a fascinating mathematical curve that resembles the shape of an infinity symbol (∞) or a figure eight. It is known for its intriguing properties in geometry and calculus. The particular lemniscate described by the equation \(r^2 = 6 \sin 2\theta\) in polar coordinates has some unique characteristics. By its nature, a lemniscate is symmetric about the origin, meaning it looks the same on both sides of every axis crossing through the origin.
The structure of a lemniscate in polar coordinates relies heavily on polar equations. These curves have two loops, and depending on the parameters of the equation, the size and shape of these loops can vary. Such properties often make the lemniscate a point of interest in advanced mathematics studies. To find specifics about any lemniscate, often calculus is applied, as seen in the determination of arc lengths or enclosed areas.
Polar Coordinates
Polar coordinates provide a different method for describing the location of a point in a plane, using a distance and an angle from a fixed point, usually the origin. They are particularly helpful in dealing with complex curves like the lemniscate, where the form in rectangular (Cartesian) coordinates would be awkward.
In the polar coordinate system, each point on a plane is determined by a radius \(r\) and an angle \(\theta\). This system is invaluable when working with circular or rotational symmetries, commonly found in nature and various applications in physics and engineering. Understanding polar coordinates allows us to visualize and analyze these curves in a more simplified manner by utilizing the angle and the distance from the center.
Derivative
When dealing with polar equations, such as \(r^2 = 6 \sin 2\theta\), the derivative \(\frac{dr}{d\theta}\) plays a crucial role in determining characteristics like arc length. Derivatives help to find how a quantity changes as another quantity changes, providing insights into the curvature and dynamics of a curve.
In the given example, the derivative \(\frac{dr}{d\theta} = \frac{6\cos 2\theta}{r}\) was obtained through implicit differentiation, which is a method used to differentiate equations where one variable is a function of another. This process is essential for further calculations and understanding how the lemniscate behaves as \(\theta\) changes.
Integral Calculation
The calculation of an integral is a fundamental technique in calculus used to find areas, volumes, central points, and many other important measurements. When trying to find the arc length of the lemniscate \(r^2 = 6 \sin 2\theta\), we use an integral formula to sum up infinitely small pieces of the curve.
The arc length formula in polar coordinates: \[L = \int_{\alpha}^{\beta} \sqrt{\left(\frac{dr}{d\theta}\right)^2 + r^2} d\theta\] allows for the evaluation of the curve's total length between limits \(\alpha\) and \(\beta\). Using symmetry properties, calculations can be simplified. For this problem, the symmetry of the lemniscate allowed us to compute the integral over half of the curve and then double the result to find the total arc length. This simplifies the computation process significantly, yielding an approximate arc length of 9.688 upon evaluation with a calculator.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Alternative derivation of the curvature Derive the computational formula for curvature using the following steps. a. Use the tangential and normal components of the acceleration to show that \(\left.\mathbf{v} \times \mathbf{a}=\kappa|\mathbf{v}|^{3} \mathbf{B} . \text { (Note that } \mathbf{T} \times \mathbf{T}=\mathbf{0} .\right)\) b. Solve the equation in part (a) for \(\kappa\) and conclude that \(\kappa=\frac{|\mathbf{v} \times \mathbf{a}|}{\left|\mathbf{v}^{3}\right|},\) as shown in the text.

Practical formula for \(\mathbf{N}\) Show that the definition of the principal unit normal vector $\mathbf{N}=\frac{d \mathbf{T} / d s}{|d \mathbf{T} / d s|}\( implies the practical formula \)\mathbf{N}=\frac{d \mathbf{T} / d t}{|d \mathbf{T} / d t|} .\( Use the Chain Rule and Note that \)|\mathbf{v}|=d s / d t>0.$

Assume that \(\mathbf{u}, \mathbf{v},\) and \(\mathbf{w}\) are vectors in \(\mathrm{R}^{3}\) that form the sides of a triangle (see figure). Use the following steps to prove that the medians intersect at a point that divides each median in a 2: 1 ratio. The proof does not use a coordinate system. a. Show that \(\mathbf{u}+\mathbf{v}+\mathbf{w}=\mathbf{0}\) b. Let \(\mathbf{M}_{1}\) be the median vector from the midpoint of \(\mathbf{u}\) to the opposite vertex. Define \(\mathbf{M}_{2}\) and \(\mathbf{M}_{3}\) similarly. Using the geometry of vector addition show that \(\mathbf{M}_{1}=\mathbf{u} / 2+\mathbf{v} .\) Find analogous expressions for \(\mathbf{M}_{2}\) and \(\mathbf{M}_{3}\) c. Let \(a, b,\) and \(c\) be the vectors from \(O\) to the points one-third of the way along \(\mathbf{M}_{1}, \mathbf{M}_{2},\) and \(\mathbf{M}_{3},\) respectively. Show that \(\mathbf{a}=\mathbf{b}=\mathbf{c}=(\mathbf{u}-\mathbf{w}) / 3\) d. Conclude that the medians intersect at a point that divides each median in a 2: 1 ratio.

Consider the ellipse \(\mathbf{r}(t)=\langle a \cos t, b \sin t\rangle\) for \(0 \leq t \leq 2 \pi,\) where \(a\) and \(b\) are real numbers. Let \(\theta\) be the angle between the position vector and the \(x\) -axis. a. Show that \(\tan \theta=(b / a) \tan t\) b. Find \(\theta^{\prime}(t)\) c. Note that the area bounded by the polar curve \(r=f(\theta)\) on the interval \([0, \theta]\) is \(A(\theta)=\frac{1}{2} \int_{0}^{\theta}(f(u))^{2} d u\) Letting \(f(\theta(t))=|\mathbf{r}(\theta(t))|,\) show that \(A^{\prime}(t)=\frac{1}{2} a b\) d. Conclude that as an object moves around the ellipse, it sweeps out equal areas in equal times.

A golfer launches a tee shot down a horizontal fairway and it follows a path given by \(\mathbf{r}(t)=\left\langle a t,(75-0.1 a) t,-5 t^{2}+80 t\right\rangle,\) where \(t \geq 0\) measures time in seconds and \(\mathbf{r}\) has units of feet. The \(y\) -axis points straight down the fairway and the z-axis points vertically upward. The parameter \(a\) is the slice factor that determines how much the shot deviates from a straight path down the fairway. a. With no slice \((a=0),\) sketch and describe the shot. How far does the ball travel horizontally (the distance between the point the ball leaves the ground and the point where it first strikes the ground)? b. With a slice \((a=0.2),\) sketch and describe the shot. How far does the ball travel horizontally? c. How far does the ball travel horizontally with \(a=2.5 ?\)

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free