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Use a line integral on the boundary to find the area of the following regions. The region bounded by the curve \(\mathbf{r}(t)=\left\langle t\left(1-t^{2}\right), 1-t^{2}\right\rangle,\) for \(-1 \leq t \leq 1\) (Hint: Plot the curve.)

Short Answer

Expert verified
Question: Find the area of the region in the plane bounded by the curve \(\mathbf{r}(t)=\langle t(1-t^2), 1-t^2\rangle\) for \(-1\leq t\leq1\). Answer: The area of the region bounded by the given curve is \(\frac{4}{15}\).

Step by step solution

01

Find the parametric equations of the curve

The given curve is $\mathbf{r}(t)=\langle t(1-t^{2}), 1-t^{2}\rangle$. The parametric equations for this curve are: $$x(t)=t(1-t^2)$$ $$y(t)=1-t^2$$
02

Calculate dy/dt and set the limits

Differentiate \(y(t)\) with respect to \(t\) to find \(\frac{dy}{dt}\): $$\frac{dy}{dt}=-2t$$ We will calculate the line integral only for the right half of the region, where \(0 \leq t \leq 1\).
03

Calculate the line integral

To find the area of the region, we need to calculate the line integral \(\oint_C x\, dy\): $$A=\int_{C} x\, dy = \int_{0}^{1} x(t)\cdot\frac{dy}{dt}\, dt$$ Plug in the expressions of \(x(t)\) and \(\frac{dy}{dt}\) we found earlier: $$A=\int_{0}^{1} t(1-t^2)(-2t)\, dt$$
04

Evaluate the integral

To evaluate the integral, first expand the expression inside the integral: $$A=-2\int_{0}^{1} t^2 - 2t^4\, dt$$ Now evaluate the integral by applying the power rule: $$A=-2\left[\frac{1}{3} t^3 -\frac{1}{5} t^5\right]_0^1$$ $$A=-2\left(\frac{1}{3} - \frac{1}{5}\right)$$
05

Account for symmetry

Since the region is symmetric about the y-axis, the total area A is twice the area of the region on the right side where \(0\leq t\leq1\). So, multiply the result by 2: $$A_{total} = 2A=-2\left(-2\left(\frac{1}{3} - \frac{1}{5}\right)\right)$$ $$A_{total} = \frac{4}{3} - \frac{4}{5}$$ $$A_{total} = \frac{12-8}{15}$$
06

Find the area

Now find the total area of the region: $$A_{total} = \frac{4}{15}$$ The area of the region bounded by the given curve is \(\frac{4}{15}\).

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Key Concepts

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

Parametric Equations
When defining curves, especially in the realm of calculus, we often talk in terms of parametric equations. These equations represent a set of points in space, with each coordinate defined as a function of a third variable, typically denoted as t, known as the parameter. The power of parametric equations lies in their ability to describe motion and curves that are not functions or have complex behavior.

For instance, the given exercise requires finding the area within a curve specified by the parametric equations:
  • \(x(t) = t(1-t^2)\)
  • \(y(t) = 1-t^2\)
By plotting these equations, we can visualize the curve in the plane and observe any symmetries or patterns that may simplify our problem. It's essential to note that since the equations are in parametric form, we can capture more complex relationships between x and y—relationships that might be impossible to describe with a single, explicit function y=f(x).
Differentiation
To delve deeper into calculus, differentiation is a fundamental process that allows us to find the rate at which a function changes at any given point. It's the cornerstone of studying motion, change, and optimization problems. In the context of the exercise, differentiation is used to calculate a derivative, which is essential when plugging into the line integral formula.

Here's how differentiation is applied to our problem:
  • We have y(t), and we need its derivative dy/dt.
  • By applying the rules of differentiation, specifically the power rule, we obtain \(\frac{dy}{dt} = -2t\).
This derivative represents the instantaneous rate of change of y with respect to the parameter t. Having this information is crucial because when we compute the line integral to find the area, we'll be integrating x(t) multiplied by this derivative.
Power Rule Integral
The power rule integral is one of the most basic yet powerful tools in calculus for finding antiderivatives of monomial functions. It's essentially the reverse operation of the power rule for differentiation.

To apply the power rule for integration, which is necessary in the final steps of our exercise solution, we follow the pattern:
  • For a term like \(t^n\), the antiderivative is \(\frac{t^{n+1}}{n+1}\), if \(neq -1\).
In our solution, we use the power rule to integrate \(t^2\) and \(t^4\), getting \(\frac{1}{3}t^3\) and \(\frac{1}{5}t^5\) respectively as antiderivatives, leading us to the area of the given region.

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Most popular questions from this chapter

Circulation in a plane \(\mathrm{A}\) circle \(C\) in the plane \(x+y+z=8\) has a radius of 4 and center (2,3,3) . Evaluate \(\oint_{C} \mathbf{F} \cdot d \mathbf{r}\) for \(\mathbf{F}=\langle 0,-z, 2 y\rangle\) where \(C\) has a counterclockwise orientation when viewed from above. Does the circulation depend on the radius of the circle? Does it depend on the location of the center of the circle?

Consider the rotational velocity field \(\mathbf{v}=\langle-2 y, 2 z, 0\rangle\). a. If a paddle wheel is placed in the \(x y\) -plane with its axis normal to this plane, what is its angular speed? b. If a paddle wheel is placed in the \(x z\) -plane with its axis normal to this plane, what is its angular speed? c. If a paddle wheel is placed in the \(y z\) -plane with its axis normal to this plane, what is its angular speed?

The heat flow vector field for conducting objects is \(\mathbf{F}=-k \nabla T,\) where \(T(x, y, z)\) is the temperature in the object and \(k>0\) is a constant that depends on the material. Compute the outward flux of \(\mathbf{F}\) across the following surfaces S for the given temperature distributions. Assume \(k=1\). \(T(x, y, z)=-\ln \left(x^{2}+y^{2}+z^{2}\right) ; S\) is the sphere \(x^{2}+y^{2}+z^{2}=a^{2}\).

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 \(R\)

Suppose a solid object in \(\mathbb{R}^{3}\) has a temperature distribution given by \(T(x, y, z) .\) The heat flow vector field in the object is \(\mathbf{F}=-k \nabla T,\) where the conductivity \(k>0\) is a property of the material. Note that the heat flow vector points in the direction opposite that of the gradient, which is the direction of greatest temperature decrease. The divergence of the heat flow vector is \(\nabla \cdot \mathbf{F}=-k \nabla \cdot \nabla T=-k \nabla^{2} T\) (the Laplacian of \(T\)). Compute the heat flow vector field and its divergence for the following temperature distributions. $$T(x, y, z)=100 e^{-\sqrt{x^{2}+y^{2}+z^{2}}}$$

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