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Use a line integral on the boundary to find the area of the following regions. The region bounded by the parabolas \(\mathbf{r}(t)=\left\langle t, 2 t^{2}\right\rangle\) and \(\mathbf{r}(t)=\left\langle t, 12-t^{2}\right\rangle,\) for \(-2 \leq t \leq 2\)

Short Answer

Expert verified
#Step 4: Interpret the result The result of the area A = 0 means that both parabolic curves meet at the same points for the given range of t (-2 to 2) and there is no enclosed area between them. This indicates that the two curves overlap within this range and don't form a distinct region between them.

Step by step solution

01

Find the derivatives of the parametric equations

First, we need to find the derivatives of both parametric functions. To find the derivative for vector function \(\mathbf{r}(t)\), we differentiate the components individually: $$\mathbf{r}_1'(t) = \frac{d}{dt}\langle t, 2t^2 \rangle = \langle 1, 4t \rangle$$ $$\mathbf{r}_2'(t) = \frac{d}{dt}\langle t, 12 - t^2 \rangle = \langle 1, -2t \rangle$$ These are the derivatives we'll be using in the area formula.
02

Set up the integral for the area

Now that we have the derivatives, we can set up the integral to find the area A: $$A = \frac{1}{2} \int_{-2}^2\left(\mathbf{r}_1(t) \cdot \mathbf{r}_2'(t) - \mathbf{r}_2(t) \cdot \mathbf{r}_1'(t)\right) dt$$ Plug in our expressions for \(\mathbf{r}_1(t)\), \(\mathbf{r}_2(t)\), \(\mathbf{r}_1'(t)\), and \(\mathbf{r}_2'(t)\): $$A = \frac{1}{2} \int_{-2}^2\left(\langle t, 2t^2 \rangle \cdot \langle 1, -2t \rangle - \langle t, 12 - t^2 \rangle \cdot \langle 1, 4t \rangle\right) dt$$ Now, we can compute the dot products: $$A = \frac{1}{2} \int_{-2}^2\left( t - 4t^3 - (t + 4t(12 - t^2))\right) dt$$ This becomes: $$A = \frac{1}{2} \int_{-2}^2\left(-4t^3 - t - 4t + 4t^3\right) dt$$ Simplifying the integrand gives us: $$A = \frac{1}{2} \int_{-2}^2\left(- 5t\right) dt$$
03

Evaluate the integral

Now, we can evaluate the integral: $$A = \frac{1}{2} \int_{-2}^2 -5t dt = -\frac{5}{2} \int_{-2}^2 t dt$$ The integral is: $$-\frac{5}{2}\left[\frac{1}{2}t^2\right]_{-2}^2$$ Evaluate the antiderivative at the bounds: $$-\frac{5}{2}\left[\frac{1}{2}(2^2) - \frac{1}{2}(-2)^2\right]$$ Which simplifies to: $$A = -\frac{5}{2}(0) = 0$$ So, the area between the two parabolas is 0. It means that both parabolas meet at the same points and there is no area enclosed between them for the given range of t.

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Key Concepts

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

Parametric Equations Derivatives
In vector calculus, a parametric equation represents a set of related quantities as dependent variables with one or more independent variables. When we talk about derivatives of parametric equations, it means taking the derivative of these dependent variables with respect to the independent variable. This process specifies how a point on a curve changes position as the parameter alters.

For example, consider the parametric equations \( t, 2t^2 \) and \( t, 12-t^2 \). To find the rate at which their corresponding y-values change, we compute the derivative of each component with respect to t. The derivatives \(1, 4t\) and \(1, -2t\) give us the velocity vectors of the points on the curves at any instant t. In the context of the area calculation, these derivatives become crucial as they help in setting up the correct integral for determining the area bounded between two paths.
Area Calculation Using Integrals
Calculating area using integrals is a fundamental concept in calculus. When we have a function or curve, the definite integral can be thought of as the accumulation of small slices of area under the curve from one point to another. In the scenario of parametric equations, the technique modifies slightly. We must consider the directional components — how much in the x-direction and how much in the y-direction — as we move along our path.

For the area between two curves described by parametric equations, one might typically subtract one curve from the other. However, in vector calculus, the concept extends to line integrals, which provide a means to calculate the area enclosed by a curve directly. This method leverages the cross product or dot product of derivatives of parametric equations and requires evaluating an integral set up with precise limits that correspond to the interval of the parameter.
Dot Product in Vector Calculus
In vector calculus, the dot product (also known as the scalar product) measures the magnitude of the projection of one vector onto another. It is a way to multiply two vectors to get a scalar, or single number, as a result. This operation is essential in many applications, including finding the angle between two vectors and determining when two vectors are perpendicular.

The dot product is defined algebraically as the sum of the products of the corresponding entries of two sequences of numbers. For vectors \(\mathbf{a}\) and \(\mathbf{b}\), their dot product is \(\mathbf{a} \cdot \mathbf{b} = a_{1}b_{1} + a_{2}b_{2} + ... + a_{n}b_{n}\). This concept is instrumental in our area problem, where we compute the dot product of the derivatives of two parametric curves to construct the integral for area calculation.
Evaluating Definite Integrals
Evaluating definite integrals is the process of calculating the exact value of an integral within certain limits. A definite integral has upper and lower bounds, which are the limits of integration, and represents the net area between the function and the x-axis within these bounds.

To evaluate a definite integral, one typically finds the indefinite integral (antiderivative) first, then applies the Fundamental Theorem of Calculus by subtracting the antiderivative evaluated at the lower limit from the antiderivative evaluated at the upper limit. In the given exercise, evaluating the integral from -2 to 2 for the function \( -5t \) leads to calculating the net area between two curves over this interval. The result of zero indicates that the curves intersect each other in such a manner that no net area is enclosed between them for the specified range of t.

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Most popular questions from this chapter

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. $$T(x, y, z)=100 e^{-x^{2}+y^{2}+z^{2}}$$

Find the work required to move an object in the following force fields along a line segment between the given points. Check to see whether the force is conservative. $$\mathbf{F}=e^{x+y}\langle 1,1, z\rangle \text { from } A(0,0,0) \text { to } B(-1,2,-4)$$

Consider the radial field \(\mathbf{F}=\frac{\mathbf{r}}{|\mathbf{r}|^{p}}=\frac{\langle x, y, z\rangle}{|\mathbf{r}|^{p}},\) where \(p>1\) (the inverse square law corresponds to \(p=3\) ). Let \(C\) be the line from (1,1,1) to \((a, a, a),\) where \(a>1,\) given by \(\mathbf{r}(t)=\langle t, t, t\rangle,\) for \(1 \leq t \leq a\) a. Find the work done in moving an object along \(C\) with \(p=2\) b. If \(a \rightarrow \infty\) in part (a), is the work finite? c. Find the work done in moving an object moving along \(C\) with \(p=4.\) d. If \(a \rightarrow \infty\) in part (c), is the work finite? e. Find the work done in moving an object moving along \(C\) for any \(p>1\) f. If \(a \rightarrow \infty\) in part (e), for what values of \(p\) is the work finite?

The area of a region \(R\) in the plane, whose boundary is the closed curve \(C,\) may be computed using line integrals with the formula $$\text { area of } R=\int_{C} x d y=-\int_{C} y d x$$ These ideas reappear later in the chapter. Let \(R=\\{(r, \theta): 0 \leq r \leq a, 0 \leq \theta \leq 2 \pi\\}\) be the disk of radius \(a\) centered at the origin and let \(C\) be the boundary of \(R\) oriented counterclockwise. Use the formula \(A=-\int_{C} y d x\) to verify that the area of the disk is \(\pi r^{2}.\)

A square plate \(R=\\{(x, y): 0 \leq x \leq 1,\) \(0 \leq y \leq 1\\}\) has a temperature distribution \(T(x, y)=100-50 x-25 y\) a. Sketch two level curves of the temperature in the plate. b. Find the gradient of the temperature \(\nabla T(x, y)\) c. Assume that the flow of heat is given by the vector field \(\mathbf{F}=-\nabla T(x, y) .\) Compute \(\mathbf{F}\) d. Find the outward heat flux across the boundary \(\\{(x, y): x=1,0 \leq y \leq 1\\}\) e. Find the outward heat flux across the boundary \(\\{(x, y): 0 \leq x \leq 1, y=1\\}\)

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