MATH 2010 Exam 2 Review Problems

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Overview

Exam #2 will be administered in Test Block on Wednesday, March 11 and will cover all Multivariable Calculus content. There will be a greater emphasis on material covered after Exam 1 (sections 15.1, 15.2, 15.3, 15.4, 16.1, 16.2, 16.3, and 17.1), but you should be prepared to answer questions from any of the sections covered on Exam 1 (sections 14.3, 14.4, 14.5, 14.6, 14.7, and 14.8)

If you submitted a ANSS memo with accommodations for exams, you will be contacted via email with details regarding the alternate location of your exam. Only students who have emailed the instructor their accommodations memorandum by Monday 3/9 at 5PM will be able to use their testing accommodations on Exam 2.

You will have 70 minutes to complete the exam. Students must arrive on time and listen to instructions regarding seating requirements. Students must leave all belongings (backpacks, jackets, and phones) in the front of the exam room up against the wall. Do not block any exits or obstruct any walkways. You will not be granted any additional time to complete your exam if you arrive after the exam has begun. Students will be required to sign in and collected exams will be cross-checked with the sign-in sheets. Exams from students who do not sign in will not be graded.

Questions

Q1. Integration in Two Variables

Evaluate ∬Dxy dA\iint_D xy \, dA where DD is the region bounded by the curves y=xy=x and y=xy=\sqrt{x}.

Answer of This Question

To evaluate the double integral ∬Dxy dA\iint_D xy \, dA, we first need to determine the region of integration DD and set up the iterated integral.

1. Determine the Region DD

The region DD is bounded by the curves y=xy = x and y=xy = \sqrt{x}. To find the intersection points of these curves, we set the equations equal to each other:

x=x x = \sqrt{x}

Squaring both sides gives:

x2=x  ⟹  x2−x=0  ⟹  x(x−1)=0 x^2 = x \implies x^2 - x = 0 \implies x(x - 1) = 0

Thus, the intersection points occur at x=0x = 0 and x=1x = 1. The corresponding yy-values are y=0y=0 and y=1y=1, giving the points (0,0)(0,0) and (1,1)(1,1).

On the interval 0<x<10 < x < 1, we have x>x\sqrt{x} > x. Therefore, the region DD can be described as:

D={(x,y)∣0≤x≤1, x≤y≤x} D = \{ (x, y) \mid 0 \le x \le 1, \, x \le y \le \sqrt{x} \}

2. Set Up the Integral

We can express the double integral as an iterated integral integrating with respect to yy first, then xx:

∬Dxy dA=∫01∫xxxy dy dx \iint_D xy \, dA = \int_0^1 \int_x^{\sqrt{x}} xy \, dy \, dx

3. Evaluate the Inner Integral

First, we integrate with respect to yy, treating xx as a constant:

∫xxxy dy=x[y22]y=xy=x \int_x^{\sqrt{x}} xy \, dy = x \left[ \frac{y^2}{2} \right]_{y=x}^{y=\sqrt{x}}

Substituting the limits of integration:

=x((x)22−x22)=x(x2−x22)=x22−x32 = x \left( \frac{(\sqrt{x})^2}{2} - \frac{x^2}{2} \right) = x \left( \frac{x}{2} - \frac{x^2}{2} \right) = \frac{x^2}{2} - \frac{x^3}{2}

4. Evaluate the Outer Integral

Now, we integrate the result with respect to xx from 00 to 11:

∫01(x22−x32)dx=[x36−x48]01 \int_0^1 \left( \frac{x^2}{2} - \frac{x^3}{2} \right) dx = \left[ \frac{x^3}{6} - \frac{x^4}{8} \right]_0^1

Evaluating at the boundaries:

=(136−148)−(0−0)=16−18 = \left( \frac{1^3}{6} - \frac{1^4}{8} \right) - (0 - 0) = \frac{1}{6} - \frac{1}{8}

Finding a common denominator:

=424−324=124 = \frac{4}{24} - \frac{3}{24} = \frac{1}{24}

Final Answer

∬Dxy dA=124 \iint_D xy \, dA = \frac{1}{24}

Q2. Integration in Polar Coordinates

Compute the integral ∬D(x2+y2) dA\iint_D (x^2+y^2) \, dA using polar coordinates, where DD is the region bounded between the circles x2+y2=4x^2+y^2=4, x2+y2=9x^2+y^2=9 and x≥0,y≥0x \ge 0, y \ge 0.

Answer of This Question

To compute the integral ∬D(x2+y2) dA\iint_D (x^2+y^2) \, dA using polar coordinates, we proceed with the following steps.

1. Coordinate Transformation We convert from Cartesian coordinates (x,y)(x, y) to polar coordinates (r,θ)(r, \theta) using the relations:

x=rcos⁡θ,y=rsin⁡θ x = r \cos \theta, \quad y = r \sin \theta

Consequently, the term x2+y2x^2 + y^2 becomes r2r^2, and the area element dAdA becomes r dr dθr \, dr \, d\theta.

2. Determine the Region of Integration The region DD is bounded by the circles x2+y2=4x^2+y^2=4 and x2+y2=9x^2+y^2=9, with the constraints x≥0x \ge 0 and y≥0y \ge 0.

  • The equations of the circles translate to r2=4  ⟹  r=2r^2 = 4 \implies r = 2 and r2=9  ⟹  r=3r^2 = 9 \implies r = 3. Thus, the radial bounds are 2≤r≤32 \le r \le 3.
  • The constraints x≥0x \ge 0 and y≥0y \ge 0 restrict the region to the first quadrant, which corresponds to 0≤θ≤π20 \le \theta \le \frac{\pi}{2}.

So, the region DD in polar coordinates is defined as:

D={(r,θ)∣2≤r≤3, 0≤θ≤π2} D = \left\{ (r, \theta) \mid 2 \le r \le 3, \, 0 \le \theta \le \frac{\pi}{2} \right\}

3. Set Up the Integral Substituting the integrand and the differential element into the double integral:

∬D(x2+y2) dA=∫0π/2∫23(r2)⋅r dr dθ=∫0π/2∫23r3 dr dθ \iint_D (x^2+y^2) \, dA = \int_0^{\pi/2} \int_2^3 (r^2) \cdot r \, dr \, d\theta = \int_0^{\pi/2} \int_2^3 r^3 \, dr \, d\theta

4. Evaluate the Integral First, we evaluate the inner integral with respect to rr:

∫23r3 dr=[r44]23=344−244=814−164=654 \int_2^3 r^3 \, dr = \left[ \frac{r^4}{4} \right]_2^3 = \frac{3^4}{4} - \frac{2^4}{4} = \frac{81}{4} - \frac{16}{4} = \frac{65}{4}

Next, we evaluate the outer integral with respect to θ\theta:

∫0π/2654 dθ=654[θ]0π/2=654(π2−0)=65π8 \int_0^{\pi/2} \frac{65}{4} \, d\theta = \frac{65}{4} \Big[ \theta \Big]_0^{\pi/2} = \frac{65}{4} \left( \frac{\pi}{2} - 0 \right) = \frac{65\pi}{8}

Final Answer

∬D(x2+y2) dA=65π8 \iint_D (x^2+y^2) \, dA = \frac{65\pi}{8}

Q3. Integration in Polar Coordinates

Calculate the integral of f(x,y)=(x2+y2)−3/2f(x,y) = (x^2+y^2)^{-3/2} over the region DD given by x2+y2≤16,x+y≥4x^2+y^2 \le 16, x+y \ge 4 by changing to polar coordinates.

Answer of This Question

To calculate the integral of f(x,y)=(x2+y2)−3/2f(x,y) = (x^2+y^2)^{-3/2} over the region DD using polar coordinates, we proceed as follows.

1. Understand the Region DD

The region DD is defined by two conditions:

  • x2+y2≤16x^2+y^2 \le 16: This is a disk of radius 4 centered at the origin.
  • x+y≥4x+y \ge 4: This is the half-plane above the line x+y=4x+y=4.

The region DD is the portion of the disk that lies above the line x+y=4x+y=4.

2. Find Intersection Points

To find where the line x+y=4x+y=4 intersects the circle x2+y2=16x^2+y^2=16, we substitute y=4−xy = 4-x into the circle equation:

x2+(4−x)2=16 x^2 + (4-x)^2 = 16

x2+16−8x+x2=16 x^2 + 16 - 8x + x^2 = 16

2x2−8x=0  ⟹  2x(x−4)=0 2x^2 - 8x = 0 \implies 2x(x-4) = 0

Thus, x=0x = 0 or x=4x = 4. The intersection points are (0,4)(0, 4) and (4,0)(4, 0).

3. Convert to Polar Coordinates

Using polar coordinates:

  • x=rcos⁡θx = r \cos \theta
  • y=rsin⁡θy = r \sin \theta
  • x2+y2=r2x^2 + y^2 = r^2
  • dA=r dr dθdA = r \, dr \, d\theta

The integrand becomes:

(x2+y2)−3/2=(r2)−3/2=r−3 (x^2+y^2)^{-3/2} = (r^2)^{-3/2} = r^{-3}

4. Determine the Bounds

  • Radial bounds: From the line x+y=4x+y=4, we have r(cos⁡θ+sin⁡θ)=4r(\cos\theta + \sin\theta) = 4, so r=4cos⁡θ+sin⁡θr = \frac{4}{\cos\theta + \sin\theta}. From the circle, r=4r = 4. Thus, 4cos⁡θ+sin⁡θ≤r≤4\frac{4}{\cos\theta + \sin\theta} \le r \le 4.
  • Angular bounds: The intersection points (4,0)(4, 0) and (0,4)(0, 4) correspond to θ=0\theta = 0 and θ=π2\theta = \frac{\pi}{2} respectively. Thus, 0≤θ≤π20 \le \theta \le \frac{\pi}{2}.

5. Set Up the Integral

∬D(x2+y2)−3/2 dA=∫0π/2∫4cos⁡θ+sin⁡θ4r−3⋅r dr dθ \iint_D (x^2+y^2)^{-3/2} \, dA = \int_0^{\pi/2} \int_{\frac{4}{\cos\theta + \sin\theta}}^4 r^{-3} \cdot r \, dr \, d\theta

=∫0π/2∫4cos⁡θ+sin⁡θ4r−2 dr dθ = \int_0^{\pi/2} \int_{\frac{4}{\cos\theta + \sin\theta}}^4 r^{-2} \, dr \, d\theta

6. Evaluate the Inner Integral

∫4cos⁡θ+sin⁡θ4r−2 dr=[−1r]4cos⁡θ+sin⁡θ4 \int_{\frac{4}{\cos\theta + \sin\theta}}^4 r^{-2} \, dr = \left[ -\frac{1}{r} \right]_{\frac{4}{\cos\theta + \sin\theta}}^4

=−14−(−cos⁡θ+sin⁡θ4)=cos⁡θ+sin⁡θ−14 = -\frac{1}{4} - \left( -\frac{\cos\theta + \sin\theta}{4} \right) = \frac{\cos\theta + \sin\theta - 1}{4}

7. Evaluate the Outer Integral

∫0π/2cos⁡θ+sin⁡θ−14 dθ=14∫0π/2(cos⁡θ+sin⁡θ−1) dθ \int_0^{\pi/2} \frac{\cos\theta + \sin\theta - 1}{4} \, d\theta = \frac{1}{4} \int_0^{\pi/2} (\cos\theta + \sin\theta - 1) \, d\theta

=14[sin⁡θ−cos⁡θ−θ]0π/2 = \frac{1}{4} \left[ \sin\theta - \cos\theta - \theta \right]_0^{\pi/2}

=14[(sin⁡π2−cos⁡π2−π2)−(sin⁡0−cos⁡0−0)] = \frac{1}{4} \left[ \left( \sin\frac{\pi}{2} - \cos\frac{\pi}{2} - \frac{\pi}{2} \right) - \left( \sin 0 - \cos 0 - 0 \right) \right]

=14[(1−0−π2)−(0−1−0)] = \frac{1}{4} \left[ (1 - 0 - \frac{\pi}{2}) - (0 - 1 - 0) \right]

=14[1−π2+1]=14[2−π2] = \frac{1}{4} \left[ 1 - \frac{\pi}{2} + 1 \right] = \frac{1}{4} \left[ 2 - \frac{\pi}{2} \right]

=12−π8 = \frac{1}{2} - \frac{\pi}{8}

Final Answer

∬D(x2+y2)−3/2 dA=12−π8 \iint_D (x^2+y^2)^{-3/2} \, dA = \frac{1}{2} - \frac{\pi}{8}

Q4. Triple Integrals

Evaluate ∭B(xz+yz2) dV\iiint_B (xz + yz^2) \, dV, where B=[0,1]×[2,4]×[0,2]B = [0,1] \times [2,4] \times [0,2].

Answer of This Question

To evaluate the triple integral ∭B(xz+yz2) dV\iiint_B (xz + yz^2) \, dV, where B=[0,1]×[2,4]×[0,2]B = [0,1] \times [2,4] \times [0,2], we set up the iterated integral based on the bounds of the rectangular box BB.

1. Set Up the Integral

The region BB is defined by the inequalities:

0≤x≤1,2≤y≤4,0≤z≤2 0 \le x \le 1, \quad 2 \le y \le 4, \quad 0 \le z \le 2

We can write the triple integral as an iterated integral. The order of integration does not matter for a rectangular box, but we will integrate with respect to zz, then yy, then xx:

∭B(xz+yz2) dV=∫01∫24∫02(xz+yz2) dz dy dx \iiint_B (xz + yz^2) \, dV = \int_0^1 \int_2^4 \int_0^2 (xz + yz^2) \, dz \, dy \, dx

2. Evaluate the Inner Integral (with respect to zz)

First, we integrate with respect to zz, treating xx and yy as constants:

∫02(xz+yz2) dz=[xz22+yz33]z=0z=2 \int_0^2 (xz + yz^2) \, dz = \left[ x \frac{z^2}{2} + y \frac{z^3}{3} \right]_{z=0}^{z=2}

Substituting the limits z=2z=2 and z=0z=0:

=(x222+y233)−0=2x+8y3 = \left( x \frac{2^2}{2} + y \frac{2^3}{3} \right) - 0 = 2x + \frac{8y}{3}

3. Evaluate the Middle Integral (with respect to yy)

Next, we integrate the result with respect to yy from 22 to 44, treating xx as a constant:

∫24(2x+8y3) dy=[2xy+83⋅y22]y=2y=4 \int_2^4 \left( 2x + \frac{8y}{3} \right) \, dy = \left[ 2xy + \frac{8}{3} \cdot \frac{y^2}{2} \right]_{y=2}^{y=4}

Simplifying the term with y2y^2:

=[2xy+4y23]y=2y=4 = \left[ 2xy + \frac{4y^2}{3} \right]_{y=2}^{y=4}

Evaluating at the boundaries:

=(2x(4)+4(4)23)−(2x(2)+4(2)23) = \left( 2x(4) + \frac{4(4)^2}{3} \right) - \left( 2x(2) + \frac{4(2)^2}{3} \right)

=(8x+643)−(4x+163) = \left( 8x + \frac{64}{3} \right) - \left( 4x + \frac{16}{3} \right)

=4x+483=4x+16 = 4x + \frac{48}{3} = 4x + 16

4. Evaluate the Outer Integral (with respect to xx)

Finally, we integrate with respect to xx from 00 to 11:

∫01(4x+16) dx=[2x2+16x]01 \int_0^1 (4x + 16) \, dx = \left[ 2x^2 + 16x \right]_0^1

Evaluating at the boundaries:

=(2(1)2+16(1))−0=2+16=18 = (2(1)^2 + 16(1)) - 0 = 2 + 16 = 18

Final Answer

∭B(xz+yz2) dV=18 \iiint_B (xz + yz^2) \, dV = 18

Q5. Triple Integrals

Evaluate ∭W66z dV\iiint_W 66z \, dV where W:x2≤y≤1,0≤x≤1,x−y≤z≤x+yW: x^2 \le y \le 1, 0 \le x \le 1, x-y \le z \le x+y

Answer of This Question

To evaluate the triple integral ∭W66z dV\iiint_W 66z \, dV over the region WW, we first need to determine the limits of integration based on the given inequalities.

1. Determine the Region of Integration

The region WW is defined by:

  • 0≤x≤10 \le x \le 1
  • x2≤y≤1x^2 \le y \le 1
  • x−y≤z≤x+yx-y \le z \le x+y

We can set up the iterated integral in the order dz dy dxdz \, dy \, dx:

∭W66z dV=∫01∫x21∫x−yx+y66z dz dy dx \iiint_W 66z \, dV = \int_0^1 \int_{x^2}^1 \int_{x-y}^{x+y} 66z \, dz \, dy \, dx

2. Evaluate the Inner Integral (with respect to zz)

First, we integrate with respect to zz, treating xx and yy as constants:

∫x−yx+y66z dz=66[z22]x−yx+y=33[z2]x−yx+y \int_{x-y}^{x+y} 66z \, dz = 66 \left[ \frac{z^2}{2} \right]_{x-y}^{x+y} = 33 \left[ z^2 \right]_{x-y}^{x+y}

Substituting the limits:

=33((x+y)2−(x−y)2) = 33 \left( (x+y)^2 - (x-y)^2 \right)

Using the identity (a+b)2−(a−b)2=4ab(a+b)^2 - (a-b)^2 = 4ab, where a=xa=x and b=yb=y:

=33(4xy)=132xy = 33 (4xy) = 132xy

3. Evaluate the Middle Integral (with respect to yy)

Now, we integrate the result with respect to yy from x2x^2 to 11, treating xx as a constant:

∫x21132xy dy=132x∫x21y dy \int_{x^2}^1 132xy \, dy = 132x \int_{x^2}^1 y \, dy

=132x[y22]x21=132x(122−(x2)22) = 132x \left[ \frac{y^2}{2} \right]_{x^2}^1 = 132x \left( \frac{1^2}{2} - \frac{(x^2)^2}{2} \right)

=132x(12−x42)=66x(1−x4)=66x−66x5 = 132x \left( \frac{1}{2} - \frac{x^4}{2} \right) = 66x (1 - x^4) = 66x - 66x^5

4. Evaluate the Outer Integral (with respect to xx)

Finally, we integrate with respect to xx from 00 to 11:

∫01(66x−66x5) dx=66∫01(x−x5) dx \int_0^1 (66x - 66x^5) \, dx = 66 \int_0^1 (x - x^5) \, dx

=66[x22−x66]01 = 66 \left[ \frac{x^2}{2} - \frac{x^6}{6} \right]_0^1

Evaluating at the boundaries:

=66((12−16)−0) = 66 \left( \left( \frac{1}{2} - \frac{1}{6} \right) - 0 \right)

Finding a common denominator for the fractions:

=66(36−16)=66(26)=66(13)=22 = 66 \left( \frac{3}{6} - \frac{1}{6} \right) = 66 \left( \frac{2}{6} \right) = 66 \left( \frac{1}{3} \right) = 22

Final Answer

∭W66z dV=22 \iiint_W 66z \, dV = 22

Q6. Vector Fields

Find div(F⃗)\text{div}(\vec{F}) and curl(F⃗)\text{curl}(\vec{F}) if F⃗=⟨xy,e2y+3z,x2+z2⟩\vec{F} = \langle xy, e^{2y+3z}, x^2+z^2 \rangle.

Answer of This Question

Let the vector field be F⃗=⟨P,Q,R⟩\vec{F} = \langle P, Q, R \rangle, where:

P=xy,Q=e2y+3z,R=x2+z2 P = xy, \quad Q = e^{2y+3z}, \quad R = x^2+z^2

1. Calculate the Divergence

The divergence of F⃗\vec{F} is given by the dot product of the del operator ∇\nabla and the vector field F⃗\vec{F}:

div(F⃗)=∇⋅F⃗=∂P∂x+∂Q∂y+∂R∂z \text{div}(\vec{F}) = \nabla \cdot \vec{F} = \frac{\partial P}{\partial x} + \frac{\partial Q}{\partial y} + \frac{\partial R}{\partial z}

We compute the partial derivatives:

∂P∂x=∂∂x(xy)=y \frac{\partial P}{\partial x} = \frac{\partial}{\partial x}(xy) = y

∂Q∂y=∂∂y(e2y+3z)=2e2y+3z \frac{\partial Q}{\partial y} = \frac{\partial}{\partial y}(e^{2y+3z}) = 2e^{2y+3z}

∂R∂z=∂∂z(x2+z2)=2z \frac{\partial R}{\partial z} = \frac{\partial}{\partial z}(x^2+z^2) = 2z

Adding these together, we get:

div(F⃗)=y+2e2y+3z+2z \text{div}(\vec{F}) = y + 2e^{2y+3z} + 2z

2. Calculate the Curl

The curl of F⃗\vec{F} is given by the cross product of the del operator ∇\nabla and the vector field F⃗\vec{F}:

curl(F⃗)=∇×F⃗=∣ijk∂∂x∂∂y∂∂zPQR∣ \text{curl}(\vec{F}) = \nabla \times \vec{F} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\ P & Q & R \end{vmatrix}

=⟨∂R∂y−∂Q∂z,∂P∂z−∂R∂x,∂Q∂x−∂P∂y⟩ = \left\langle \frac{\partial R}{\partial y} - \frac{\partial Q}{\partial z}, \frac{\partial P}{\partial z} - \frac{\partial R}{\partial x}, \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right\rangle

We compute the necessary partial derivatives:

  • For the i\mathbf{i}-component: ∂R∂y=0,∂Q∂z=3e2y+3z  ⟹  0−3e2y+3z=−3e2y+3z \frac{\partial R}{\partial y} = 0, \quad \frac{\partial Q}{\partial z} = 3e^{2y+3z} \implies 0 - 3e^{2y+3z} = -3e^{2y+3z}
  • For the j\mathbf{j}-component: ∂P∂z=0,∂R∂x=2x  ⟹  0−2x=−2x \frac{\partial P}{\partial z} = 0, \quad \frac{\partial R}{\partial x} = 2x \implies 0 - 2x = -2x
  • For the k\mathbf{k}-component: ∂Q∂x=0,∂P∂y=x  ⟹  0−x=−x \frac{\partial Q}{\partial x} = 0, \quad \frac{\partial P}{\partial y} = x \implies 0 - x = -x

Thus, the curl is:

curl(F⃗)=⟨−3e2y+3z,−2x,−x⟩ \text{curl}(\vec{F}) = \langle -3e^{2y+3z}, -2x, -x \rangle

Final Answer

div(F⃗)=y+2e2y+3z+2z \text{div}(\vec{F}) = y + 2e^{2y+3z} + 2z

curl(F⃗)=⟨−3e2y+3z,−2x,−x⟩ \text{curl}(\vec{F}) = \langle -3e^{2y+3z}, -2x, -x \rangle

Q7. Scalar Line Integrals

Evaluate ∫C1+36xy ds\int_C \sqrt{1+36xy} \, ds where CC is the curve y=4x3y=4x^3 from (0,0)(0,0) to (1,4)(1,4).

Answer of This Question

To evaluate the line integral ∫C1+36xy ds\int_C \sqrt{1+36xy} \, ds, we need to parametrize the curve CC, determine the arc length element dsds, and then compute the definite integral.

1. Parametrize the Curve CC

The curve CC is given by the function y=4x3y = 4x^3 from the point (0,0)(0,0) to (1,4)(1,4). We can use xx as the parameter.
Let x=tx = t. Then y=4t3y = 4t^3.
The range for xx is from 00 to 11, so the parameter tt ranges from 00 to 11.

r⃗(t)=⟨t,4t3⟩,0≤t≤1 \vec{r}(t) = \langle t, 4t^3 \rangle, \quad 0 \le t \le 1

2. Calculate the Arc Length Element dsds

The differential arc length dsds is given by:

ds=(dxdt)2+(dydt)2 dt ds = \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2} \, dt

First, compute the derivatives with respect to tt:

dxdt=1,dydt=12t2 \frac{dx}{dt} = 1, \quad \frac{dy}{dt} = 12t^2

Substitute these into the formula for dsds:

ds=(1)2+(12t2)2 dt=1+144t4 dt ds = \sqrt{(1)^2 + (12t^2)^2} \, dt = \sqrt{1 + 144t^4} \, dt

3. Express the Integrand in Terms of tt

The integrand is f(x,y)=1+36xyf(x,y) = \sqrt{1+36xy}. Substitute x=tx=t and y=4t3y=4t^3:

1+36(t)(4t3)=1+144t4 \sqrt{1+36(t)(4t^3)} = \sqrt{1 + 144t^4}

4. Set Up and Evaluate the Integral

Now, substitute the integrand and dsds into the line integral:

∫C1+36xy ds=∫011+144t4⋅1+144t4 dt \int_C \sqrt{1+36xy} \, ds = \int_0^1 \sqrt{1 + 144t^4} \cdot \sqrt{1 + 144t^4} \, dt

The two square root terms multiply to form the expression inside the root:

=∫01(1+144t4) dt = \int_0^1 (1 + 144t^4) \, dt

Now, evaluate the definite integral:

=[t+144t55]01 = \left[ t + 144 \frac{t^5}{5} \right]_0^1

=(1+1445)−(0+0) = \left( 1 + \frac{144}{5} \right) - (0 + 0)

=55+1445=1495 = \frac{5}{5} + \frac{144}{5} = \frac{149}{5}

Final Answer

∫C1+36xy ds=1495 \int_C \sqrt{1+36xy} \, ds = \frac{149}{5}

Q8. Vector Line Integrals

Compute ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r} if F⃗=⟨xy,3,z3⟩\vec{F} = \langle xy, 3, z^3 \rangle and CC is the curve parameterized by r⃗(t)=⟨cos⁡t,sin⁡t,t⟩\vec{r}(t) = \langle \cos t, \sin t, t \rangle for 0≤t≤π0 \le t \le \pi.
Note: F⃗\vec{F} is not conservative. How do you know?

Answer of This Question

To address the note first, we determine if the vector field F⃗\vec{F} is conservative by calculating its curl.

1. Is F⃗\vec{F} Conservative?

A vector field F⃗=⟨P,Q,R⟩\vec{F} = \langle P, Q, R \rangle is conservative if and only if curl(F⃗)=0⃗\text{curl}(\vec{F}) = \vec{0} (assuming the domain is simply connected).
Given F⃗=⟨xy,3,z3⟩\vec{F} = \langle xy, 3, z^3 \rangle, we have P=xyP = xy, Q=3Q = 3, and R=z3R = z^3.
The curl is given by:

curl(F⃗)=∇×F⃗=⟨∂R∂y−∂Q∂z,∂P∂z−∂R∂x,∂Q∂x−∂P∂y⟩ \text{curl}(\vec{F}) = \nabla \times \vec{F} = \left\langle \frac{\partial R}{\partial y} - \frac{\partial Q}{\partial z}, \frac{\partial P}{\partial z} - \frac{\partial R}{\partial x}, \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right\rangle

Calculating the components:

  • ∂R∂y−∂Q∂z=0−0=0\frac{\partial R}{\partial y} - \frac{\partial Q}{\partial z} = 0 - 0 = 0
  • ∂P∂z−∂R∂x=0−0=0\frac{\partial P}{\partial z} - \frac{\partial R}{\partial x} = 0 - 0 = 0
  • ∂Q∂x−∂P∂y=0−x=−x\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 0 - x = -x

Thus,

curl(F⃗)=⟨0,0,−x⟩ \text{curl}(\vec{F}) = \langle 0, 0, -x \rangle

Since curl(F⃗)≠0⃗\text{curl}(\vec{F}) \neq \vec{0} (specifically, the zz-component is −x-x, which is not identically zero), the vector field is not conservative. This is why we cannot use the Fundamental Theorem of Line Integrals and must evaluate the integral directly.

2. Compute the Line Integral

We evaluate ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r} using the parameterization r⃗(t)=⟨cos⁡t,sin⁡t,t⟩\vec{r}(t) = \langle \cos t, \sin t, t \rangle for 0≤t≤π0 \le t \le \pi.

Step 1: Find dr⃗d\vec{r}

r⃗′(t)=ddt⟨cos⁡t,sin⁡t,t⟩=⟨−sin⁡t,cos⁡t,1⟩ \vec{r}'(t) = \frac{d}{dt}\langle \cos t, \sin t, t \rangle = \langle -\sin t, \cos t, 1 \rangle

dr⃗=r⃗′(t) dt=⟨−sin⁡t,cos⁡t,1⟩ dt d\vec{r} = \vec{r}'(t) \, dt = \langle -\sin t, \cos t, 1 \rangle \, dt

Step 2: Evaluate F⃗\vec{F} on the curve Substitute x=cos⁡tx = \cos t, y=sin⁡ty = \sin t, and z=tz = t into F⃗\vec{F}:

F⃗(r⃗(t))=⟨(cos⁡t)(sin⁡t),3,t3⟩=⟨cos⁡tsin⁡t,3,t3⟩ \vec{F}(\vec{r}(t)) = \langle (\cos t)(\sin t), 3, t^3 \rangle = \langle \cos t \sin t, 3, t^3 \rangle

Step 3: Compute the dot product F⃗⋅dr⃗\vec{F} \cdot d\vec{r}

F⃗(r⃗(t))⋅r⃗′(t)=(cos⁡tsin⁡t)(−sin⁡t)+(3)(cos⁡t)+(t3)(1) \vec{F}(\vec{r}(t)) \cdot \vec{r}'(t) = (\cos t \sin t)(-\sin t) + (3)(\cos t) + (t^3)(1)

=−cos⁡tsin⁡2t+3cos⁡t+t3 = -\cos t \sin^2 t + 3 \cos t + t^3

Step 4: Integrate with respect to tt

∫CF⃗⋅dr⃗=∫0π(−cos⁡tsin⁡2t+3cos⁡t+t3) dt \int_C \vec{F} \cdot d\vec{r} = \int_0^{\pi} \left( -\cos t \sin^2 t + 3 \cos t + t^3 \right) \, dt

We can split this into three integrals:

=∫0π−cos⁡tsin⁡2t dt+∫0π3cos⁡t dt+∫0πt3 dt = \int_0^{\pi} -\cos t \sin^2 t \, dt + \int_0^{\pi} 3 \cos t \, dt + \int_0^{\pi} t^3 \, dt
  • First integral: Let u=sin⁡tu = \sin t, then du=cos⁡t dtdu = \cos t \, dt. The limits change from 0→00 \to 0 and π→0\pi \to 0.

    ∫0π−sin⁡2tcos⁡t dt=[−sin⁡3t3]0π=0−0=0 \int_0^{\pi} -\sin^2 t \cos t \, dt = \left[ -\frac{\sin^3 t}{3} \right]_0^{\pi} = 0 - 0 = 0
  • Second integral:

    ∫0π3cos⁡t dt=3[sin⁡t]0π=3(0−0)=0 \int_0^{\pi} 3 \cos t \, dt = 3 [\sin t]_0^{\pi} = 3(0 - 0) = 0
  • Third integral:

    ∫0πt3 dt=[t44]0π=π44−0=π44 \int_0^{\pi} t^3 \, dt = \left[ \frac{t^4}{4} \right]_0^{\pi} = \frac{\pi^4}{4} - 0 = \frac{\pi^4}{4}

Summing these results:

0+0+π44=π44 0 + 0 + \frac{\pi^4}{4} = \frac{\pi^4}{4}

Final Answer

∫CF⃗⋅dr⃗=π44 \int_C \vec{F} \cdot d\vec{r} = \frac{\pi^4}{4}

Q9. Scalar/Vector Line Integrals

Let CC be the line segment from the point (−2,1,0)(-2, 1, 0) to the point (−1,2,1)(-1, 2, 1). Set up the following integrals. Simplify the integrands.

  • (a) ∫Cf(x,y,z) ds\int_C f(x,y,z) \, ds, where f(x,y,z)=yz−x2f(x,y,z) = yz - x^2
  • (b) ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r}, where F⃗=⟨2x−y,2z,y−z⟩\vec{F} = \langle 2x-y, 2z, y-z \rangle
Answer of This Question

To solve these integrals, we first need to parametrize the line segment CC.

1. Parametrize the Curve CC

The curve CC is the line segment from P0=(−2,1,0)P_0 = (-2, 1, 0) to P1=(−1,2,1)P_1 = (-1, 2, 1).
The direction vector is v⃗=P1−P0=⟨−1−(−2),2−1,1−0⟩=⟨1,1,1⟩\vec{v} = P_1 - P_0 = \langle -1 - (-2), 2 - 1, 1 - 0 \rangle = \langle 1, 1, 1 \rangle.
We can parametrize the curve using tt where 0≤t≤10 \le t \le 1:

r⃗(t)=P0+tv⃗=⟨−2,1,0⟩+t⟨1,1,1⟩=⟨−2+t,1+t,t⟩ \vec{r}(t) = P_0 + t\vec{v} = \langle -2, 1, 0 \rangle + t\langle 1, 1, 1 \rangle = \langle -2+t, 1+t, t \rangle

Thus, the coordinates are:

x(t)=−2+t,y(t)=1+t,z(t)=t x(t) = -2+t, \quad y(t) = 1+t, \quad z(t) = t

The derivative of the position vector is:

r⃗′(t)=⟨1,1,1⟩ \vec{r}'(t) = \langle 1, 1, 1 \rangle

The magnitude of the derivative is:

∥r⃗′(t)∥=12+12+12=3 \|\vec{r}'(t)\| = \sqrt{1^2 + 1^2 + 1^2} = \sqrt{3}

Therefore, the differential arc length is ds=3 dtds = \sqrt{3} \, dt, and the differential vector is dr⃗=⟨1,1,1⟩ dtd\vec{r} = \langle 1, 1, 1 \rangle \, dt.


a. Scalar Line Integral

We need to set up ∫Cf(x,y,z) ds\int_C f(x,y,z) \, ds where f(x,y,z)=yz−x2f(x,y,z) = yz - x^2.

Step 1: Substitute the parametrization into ff

f(r⃗(t))=y(t)z(t)−(x(t))2=(1+t)(t)−(−2+t)2 f(\vec{r}(t)) = y(t)z(t) - (x(t))^2 = (1+t)(t) - (-2+t)^2

Step 2: Simplify the integrand

=(t+t2)−(4−4t+t2) = (t + t^2) - (4 - 4t + t^2)

=t+t2−4+4t−t2 = t + t^2 - 4 + 4t - t^2

=5t−4 = 5t - 4

Step 3: Set up the integral

∫Cf(x,y,z) ds=∫01(5t−4)3 dt \int_C f(x,y,z) \, ds = \int_0^1 (5t - 4) \sqrt{3} \, dt

Step 4: Evaluate

=3∫01(5t−4) dt=3[5t22−4t]01 = \sqrt{3} \int_0^1 (5t - 4) \, dt = \sqrt{3} \left[ \frac{5t^2}{2} - 4t \right]_0^1

=3(52−4)=3(−32)=−332 = \sqrt{3} \left( \frac{5}{2} - 4 \right) = \sqrt{3} \left( -\frac{3}{2} \right) = -\frac{3\sqrt{3}}{2}

b. Vector Line Integral

We need to set up ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r} where F⃗=⟨2x−y,2z,y−z⟩\vec{F} = \langle 2x-y, 2z, y-z \rangle.

Step 1: Substitute the parametrization into F⃗\vec{F}

F⃗(r⃗(t))=⟨2(−2+t)−(1+t), 2(t), (1+t)−t⟩ \vec{F}(\vec{r}(t)) = \langle 2(-2+t) - (1+t), \, 2(t), \, (1+t) - t \rangle

Step 2: Simplify the components of F⃗\vec{F}

  • xx-component: 2(−2+t)−(1+t)=−4+2t−1−t=t−52(-2+t) - (1+t) = -4 + 2t - 1 - t = t - 5
  • yy-component: 2t2t
  • zz-component: 1+t−t=11 + t - t = 1 So, F⃗(r⃗(t))=⟨t−5,2t,1⟩\vec{F}(\vec{r}(t)) = \langle t - 5, 2t, 1 \rangle.

Step 3: Compute the dot product F⃗⋅r⃗′(t)\vec{F} \cdot \vec{r}'(t)

F⃗(r⃗(t))⋅r⃗′(t)=⟨t−5,2t,1⟩⋅⟨1,1,1⟩ \vec{F}(\vec{r}(t)) \cdot \vec{r}'(t) = \langle t - 5, 2t, 1 \rangle \cdot \langle 1, 1, 1 \rangle

=(t−5)(1)+(2t)(1)+(1)(1) = (t - 5)(1) + (2t)(1) + (1)(1)

=t−5+2t+1=3t−4 = t - 5 + 2t + 1 = 3t - 4

Step 4: Set up the integral

∫CF⃗⋅dr⃗=∫01(3t−4) dt \int_C \vec{F} \cdot d\vec{r} = \int_0^1 (3t - 4) \, dt

Step 5: Evaluate

=[3t22−4t]01 = \left[ \frac{3t^2}{2} - 4t \right]_0^1

=(32−4)−0=32−82=−52 = \left( \frac{3}{2} - 4 \right) - 0 = \frac{3}{2} - \frac{8}{2} = -\frac{5}{2}

Final Answer

a. ∫C(yz−x2) ds=∫013(5t−4) dt=−332\displaystyle \int_C (yz - x^2) \, ds = \int_0^1 \sqrt{3}(5t - 4) \, dt = -\frac{3\sqrt{3}}{2}
b. ∫CF⃗⋅dr⃗=∫01(3t−4) dt=−52\displaystyle \int_C \vec{F} \cdot d\vec{r} = \int_0^1 (3t - 4) \, dt = -\frac{5}{2}

Q10 Conservative Vector Field

Let F⃗=⟨3+2xy,x2−3y2⟩\vec{F} = \langle 3+2xy, x^2-3y^2 \rangle.

  • (a) Show that F⃗\vec{F} is conservative, then find a potential function for F⃗\vec{F}.
  • (b) Evaluate ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r}, where CC is given by r⃗(t)=⟨etsin⁡t,etcos⁡t⟩,0≤t≤π\vec{r}(t) = \langle e^t \sin t, e^t \cos t \rangle, 0 \le t \le \pi.
Answer of This Question

a. Show that F⃗\vec{F} is conservative and find a potential function

Let F⃗=⟨P,Q⟩\vec{F} = \langle P, Q \rangle, where P=3+2xyP = 3+2xy and Q=x2−3y2Q = x^2-3y^2.
For F⃗\vec{F} to be conservative on a simply connected domain (like R2\mathbb{R}^2), the condition ∂P∂y=∂Q∂x\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x} must hold.

Calculate the partial derivatives:

∂P∂y=∂∂y(3+2xy)=2x \frac{\partial P}{\partial y} = \frac{\partial}{\partial y}(3+2xy) = 2x

∂Q∂x=∂∂x(x2−3y2)=2x \frac{\partial Q}{\partial x} = \frac{\partial}{\partial x}(x^2-3y^2) = 2x

Since ∂P∂y=∂Q∂x\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x}, the vector field F⃗\vec{F} is conservative.

To find the potential function f(x,y)f(x,y) such that ∇f=F⃗\nabla f = \vec{F}, we solve the system:

  1. ∂f∂x=3+2xy\frac{\partial f}{\partial x} = 3+2xy
  2. ∂f∂y=x2−3y2\frac{\partial f}{\partial y} = x^2-3y^2

Integrate the first equation with respect to xx:

f(x,y)=∫(3+2xy) dx=3x+x2y+g(y) f(x,y) = \int (3+2xy) \, dx = 3x + x^2y + g(y)

where g(y)g(y) is an arbitrary function of yy.

Now, differentiate this expression with respect to yy and set it equal to QQ:

∂f∂y=∂∂y(3x+x2y+g(y))=x2+g′(y) \frac{\partial f}{\partial y} = \frac{\partial}{\partial y}(3x + x^2y + g(y)) = x^2 + g'(y)

x2+g′(y)=x2−3y2 x^2 + g'(y) = x^2 - 3y^2

g′(y)=−3y2 g'(y) = -3y^2

Integrate with respect to yy:

g(y)=∫−3y2 dy=−y3+C g(y) = \int -3y^2 \, dy = -y^3 + C

Thus, the potential function is:

f(x,y)=3x+x2y−y3+C f(x,y) = 3x + x^2y - y^3 + C

We can choose C=0C=0 for simplicity.


b. Evaluate ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r}

Since F⃗\vec{F} is conservative, we can use the Fundamental Theorem of Line Integrals:

∫CF⃗⋅dr⃗=f(end point)−f(start point) \int_C \vec{F} \cdot d\vec{r} = f(\text{end point}) - f(\text{start point})

The curve CC is parameterized by r⃗(t)=⟨etsin⁡t,etcos⁡t⟩\vec{r}(t) = \langle e^t \sin t, e^t \cos t \rangle for 0≤t≤π0 \le t \le \pi.

Find the start point (t=0t=0):

r⃗(0)=⟨e0sin⁡0,e0cos⁡0⟩=⟨0,1⟩ \vec{r}(0) = \langle e^0 \sin 0, e^0 \cos 0 \rangle = \langle 0, 1 \rangle

Find the end point (t=πt=\pi):

r⃗(π)=⟨eπsin⁡π,eπcos⁡π⟩=⟨0,−eπ⟩ \vec{r}(\pi) = \langle e^\pi \sin \pi, e^\pi \cos \pi \rangle = \langle 0, -e^\pi \rangle

Evaluate the potential function f(x,y)=3x+x2y−y3f(x,y) = 3x + x^2y - y^3 at these points: At the start point (0,1)(0, 1):

f(0,1)=3(0)+02(1)−13=−1 f(0, 1) = 3(0) + 0^2(1) - 1^3 = -1

At the end point (0,−eπ)(0, -e^\pi):

f(0,−eπ)=3(0)+02(−eπ)−(−eπ)3=−(−e3π)=e3π f(0, -e^\pi) = 3(0) + 0^2(-e^\pi) - (-e^\pi)^3 = -(-e^{3\pi}) = e^{3\pi}

Calculate the integral:

∫CF⃗⋅dr⃗=f(0,−eπ)−f(0,1)=e3π−(−1)=e3π+1 \int_C \vec{F} \cdot d\vec{r} = f(0, -e^\pi) - f(0, 1) = e^{3\pi} - (-1) = e^{3\pi} + 1

Final Answer

a. F⃗\vec{F} is conservative because ∂P∂y=∂Q∂x=2x\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x} = 2x. A potential function is f(x,y)=3x+x2y−y3f(x,y) = 3x + x^2y - y^3.
b. ∫CF⃗⋅dr⃗=e3π+1\displaystyle \int_C \vec{F} \cdot d\vec{r} = e^{3\pi} + 1

Q11. Conservative Vector Field

The vector field F⃗=⟨2xy−z,x2+2y,1−x⟩\vec{F} = \langle 2xy-z, x^2+2y, 1-x \rangle is conservative.

  • (a) Find a potential function for F⃗\vec{F}.
  • (b) Using the potential function from (a) evaluate ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r} where CC is any curve from (1,0,2)(1, 0, 2) to (2,1,3)(2, 1, 3).
Answer of This Question

a. Find a potential function for F⃗\vec{F}

Since F⃗\vec{F} is conservative, there exists a potential function f(x,y,z)f(x, y, z) such that ∇f=F⃗\nabla f = \vec{F}. This implies:

∂f∂x=2xy−z,∂f∂y=x2+2y,∂f∂z=1−x \frac{\partial f}{\partial x} = 2xy - z, \quad \frac{\partial f}{\partial y} = x^2 + 2y, \quad \frac{\partial f}{\partial z} = 1 - x
  1. Integrate with respect to xx:

    f(x,y,z)=∫(2xy−z) dx=x2y−xz+g(y,z) f(x, y, z) = \int (2xy - z) \, dx = x^2y - xz + g(y, z)

    where g(y,z)g(y, z) is an arbitrary function of yy and zz.

  2. Differentiate with respect to yy and compare:

    ∂f∂y=∂∂y(x2y−xz+g(y,z))=x2+∂g∂y \frac{\partial f}{\partial y} = \frac{\partial}{\partial y}(x^2y - xz + g(y, z)) = x^2 + \frac{\partial g}{\partial y}

    Comparing this to the given component ∂f∂y=x2+2y\frac{\partial f}{\partial y} = x^2 + 2y, we get:

    x2+∂g∂y=x2+2y  ⟹  ∂g∂y=2y x^2 + \frac{\partial g}{\partial y} = x^2 + 2y \implies \frac{\partial g}{\partial y} = 2y
  3. Integrate with respect to yy:

    g(y,z)=∫2y dy=y2+h(z) g(y, z) = \int 2y \, dy = y^2 + h(z)

    where h(z)h(z) is an arbitrary function of zz. Substituting this back into ff:

    f(x,y,z)=x2y−xz+y2+h(z) f(x, y, z) = x^2y - xz + y^2 + h(z)
  4. Differentiate with respect to zz and compare:

    ∂f∂z=∂∂z(x2y−xz+y2+h(z))=−x+h′(z) \frac{\partial f}{\partial z} = \frac{\partial}{\partial z}(x^2y - xz + y^2 + h(z)) = -x + h'(z)

    Comparing this to the given component ∂f∂z=1−x\frac{\partial f}{\partial z} = 1 - x, we get:

    −x+h′(z)=1−x  ⟹  h′(z)=1 -x + h'(z) = 1 - x \implies h'(z) = 1
  5. Integrate with respect to zz:

    h(z)=∫1 dz=z+C h(z) = \int 1 \, dz = z + C

    Combining all parts, the potential function is:

    f(x,y,z)=x2y−xz+y2+z+C f(x, y, z) = x^2y - xz + y^2 + z + C

    We can set C=0C=0 for simplicity.


b. Evaluate ∫CF⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r}

By the Fundamental Theorem of Line Integrals, since F⃗=∇f\vec{F} = \nabla f:

∫CF⃗⋅dr⃗=f(end point)−f(start point) \int_C \vec{F} \cdot d\vec{r} = f(\text{end point}) - f(\text{start point})

The curve CC goes from A=(1,0,2)A = (1, 0, 2) to B=(2,1,3)B = (2, 1, 3).

Evaluate ff at B(2,1,3)B(2, 1, 3):

f(2,1,3)=(2)2(1)−(2)(3)+(1)2+3=4−6+1+3=2 f(2, 1, 3) = (2)^2(1) - (2)(3) + (1)^2 + 3 = 4 - 6 + 1 + 3 = 2

Evaluate ff at A(1,0,2)A(1, 0, 2):

f(1,0,2)=(1)2(0)−(1)(2)+(0)2+2=0−2+0+2=0 f(1, 0, 2) = (1)^2(0) - (1)(2) + (0)^2 + 2 = 0 - 2 + 0 + 2 = 0

Calculate the difference:

∫CF⃗⋅dr⃗=2−0=2 \int_C \vec{F} \cdot d\vec{r} = 2 - 0 = 2

Final Answer

a. A potential function is f(x,y,z)=x2y−xz+y2+zf(x, y, z) = x^2y - xz + y^2 + z.
b. ∫CF⃗⋅dr⃗=2\displaystyle \int_C \vec{F} \cdot d\vec{r} = 2

Q12. Green’s Theorem

Use Green’s Theorem to compute the integral ∮Cxy3 dx+x2y2 dy\oint_C xy^3 \, dx + x^2y^2 \, dy where CC is the rectangle with vertices (0,0),(2,0),(2,3),(0,3)(0,0), (2,0), (2,3), (0,3) oriented counter clockwise.

Answer of This Question

To evaluate the line integral using Green’s Theorem, we proceed with the following steps.

1. State Green’s Theorem

Green’s Theorem relates a line integral around a simple closed curve CC to a double integral over the plane region DD bounded by CC. For a positively oriented (counter-clockwise) curve CC:

∮CP dx+Q dy=∬D(∂Q∂x−∂P∂y) dA \oint_C P \, dx + Q \, dy = \iint_D \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) \, dA

2. Identify PP and QQ

From the given integral ∮Cxy3 dx+x2y2 dy\oint_C xy^3 \, dx + x^2y^2 \, dy, we identify:

P(x,y)=xy3,Q(x,y)=x2y2 P(x, y) = xy^3, \quad Q(x, y) = x^2y^2

3. Compute the Partial Derivatives

Calculate the partial derivative of QQ with respect to xx:

∂Q∂x=∂∂x(x2y2)=2xy2 \frac{\partial Q}{\partial x} = \frac{\partial}{\partial x}(x^2y^2) = 2xy^2

Calculate the partial derivative of PP with respect to yy:

∂P∂y=∂∂y(xy3)=3xy2 \frac{\partial P}{\partial y} = \frac{\partial}{\partial y}(xy^3) = 3xy^2

4. Determine the Integrand

Subtract the partial derivatives:

∂Q∂x−∂P∂y=2xy2−3xy2=−xy2 \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 2xy^2 - 3xy^2 = -xy^2

5. Define the Region DD

The region DD is the rectangle with vertices (0,0),(2,0),(2,3),(0,3)(0,0), (2,0), (2,3), (0,3). This region can be described by the inequalities:

0≤x≤2,0≤y≤3 0 \le x \le 2, \quad 0 \le y \le 3

6. Set Up and Evaluate the Double Integral

Substitute the integrand and the limits into the double integral:

∬D(−xy2) dA=∫03∫02−xy2 dx dy \iint_D (-xy^2) \, dA = \int_0^3 \int_0^2 -xy^2 \, dx \, dy

First, evaluate the inner integral with respect to xx:

∫02−xy2 dx=−y2[x22]02=−y2(42−0)=−2y2 \int_0^2 -xy^2 \, dx = -y^2 \left[ \frac{x^2}{2} \right]_0^2 = -y^2 \left( \frac{4}{2} - 0 \right) = -2y^2

Next, evaluate the outer integral with respect to yy:

∫03−2y2 dy=−2[y33]03=−2(273−0)=−2(9)=−18 \int_0^3 -2y^2 \, dy = -2 \left[ \frac{y^3}{3} \right]_0^3 = -2 \left( \frac{27}{3} - 0 \right) = -2(9) = -18

Final Answer

∮Cxy3 dx+x2y2 dy=−18 \oint_C xy^3 \, dx + x^2y^2 \, dy = -18

Q13. Green’s Theorem

Use Green’s Theorem to evaluate ∮C(3y−esin⁡x) dx+(7x+y4+1) dy\oint_C (3y - e^{\sin x}) \, dx + (7x + \sqrt{y^4+1}) \, dy, where CC is the circle x2+y2=9x^2+y^2=9 oriented counterclockwise.

Answer of This Question

To evaluate the line integral using Green’s Theorem, we proceed with the following steps.

1. State Green’s Theorem

Green’s Theorem relates a line integral around a simple closed curve CC to a double integral over the plane region DD bounded by CC. For a positively oriented (counter-clockwise) curve CC:

∮CP dx+Q dy=∬D(∂Q∂x−∂P∂y) dA \oint_C P \, dx + Q \, dy = \iint_D \left( \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} \right) \, dA

2. Identify PP and QQ

From the given integral ∮C(3y−esin⁡x) dx+(7x+y4+1) dy\oint_C (3y - e^{\sin x}) \, dx + (7x + \sqrt{y^4+1}) \, dy, we identify:

P(x,y)=3y−esin⁡x,Q(x,y)=7x+y4+1 P(x, y) = 3y - e^{\sin x}, \quad Q(x, y) = 7x + \sqrt{y^4+1}

3. Compute the Partial Derivatives

Calculate the partial derivative of QQ with respect to xx:

∂Q∂x=∂∂x(7x+y4+1)=7+0=7 \frac{\partial Q}{\partial x} = \frac{\partial}{\partial x}(7x + \sqrt{y^4+1}) = 7 + 0 = 7

Calculate the partial derivative of PP with respect to yy:

∂P∂y=∂∂y(3y−esin⁡x)=3−0=3 \frac{\partial P}{\partial y} = \frac{\partial}{\partial y}(3y - e^{\sin x}) = 3 - 0 = 3

Note that the complicated terms esin⁡xe^{\sin x} and y4+1\sqrt{y^4+1} vanish upon differentiation because they depend only on xx and yy respectively, not the variable of differentiation.

4. Determine the Integrand

Subtract the partial derivatives:

∂Q∂x−∂P∂y=7−3=4 \frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 7 - 3 = 4

5. Define the Region DD

The curve CC is the circle x2+y2=9x^2+y^2=9. This is a circle centered at the origin with radius r=9=3r = \sqrt{9} = 3.
The region DD is the disk enclosed by this circle.

6. Set Up and Evaluate the Double Integral

Substitute the integrand and the limits into the double integral:

∬D4 dA=4∬DdA \iint_D 4 \, dA = 4 \iint_D dA

The integral ∬DdA\iint_D dA represents the area of the region DD. Since DD is a disk with radius r=3r=3, its area is:

Area(D)=πr2=π(3)2=9π \text{Area}(D) = \pi r^2 = \pi (3)^2 = 9\pi

Therefore, the value of the double integral is:

4×9π=36π 4 \times 9\pi = 36\pi

Final Answer

∮C(3y−esin⁡x) dx+(7x+y4+1) dy=36π \oint_C (3y - e^{\sin x}) \, dx + (7x + \sqrt{y^4+1}) \, dy = 36\pi

Cribs

Double Integral in Polar Coordinates

For a continuous function ff on the domain

D:θ1≤θ≤θ2,r1(θ)≤r≤r2(θ)D: \theta_1 \le \theta \le \theta_2, \quad r_1(\theta) \le r \le r_2(\theta)∬Df(x,y) dA=∫θ1θ2∫r1(θ)r2(θ)f(rcos⁡θ,rsin⁡θ) r dr dθ\iint_D f(x,y) \, dA = \int_{\theta_1}^{\theta_2} \int_{r_1(\theta)}^{r_2(\theta)} f(r\cos\theta, r\sin\theta) \, r \, dr \, d\theta

Here, the region DD is radially simple.

Notes:

  • The transformation uses: x=rcos⁡θx = r\cos\theta, y=rsin⁡θy = r\sin\theta
  • The extra factor of rr in the integrand comes from the Jacobian determinant of the polar coordinate transformation
  • The region DD is described as a polar rectangle where the radial bounds may depend on the angle θ\theta

Operations on Vector Fields

Let F⃗=⟨F1,F2,F3⟩\vec{F} = \langle F_1, F_2, F_3 \rangle be a vector field. We define:

  1. The Divergence of F⃗\vec{F}

    div(F⃗)=∇⋅F⃗=⟨∂∂x,∂∂y,∂∂z⟩⋅⟨F1,F2,F3⟩\text{div}(\vec{F}) = \nabla \cdot \vec{F} = \left\langle \frac{\partial}{\partial x}, \frac{\partial}{\partial y}, \frac{\partial}{\partial z} \right\rangle \cdot \langle F_1, F_2, F_3 \rangle=∂F1∂x+∂F2∂y+∂F3∂z= \frac{\partial F_1}{\partial x} + \frac{\partial F_2}{\partial y} + \frac{\partial F_3}{\partial z}
  2. The Curl of F⃗\vec{F}

    curl(F⃗)=∇×F⃗=∣i^j^k^∂∂x∂∂y∂∂zF1F2F3∣\text{curl}(\vec{F}) = \nabla \times \vec{F} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\ F_1 & F_2 & F_3 \end{vmatrix}=(∂F3∂y−∂F2∂z)i^−(∂F3∂x−∂F1∂z)j^+(∂F2∂x−∂F1∂y)k^= \left(\frac{\partial F_3}{\partial y} - \frac{\partial F_2}{\partial z}\right)\hat{i} - \left(\frac{\partial F_3}{\partial x} - \frac{\partial F_1}{\partial z}\right)\hat{j} + \left(\frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y}\right)\hat{k}=⟨∂F3∂y−∂F2∂z, ∂F1∂z−∂F3∂x, ∂F2∂x−∂F1∂y⟩= \left\langle \frac{\partial F_3}{\partial y} - \frac{\partial F_2}{\partial z}, \ \frac{\partial F_1}{\partial z} - \frac{\partial F_3}{\partial x}, \ \frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y} \right\rangle

Curl of a Conservative Vector Field

  1. In R2\mathbf{R}^2, if the vector field F=⟨F1,F2⟩\mathbf{F} = \langle F_1, F_2 \rangle is conservative, then
∂F1∂y=∂F2∂x\frac{\partial F_1}{\partial y} = \frac{\partial F_2}{\partial x}
  1. In R3\mathbf{R}^3, if the vector field F=⟨F1,F2,F3⟩\mathbf{F} = \langle F_1, F_2, F_3 \rangle is conservative, then
curl(F)=0,or equivalently,∂F1∂y=∂F2∂x, ∂F2∂z=∂F3∂y, ∂F3∂x=∂F1∂z\text{curl}(\mathbf{F}) = \mathbf{0}, \quad \text{or equivalently,} \quad \frac{\partial F_1}{\partial y} = \frac{\partial F_2}{\partial x}, \ \frac{\partial F_2}{\partial z} = \frac{\partial F_3}{\partial y}, \ \frac{\partial F_3}{\partial x} = \frac{\partial F_1}{\partial z}

Computing a Scalar Line Integral

Let r⃗(t)\vec{r}(t) be a parameterization that directly traverses a curve CC for a≤t≤ba \le t \le b. If f(x,y,z)f(x,y,z) and r⃗(t)\vec{r}(t) are continuous, then

∫Cf(x,y,z) ds=∫t=at=bf(r⃗(t)) ∥r⃗′(t)∥ dt(similar in 2D)\int_C f(x,y,z) \, ds = \int_{t=a}^{t=b} f(\vec{r}(t)) \, \|\vec{r}'(t)\| \, dt \quad \text{(similar in 2D)}

∫Cf(x,y),ds=∫abf(x(t),y(t)) (dxdt)2+(dydt)2 dt\int_C f(x,y),ds=\int_a^b f(x(t),y(t)) \, \sqrt{\left(\frac{dx}{dt}\right)^2+\left(\frac{dy}{dt}\right)^2} \, dt

where r⃗(t)=⟨x(t),y(t),z(t)⟩\vec{r}(t) = \langle x(t), y(t), z(t) \rangle

  • ds=∥r⃗′(t)∥ dtds = \|\vec{r}'(t)\| \, dt is called the arc length differential

  • The value of the scalar line integral does not depend on the parameterization of CC used as long as CC is only traced once from t=at=a to t=bt=b.

Computing a Vector Line Integrals

Let F⃗\vec{F} be a continuous vector field defined on a smooth, oriented curve CC given by r⃗(t)\vec{r}(t), a≤t≤ba \le t \le b. Then the line integral of F⃗\vec{F} along CC is:

∫CF⃗⋅dr⃗=∫abF⃗(r⃗(t))⋅r⃗′(t) dt=∫CF⃗⋅r⃗′(t)∥r⃗′(t)∥∥r⃗′(t)∥ dt=∫CF⃗⋅T⃗ ds\int_C \vec{F} \cdot d\vec{r} = \int_a^b \vec{F}(\vec{r}(t)) \cdot \vec{r}'(t) \, dt = \int_C \vec{F} \cdot \frac{\vec{r}'(t)}{\|\vec{r}'(t)\|} \|\vec{r}'(t)\| \, dt = \int_C \vec{F} \cdot \vec{T} \, ds

where T⃗=r⃗′(t)∥r⃗′(t)∥\vec{T} = \frac{\vec{r}'(t)}{\|\vec{r}'(t)\|} is the unit tangent vector.

Fundamental Theorem of Line Integrals

∫CF⃗⋅dr⃗=f(end point)−f(start point) \int_C \vec{F} \cdot d\vec{r} = f(\text{end point}) - f(\text{start point})

Green’s Theorem

Let DD be a domain whose boundary ∂D\partial D is a positively-oriented, simple closed curve in the plane. If F⃗=⟨F1,F2⟩\vec{F} = \langle F_1, F_2 \rangle, where F1F_1 and F2F_2 have continuous partial derivatives, then

∮CF⃗⋅dr⃗=∮∂DF1 dx+F2 dy=∬D(∂F2∂x−∂F1∂y) dA\oint_C \vec{F} \cdot d\vec{r} = \oint_{\partial D} F_1 \, dx + F_2 \, dy = \iint_D \left(\frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y}\right) \, dA

where C=∂DC = \partial D

Notation for vector line integrals:

  • ∮CF⃗⋅dr⃗\oint_C \vec{F} \cdot d\vec{r} — Notation 1
  • ∮∂DF1 dx+F2 dy\oint_{\partial D} F_1 \, dx + F_2 \, dy — Notation 2

Green’s Theorem for a Curve That Is Not Closed

Let CC be a non-closed curve that can be completed to form a closed boundary ∂D=C+C1\partial D = C + C_1, where C1C_1 is an auxiliary curve that closes the region DD. If F⃗=⟨F1,F2⟩\vec{F} = \langle F_1, F_2 \rangle has continuous partial derivatives on DD, then by Green’s Theorem:

∮∂DF⃗⋅dr⃗=∫CF⃗⋅dr⃗+∫C1F⃗⋅dr⃗=∬D(∂F2∂x−∂F1∂y)dA\oint_{\partial D} \vec{F} \cdot d\vec{r} = \int_C \vec{F} \cdot d\vec{r} + \int_{C_1} \vec{F} \cdot d\vec{r} = \iint_D \left(\frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y}\right) dA

Rearranging to solve for the line integral along the non-closed curve CC:

∫CF⃗⋅dr⃗=∬D(∂F2∂x−∂F1∂y)dA−∫C1F⃗⋅dr⃗\int_C \vec{F} \cdot d\vec{r} = \iint_D \left(\frac{\partial F_2}{\partial x} - \frac{\partial F_1}{\partial y}\right) dA - \int_{C_1} \vec{F} \cdot d\vec{r}

Note: The orientation of CC and C1C_1 must be consistent with the positive (counterclockwise) orientation of the closed boundary ∂D\partial D.

Trigonometric Function

cos⁡(θ)=x, sin⁡(θ)=ytan⁡(θ)=sin⁡(θ)cos⁡(θ)=yxsec⁡(θ)=1cos⁡(θ)=1xcsc⁡(θ)=1sin⁡(θ)=1ycot⁡(θ)=cos⁡(θ)sin⁡(θ)=xysin⁡(θ)=opphypcos⁡(θ)=adjhyptan⁡(θ)=sin⁡(θ)cos⁡(θ)=opphypadjhyp⋅hyp1hyp1=oppadj \begin{align*} \cos(\theta) &= x ,\: \sin(\theta) = y \\ \tan(\theta) &= \frac{\sin(\theta)}{\cos(\theta)} = \frac{y}{x} \\ \sec(\theta) &= \frac{1}{\cos(\theta)} = \frac{1}{x} \\ \csc(\theta) &= \frac{1}{\sin(\theta)} = \frac{1}{y} \\ \cot(\theta) &= \frac{\cos(\theta)}{\sin(\theta)} = \frac{x}{y} \\ \sin(\theta) &= \frac{opp}{hyp} \\ \cos(\theta) &= \frac{adj}{hyp} \\ \tan(\theta) &= \frac{\sin(\theta)}{\cos(\theta)} = \frac{\frac{opp}{\cancel{hyp}}}{\frac{adj}{\cancel{hyp}}} \cdot \frac{\frac{\cancel{hyp}}{1}}{\frac{\cancel{hyp}}{1}} = \frac{opp}{adj} \end{align*}
a  rada\;rad 00 π6\frac{\pi}{6} π4\frac{\pi}{4} π3\frac{\pi}{3} π2\frac{\pi}{2} π\pi
sin⁡(a)\sin(a) 00 12\frac{1}{2} 22\frac{\sqrt{2}}{2} 32\frac{\sqrt{3}}{2} 11 00
cos⁡(a)\cos(a) 11 32\frac{\sqrt{3}}{2} 22\frac{\sqrt{2}}{2} 12\frac{1}{2} 00 −1-1
tan⁡(a)\tan(a) 00 13\frac{1}{\sqrt{3}} 11 3\sqrt{3} −- 00

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