Problem 12
Question
Use Green's Theorem to evaluate the indicated line integral. \(\oint_{C} \mathbf{F} \cdot d \mathbf{r},\) where \(\mathbf{F}=\left\langle y^{2}+3 x^{2} y, x y+x^{3}\right\rangle\) and \(C\) is formed by \(y=x^{2}\) and \(y=2 x\)
Step-by-Step Solution
Verified Answer
To evaluate this integral using Green's Theorem, calculate the curl of F, identify the region D, and set up and calculate the double integral of curl F over D.
1Step 1: Express the vector field
The given vector field is \(\mathbf{F}=\left\langle y^{2}+3 x^{2} y, x y+x^{3}\right\rangle.\)
2Step 2: Calculate the curl of F
The curl of F in two dimensions is determined by \(\nabla \times \mathbf{F} = \frac{∂ F_2}{∂x} - \frac{∂ F_1}{∂y}\). Here \(F_1 = y^{2}+3 x^{2} y\) and \(F_2 = x y+x^{3}\). So \(\nabla \times \mathbf{F} = \frac{∂ (x y+x^{3}) }{∂x} - \frac{∂ (y^{2}+3 x^{2} y)}{∂y} = 2x^2 - (2y+3x^2) = 2x^2 - 2y - 3x^2 = -2y -x^2.\)
3Step 3: Identify the region D
The curves \(y=x^2\) and \(y=2x\) bound the region D in the xy-plane. If we sketch these curves, we see the region is bounded by \(x^2 ≤ y ≤ 2x\). For \(x^2 = 2x\), we find the limits of x are 0 and 2.
4Step 4: Set up and calculate the double integral
By Green's Theorem, the integral of curl F over D is equal to the line integral of F over C: \(\oint_{C} \mathbf{F} \cdot d \mathbf{r}= \int \int_D \nabla \times \mathbf{F} \,dA\). Substituting curl of \(\mathbf{F}\) we get: \(\int_{0}^{2} \int_{x^{2}}^{2x} (-2y -x^2) \, dy \, dx.\) Evaluating this double integral gives the final solution.
Key Concepts
Vector FieldLine IntegralDouble IntegralCurl of a Vector Field
Vector Field
In mathematics and physics, a vector field is a construction that assigns a vector to every point in a space. Imagine a flowing stream where every point has a direction and a magnitude, like arrows showing the direction of flow and their intensity.
In our exercise, the vector field is given as \(\mathbf{F}=\langle y^{2}+3 x^{2} y, x y+x^{3}\rangle\). Here, we have two components:
In our exercise, the vector field is given as \(\mathbf{F}=\langle y^{2}+3 x^{2} y, x y+x^{3}\rangle\). Here, we have two components:
- \(y^{2}+3 x^{2} y\) influencing direction along the x-axis
- \(x y+x^{3}\) directing along the y-axis
Line Integral
A line integral is a way to integrate functions along a curve. Think of it as summing up values of some vector field components along a path.
For instance, in the given exercise, the line integral \(\oint_{C} \mathbf{F} \cdot d \mathbf{r}\) is evaluated along the curve \(C\), which is formed by \(y=x^{2}\) and \(y=2x\).
The line integral considers both the path and the function applied over it:
For instance, in the given exercise, the line integral \(\oint_{C} \mathbf{F} \cdot d \mathbf{r}\) is evaluated along the curve \(C\), which is formed by \(y=x^{2}\) and \(y=2x\).
The line integral considers both the path and the function applied over it:
- \(\mathbf{F}\): The vector field function
- \(d \mathbf{r}\): A small segment of the curve
Double Integral
Double integrals extend the concept of integrating a function over a domain in two-dimensional space. It effectively allows us to accumulate values over an area, considering both x and y coordinates.
In Green's Theorem application, instead of calculating a line integral over a path, we calculate a double integral over a region using the curl of a vector field. The bounded region \(D\) in our problem is enclosed by curves \(y=x^2\) and \(y=2x\). We determine the limits of integration within this region by:
In Green's Theorem application, instead of calculating a line integral over a path, we calculate a double integral over a region using the curl of a vector field. The bounded region \(D\) in our problem is enclosed by curves \(y=x^2\) and \(y=2x\). We determine the limits of integration within this region by:
- Knowing the outer curve boundary
- Identifying the intersection points of the curves
Curl of a Vector Field
The concept of the curl of a vector field encompasses understanding how a vector field rotates. In physics, it can be viewed as the swirling strength of the field at a certain point.
Green's Theorem, used in our exercise, involves calculating this curl to convert a line integral into a double integral. The curl in two dimensions is given by \(abla \times \mathbf{F} = \frac{∂ F_2}{∂x} - \frac{∂ F_1}{∂y}\).
From the solution, the curl \(abla \times \mathbf{F}\) simplifies to \(-2y -x^2\). Here's why that matters:
Green's Theorem, used in our exercise, involves calculating this curl to convert a line integral into a double integral. The curl in two dimensions is given by \(abla \times \mathbf{F} = \frac{∂ F_2}{∂x} - \frac{∂ F_1}{∂y}\).
From the solution, the curl \(abla \times \mathbf{F}\) simplifies to \(-2y -x^2\). Here's why that matters:
- Describes the tendency to rotate within a small region of the vector field
- Directly relates to how easily the path integral can be transformed using Green's Theorem
Other exercises in this chapter
Problem 12
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