/*! 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 56 Evaluate the following line inte... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Evaluate the following line integrals using a method of your choice. \(\int_{C} x^{3} d x+y^{3} d y,\) where \(C\) is the curve \(\mathbf{r}(t)=\left\langle 1+\sin t, \cos ^{2} t\right\rangle\) for \(0 \leq t \leq \pi / 2\)

Short Answer

Expert verified
The value of the line integral is 47/12.

Step by step solution

01

Determine the derivative of r(t)

First, let's find the derivative of \({\bf r}(t)=\langle 1+\sin t, \cos^2 t\rangle\) with respect to \(t\): \({\bf r}'(t) = \frac{d}{dt} \langle 1+\sin t, \cos^2 t \rangle = \langle \cos t, -2\cos t \sin t \rangle\) Now, we can proceed to the next step.
02

Substitute r(t) and r'(t) into the line integral

Next, we need to substitute the parameterized curve \({\bf r}(t)\) and its derivative \({\bf r}'(t)\) into the line integral: \(\int_{C} x^{3} d x+y^{3} d y = \int_{0}^{\frac{\pi}{2}} [(1+\sin t)^{3}(\cos t) + (\cos^2 t)^{3}(-2\cos t \sin t)] dt\) Now, the expression inside the integral is ready to be integrated.
03

Integrate with respect to t over [0, π/2]

Now, we integrate the expression inside the integral with respect to \(t\), over the interval \([0, \frac{\pi}{2}]\): \(\int_{0}^{\frac{\pi}{2}} [(1+\sin t)^{3}(\cos t) - 2(\cos^4 t)(\sin t \cos t)] dt\) Now, we can use substitution with \(u = 1+\sin t\) and \(v=\cos^2t\). For \(u\), we get \(du=\cos t dt\), so the first part becomes: \(\int u^3du=\int (1+\sin t)^3\cos t dt = \frac{1}{4}u^4=\frac{1}{4}(1+\sin t)^4+C_1\) For \(v\), we get \(dv=-2\sin t \cos t dt\), so the second part becomes: \(\int -2v^2dv=-2\int \cos^4 t \sin t \cos t dt = -\frac{2}{3} v^3 = -\frac{2}{3} \cos^6 t +C_2\) Thus, the overall line integral is: \(\int_{0}^{\frac{\pi}{2}} x^3 dx+y^3dy=\frac{1}{4}(1+\sin t)^4-\frac{2}{3} \cos^6 t +C\) Now, we need to find the definite integral over the interval \([0, \frac{\pi}{2}]\): \(=\left[\frac{1}{4}(1+\sin t)^4\right]_{0}^{\frac{\pi}{2}}-\left[\frac{2}{3} \cos^6 t\right]_{0}^{\frac{\pi}{2}}\) \(= \frac{1}{4}(1+\sin(\frac{\pi}{2}))^4-\frac{2}{3} \cos^6 (\frac{\pi}{2})-\left(\frac{1}{4}(1+\sin(0))^4-\frac{2}{3} \cos^6 (0)\right)\) \(= \frac{1}{4}(2)^4-\frac{2}{3}(0)-\left(\frac{1}{4}(1)^4-\frac{2}{3}(1)\right)\) \(= 4 -\left( \frac{1}{4} - \frac{2}{3}\right)\) \(= 4-\frac{1}{12}\) \(= \frac{47}{12}\) So, the value of the line integral is: \(\int_{C}x^{3}d x+y^{3}d y =\frac{47}{12}\)

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 91Ó°ÊÓ!

Key Concepts

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

Parameterized Curve
To understand line integrals, we need to first grasp the concept of parameterized curves. In mathematics, a parameterized curve in two-dimensional space is a smooth curve defined by a parameter, usually denoted as \( t \). This parameter traces the curve as it takes on values, usually within a given interval.

For example, given \( \mathbf{r}(t) = \langle 1 + \sin t, \cos^2 t \rangle \), \( t \) ranges from \( 0 \) to \( \pi/2 \). This parameterized curve is a vector function that assigns a unique point on the curve for each value of \( t \).

Visualizing parameterized curves can help: imagine the parameter \( t \) as a timer moving through specific positions on a path as time progresses. By applying the parameterized curve to our scenario, we can recognize how it defines the trajectory on which the line integral acts.
Substitution Method
The substitution method is an essential technique in calculus that simplifies the process of finding integrals. Often used with line integrals, substitution involves replacing a variable or expression with another variable or function to make integration easier.

In our case, during the integration process within the line integral calculation, substitution was used:
  • For the first integral portion, we substituted \( u = 1 + \sin t \), resulting in \( du = \cos t \, dt \).
  • For the second part, \( v = \cos^2 t \), giving \( dv = -2 \sin t \cos t \, dt \).
These substitutions transform the integrals into simpler forms that we can evaluate more easily. Essentially, substitution is like changing the lenses on a camera; it clarifies the picture to see the solution more distinctly.
Definite Integral
A definite integral is a concept in calculus that represents the accumulation of quantities, like area under a curve, over a specific interval. Defined by an integral symbol with upper and lower bounds, it evaluates the net area and gives a precise number as a result.

For the line integral problem, once we've expressed the integrand in terms of our parameter, the problem involved calculating a definite integral over the interval \([0, \pi/2]\). Doing so gives a single numeric value that sums up the contributions of the dotted points along this interval.

In practical terms, by evaluating the definite integral, we quantify the entire 'journey' along the parameterized curve, not just individual segments of the path.
Integration by Substitution
Integration by substitution is often likened to the reverse of the chain rule in differentiation. It helps simplify integrals by altering the variable of integration. In the context of solving line integrals, this method proves invaluable when the integrand (the function inside the integral) becomes complex.

By substituting variables \( u \) and \( v \) during the integral steps, we altered the integrands from complex polynomials in sine and cosine to simpler power functions. These transformed expressions allowed us to easily apply elementary integration techniques to obtain the solution.
Integration by substitution systematically unwinds complicated expressions, making them more digestible for calculation, much like unraveling a tangled ball of yarn so you can see each string clearly.

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

Green's Second Identity Prove Green's Second Identity for scalar-valued functions \(u\) and \(v\) defined on a region \(D:\) $$\iiint_{D}\left(u \nabla^{2} v-v \nabla^{2} u\right) d V=\iint_{S}(u \nabla v-v \nabla u) \cdot \mathbf{n} d S$$ (Hint: Reverse the roles of \(u\) and \(v\) in Green's First Identity.)

Special case of surface integrals of scalar-valued functions Suppose a surface \(S\) is defined as \(z=g(x, y)\) on a region \(R\) Show that \(\mathbf{t}_{x} \times \mathbf{t}_{y}=\left\langle-z_{x},-z_{y}, 1\right\rangle\) and that \(\iint_{S} f(x, y, z) d S=\iint_{R} f(x, y, g(x, y)) \sqrt{z_{x}^{2}+z_{y}^{2}+1} d A\)

Conservation of energy Suppose an object with mass \(m\) moves in a region \(R\) in a conservative force field given by \(\mathbf{F}=-\nabla \varphi,\) where \(\varphi\) is a potential function in a region \(R .\) The motion of the object is governed by Newton's Second Law of Motion, \(\mathbf{F}=m \mathbf{a},\) where a is the acceleration. Suppose the object moves from point \(A\) to point \(B\) in \(R\) a. Show that the equation of motion is \(m \frac{d \mathbf{v}}{d t}=-\nabla \varphi\) b. Show that \(\frac{d \mathbf{v}}{d t} \cdot \mathbf{v}=\frac{1}{2} \frac{d}{d t}(\mathbf{v} \cdot \mathbf{v})\) c. Take the dot product of both sides of the equation in part (a) with \(\mathbf{v}(t)=\mathbf{r}^{\prime}(t)\) and integrate along a curve between \(A\) and B. Use part (b) and the fact that \(\mathbf{F}\) is conservative to show that the total energy (kinetic plus potential) \(\frac{1}{2} m|\mathbf{v}|^{2}+\varphi\) is the same at \(A\) and \(B\). Conclude that because \(A\) and \(B\) are arbitrary, energy is conserved in \(R\).

Let \(\mathbf{F}=\langle z, 0,-y\rangle\) a. Find the scalar component of curl \(\mathbf{F}\) in the direction of the unit vector \(\mathbf{n}=\langle 1,0,0\rangle\). b. Find the scalar component of curl \(\mathbf{F}\) in the direction of the unit vector \(\mathbf{n}=\left\langle\frac{1}{\sqrt{3}},-\frac{1}{\sqrt{3}}, \frac{1}{\sqrt{3}}\right\rangle\). c. Find the unit vector \(\mathbf{n}\) that maximizes \(\operatorname{scal}_{\mathbf{n}}\langle-1,1,0\rangle\) and state the value of \(\operatorname{scal}_{\mathbf{n}}\langle-1,1,0\rangle\) in this direction.

Radial fields in \(\mathbb{R}^{3}\) are conservative Prove that the radial field \(\mathbf{F}=\frac{\mathbf{r}}{|\mathbf{r}|^{p}},\) where \(\mathbf{r}=\langle x, y, z\rangle\) and \(p\) is a real number, is conservative on any region not containing the origin. For what values of \(p\) is \(\mathbf{F}\) conservative on a region that contains the origin?

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.