Math Problem Statement

By using Green's theorem, evaluate the curve integral I = ∮C (y^3 dx - 2x^3 dy), where C is the counterclockwise circle x^2 + y^2 = a^2.

Solution

We are tasked with evaluating the line integral I=C(y3dx2x3dy)I = \oint_C \left( y^3 \, dx - 2x^3 \, dy \right), where CC is the counterclockwise circle x2+y2=a2x^2 + y^2 = a^2, by using Green's Theorem.

Step 1: Green's Theorem

Green's theorem relates a line integral around a simple, closed curve CC to a double integral over the region RR enclosed by CC. The theorem states: C(Pdx+Qdy)=R(QxPy)dA\oint_C \left( P \, dx + Q \, dy \right) = \iint_R \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) \, dA For our problem:

  • P(x,y)=y3P(x, y) = y^3
  • Q(x,y)=2x3Q(x, y) = -2x^3

Thus, we need to compute QxPy\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y}.

Step 2: Compute the Partial Derivatives

  • Qx=x(2x3)=6x2\frac{\partial Q}{\partial x} = \frac{\partial}{\partial x} (-2x^3) = -6x^2
  • Py=y(y3)=3y2\frac{\partial P}{\partial y} = \frac{\partial}{\partial y} (y^3) = 3y^2

Thus, Green's theorem reduces the line integral to the double integral: R(6x23y2)dA\iint_R \left( -6x^2 - 3y^2 \right) \, dA This can be rewritten as: R3(2x2+y2)dA\iint_R -3(2x^2 + y^2) \, dA

Step 3: Convert to Polar Coordinates

To evaluate this integral, it is convenient to switch to polar coordinates, where:

  • x=rcos(θ)x = r\cos(\theta)
  • y=rsin(θ)y = r\sin(\theta)
  • dA=rdrdθdA = r \, dr \, d\theta
  • The equation of the circle x2+y2=a2x^2 + y^2 = a^2 becomes r=ar = a, so r[0,a]r \in [0, a] and θ[0,2π]\theta \in [0, 2\pi].

In polar coordinates, we have: 2x2+y2=2r2cos2(θ)+r2sin2(θ)=r2(2cos2(θ)+sin2(θ))=r2(1+cos2(θ))2x^2 + y^2 = 2r^2\cos^2(\theta) + r^2\sin^2(\theta) = r^2(2\cos^2(\theta) + \sin^2(\theta)) = r^2(1 + \cos^2(\theta))

Thus, the integral becomes: I=R3r2(1+cos2(θ))rdrdθ=302π0ar3(1+cos2(θ))drdθI = \iint_R -3r^2(1 + \cos^2(\theta)) \, r \, dr \, d\theta = -3 \int_0^{2\pi} \int_0^a r^3(1 + \cos^2(\theta)) \, dr \, d\theta

Step 4: Perform the Integration

  1. Integrating with respect to rr: 0ar3dr=a44\int_0^a r^3 \, dr = \frac{a^4}{4} Thus, the integral becomes: I=3a4402π(1+cos2(θ))dθI = -3 \cdot \frac{a^4}{4} \int_0^{2\pi} (1 + \cos^2(\theta)) \, d\theta

  2. Now, integrate with respect to θ\theta. Using the hint from the problem, cos2(θ)\cos^2(\theta) has the identity: cos2(θ)=1+cos(2θ)2\cos^2(\theta) = \frac{1 + \cos(2\theta)}{2} Thus: 02π(1+1+cos(2θ)2)dθ=02π32dθ=322π=3π\int_0^{2\pi} \left( 1 + \frac{1 + \cos(2\theta)}{2} \right) \, d\theta = \int_0^{2\pi} \frac{3}{2} \, d\theta = \frac{3}{2} \cdot 2\pi = 3\pi

Step 5: Final Answer

Substituting this result back into the integral: I=3a443π=9πa44I = -3 \cdot \frac{a^4}{4} \cdot 3\pi = -\frac{9\pi a^4}{4}

Thus, the value of the line integral is: I=9πa44I = -\frac{9\pi a^4}{4}

Let me know if you would like additional details or clarifications!

Relative questions:

  1. What is the main application of Green's Theorem in vector calculus?
  2. How do you convert Cartesian coordinates to polar coordinates?
  3. Why is it useful to apply Green's Theorem instead of directly calculating line integrals?
  4. Can you explain how the polar form simplifies integration over circular regions?
  5. What other types of problems can Green's Theorem help solve?

Tip:

When applying Green's Theorem, always check if converting the problem to polar coordinates simplifies the integrals, especially for regions like circles or disks.

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Math Problem Analysis

Mathematical Concepts

Vector Calculus
Green's Theorem
Line Integrals
Polar Coordinates

Formulas

Green's Theorem: ∮C (P dx + Q dy) = ∬R (∂Q/∂x - ∂P/∂y) dA
Polar coordinates transformation: x = rcos(θ), y = rsin(θ), dA = r dr dθ
Integral of cos^2(θ): cos^2(θ) = (1 + cos(2θ)) / 2

Theorems

Green's Theorem

Suitable Grade Level

College/University