Exam 2 Review Problems

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 DxydA\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 DxydA\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    x2x=0    x(x1)=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)0x1,xyx} 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:

DxydA=01xxxydydx \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:

xxxydy=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)22x22)=x(x2x22)=x22x32 = 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(x22x32)dx=[x36x48]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:

=(136148)(00)=1618 = \left( \frac{1^3}{6} - \frac{1^4}{8} \right) - (0 - 0) = \frac{1}{6} - \frac{1}{8}

Finding a common denominator:

=424324=124 = \frac{4}{24} - \frac{3}{24} = \frac{1}{24}

Final Answer

DxydA=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 x0,y0x \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=rcosθ,y=rsinθ 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 rdrdθr \, 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 x0x \ge 0 and y0y \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 2r32 \le r \le 3.
  • The constraints x0x \ge 0 and y0y \ge 0 restrict the region to the first quadrant, which corresponds to 0θπ20 \le \theta \le \frac{\pi}{2}.

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

D={(r,θ)2r3,0θπ2} 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/223(r2)rdrdθ=0π/223r3drdθ \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:

23r3dr=[r44]23=344244=814164=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/2654dθ=654[θ]0π/2=654(π20)=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+y216,x+y4x^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+y216x^2+y^2 \le 16: This is a disk of radius 4 centered at the origin.
  • x+y4x+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=4xy = 4-x into the circle equation:

x2+(4x)2=16 x^2 + (4-x)^2 = 16

x2+168x+x2=16 x^2 + 16 - 8x + x^2 = 16

2x28x=0    2x(x4)=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=rcosθx = r \cos \theta
  • y=rsinθy = r \sin \theta
  • x2+y2=r2x^2 + y^2 = r^2
  • dA=rdrdθdA = r \, dr \, d\theta

The integrand becomes:

(x2+y2)3/2=(r2)3/2=r3 (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(cosθ+sinθ)=4r(\cos\theta + \sin\theta) = 4, so r=4cosθ+sinθr = \frac{4}{\cos\theta + \sin\theta}. From the circle, r=4r = 4. Thus, 4cosθ+sinθr4\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, 0θπ20 \le \theta \le \frac{\pi}{2}.

5. Set Up the Integral

D(x2+y2)3/2dA=0π/24cosθ+sinθ4r3rdrdθ \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/24cosθ+sinθ4r2drdθ = \int_0^{\pi/2} \int_{\frac{4}{\cos\theta + \sin\theta}}^4 r^{-2} \, dr \, d\theta

6. Evaluate the Inner Integral

4cosθ+sinθ4r2dr=[1r]4cosθ+sinθ4 \int_{\frac{4}{\cos\theta + \sin\theta}}^4 r^{-2} \, dr = \left[ -\frac{1}{r} \right]_{\frac{4}{\cos\theta + \sin\theta}}^4

=14(cosθ+sinθ4)=cosθ+sinθ14 = -\frac{1}{4} - \left( -\frac{\cos\theta + \sin\theta}{4} \right) = \frac{\cos\theta + \sin\theta - 1}{4}

7. Evaluate the Outer Integral

0π/2cosθ+sinθ14dθ=140π/2(cosθ+sinθ1)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[sinθcosθθ]0π/2 = \frac{1}{4} \left[ \sin\theta - \cos\theta - \theta \right]_0^{\pi/2}

=14[(sinπ2cosπ2π2)(sin0cos00)] = \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[(10π2)(010)] = \frac{1}{4} \left[ (1 - 0 - \frac{\pi}{2}) - (0 - 1 - 0) \right]

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

=12π8 = \frac{1}{2} - \frac{\pi}{8}

Final Answer

D(x2+y2)3/2dA=12π8 \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:

0x1,2y4,0z2 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=012402(xz+yz2)dzdydx \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+83y22]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 W66zdV\iiint_W 66z \, dV where W:x2y1,0x1,xyzx+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 W66zdV\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:

  • 0x10 \le x \le 1
  • x2y1x^2 \le y \le 1
  • xyzx+yx-y \le z \le x+y

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

W66zdV=01x21xyx+y66zdzdydx \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:

xyx+y66zdz=66[z22]xyx+y=33[z2]xyx+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(xy)2) = 33 \left( (x+y)^2 - (x-y)^2 \right)

Using the identity (a+b)2(ab)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:

x21132xydy=132xx21ydy \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(12x42)=66x(1x4)=66x66x5 = 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(66x66x5)dx=6601(xx5)dx \int_0^1 (66x - 66x^5) \, dx = 66 \int_0^1 (x - x^5) \, dx

=66[x22x66]01 = 66 \left[ \frac{x^2}{2} - \frac{x^6}{6} \right]_0^1

Evaluating at the boundaries:

=66((1216)0) = 66 \left( \left( \frac{1}{2} - \frac{1}{6} \right) - 0 \right)

Finding a common denominator for the fractions:

=66(3616)=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

W66zdV=22 \iiint_W 66z \, dV = 22

Q6. Vector Fields

Find div(F)\text{div}(\vec{F}) and curl(F)\text{curl}(\vec{F}) if F=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 F=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 F\vec{F} is given by the dot product of the del operator \nabla and the vector field F\vec{F}:

div(F)=F=Px+Qy+Rz \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:

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

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

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

Adding these together, we get:

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

2. Calculate the Curl

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

curl(F)=×F=ijkxyzPQR \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}

=RyQz,PzRx,QxPy = \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: Ry=0,Qz=3e2y+3z    03e2y+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: Pz=0,Rx=2x    02x=2x \frac{\partial P}{\partial z} = 0, \quad \frac{\partial R}{\partial x} = 2x \implies 0 - 2x = -2x
  • For the k\mathbf{k}-component: Qx=0,Py=x    0x=x \frac{\partial Q}{\partial x} = 0, \quad \frac{\partial P}{\partial y} = x \implies 0 - x = -x

Thus, the curl is:

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

Final Answer

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

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

Q7. Line Integrals

Evaluate C1+36xyds\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+36xyds\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.

r(t)=t,4t3,0t1 \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)2dt 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)2dt=1+144t4dt 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+36xyds=011+144t41+144t4dt \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+36xyds=1495 \int_C \sqrt{1+36xy} \, ds = \frac{149}{5}

Q8. Line Integrals

Compute CFdr\int_C \vec{F} \cdot d\vec{r} if F=xy,3,z3\vec{F} = \langle xy, 3, z^3 \rangle and CC is the curve parameterized by r(t)=cost,sint,t\vec{r}(t) = \langle \cos t, \sin t, t \rangle for 0tπ0 \le t \le \pi.
Note: F\vec{F} is not conservative. How do you know?

Answer of This Question

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

1. Is F\vec{F} Conservative?

A vector field F=P,Q,R\vec{F} = \langle P, Q, R \rangle is conservative if and only if curl(F)=0\text{curl}(\vec{F}) = \vec{0} (assuming the domain is simply connected).
Given F=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(F)=×F=RyQz,PzRx,QxPy \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:

  • RyQz=00=0\frac{\partial R}{\partial y} - \frac{\partial Q}{\partial z} = 0 - 0 = 0
  • PzRx=00=0\frac{\partial P}{\partial z} - \frac{\partial R}{\partial x} = 0 - 0 = 0
  • QxPy=0x=x\frac{\partial Q}{\partial x} - \frac{\partial P}{\partial y} = 0 - x = -x

Thus,

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

Since curl(F)0\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 CFdr\int_C \vec{F} \cdot d\vec{r} using the parameterization r(t)=cost,sint,t\vec{r}(t) = \langle \cos t, \sin t, t \rangle for 0tπ0 \le t \le \pi.

Step 1: Find drd\vec{r}

r(t)=ddtcost,sint,t=sint,cost,1 \vec{r}'(t) = \frac{d}{dt}\langle \cos t, \sin t, t \rangle = \langle -\sin t, \cos t, 1 \rangle

dr=r(t)dt=sint,cost,1dt d\vec{r} = \vec{r}'(t) \, dt = \langle -\sin t, \cos t, 1 \rangle \, dt

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

F(r(t))=(cost)(sint),3,t3=costsint,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 Fdr\vec{F} \cdot d\vec{r}

F(r(t))r(t)=(costsint)(sint)+(3)(cost)+(t3)(1) \vec{F}(\vec{r}(t)) \cdot \vec{r}'(t) = (\cos t \sin t)(-\sin t) + (3)(\cos t) + (t^3)(1)

=costsin2t+3cost+t3 = -\cos t \sin^2 t + 3 \cos t + t^3

Step 4: Integrate with respect to tt

CFdr=0π(costsin2t+3cost+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:

=0πcostsin2tdt+0π3costdt+0πt3dt = \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=sintu = \sin t, then du=costdtdu = \cos t \, dt. The limits change from 000 \to 0 and π0\pi \to 0.

    0πsin2tcostdt=[sin3t3]0π=00=0 \int_0^{\pi} -\sin^2 t \cos t \, dt = \left[ -\frac{\sin^3 t}{3} \right]_0^{\pi} = 0 - 0 = 0
  • Second integral:

    0π3costdt=3[sint]0π=3(00)=0 \int_0^{\pi} 3 \cos t \, dt = 3 [\sin t]_0^{\pi} = 3(0 - 0) = 0
  • Third integral:

    0πt3dt=[t44]0π=π440=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

CFdr=π44 \int_C \vec{F} \cdot d\vec{r} = \frac{\pi^4}{4}

Q9. 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)=yzx2f(x,y,z) = yz - x^2
b. CFdr\int_C \vec{F} \cdot d\vec{r}, where F=2xy,2z,yz\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 v=P1P0=1(2),21,10=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 0t10 \le t \le 1:

r(t)=P0+tv=2,1,0+t1,1,1=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:

r(t)=1,1,1 \vec{r}'(t) = \langle 1, 1, 1 \rangle

The magnitude of the derivative is:

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

Therefore, the differential arc length is ds=3dtds = \sqrt{3} \, dt, and the differential vector is dr=1,1,1dtd\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)=yzx2f(x,y,z) = yz - x^2.

Step 1: Substitute the parametrization into ff

f(r(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)(44t+t2) = (t + t^2) - (4 - 4t + t^2)

=t+t24+4tt2 = t + t^2 - 4 + 4t - t^2

=5t4 = 5t - 4

Step 3: Set up the integral

Cf(x,y,z)ds=01(5t4)3dt \int_C f(x,y,z) \, ds = \int_0^1 (5t - 4) \sqrt{3} \, dt

Step 4: Evaluate

=301(5t4)dt=3[5t224t]01 = \sqrt{3} \int_0^1 (5t - 4) \, dt = \sqrt{3} \left[ \frac{5t^2}{2} - 4t \right]_0^1

=3(524)=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 CFdr\int_C \vec{F} \cdot d\vec{r} where F=2xy,2z,yz\vec{F} = \langle 2x-y, 2z, y-z \rangle.

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

F(r(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 F\vec{F}

  • xx-component: 2(2+t)(1+t)=4+2t1t=t52(-2+t) - (1+t) = -4 + 2t - 1 - t = t - 5
  • yy-component: 2t2t
  • zz-component: 1+tt=11 + t - t = 1 So, F(r(t))=t5,2t,1\vec{F}(\vec{r}(t)) = \langle t - 5, 2t, 1 \rangle.

Step 3: Compute the dot product Fr(t)\vec{F} \cdot \vec{r}'(t)

F(r(t))r(t)=t5,2t,11,1,1 \vec{F}(\vec{r}(t)) \cdot \vec{r}'(t) = \langle t - 5, 2t, 1 \rangle \cdot \langle 1, 1, 1 \rangle

=(t5)(1)+(2t)(1)+(1)(1) = (t - 5)(1) + (2t)(1) + (1)(1)

=t5+2t+1=3t4 = t - 5 + 2t + 1 = 3t - 4

Step 4: Set up the integral

CFdr=01(3t4)dt \int_C \vec{F} \cdot d\vec{r} = \int_0^1 (3t - 4) \, dt

Step 5: Evaluate

=[3t224t]01 = \left[ \frac{3t^2}{2} - 4t \right]_0^1

=(324)0=3282=52 = \left( \frac{3}{2} - 4 \right) - 0 = \frac{3}{2} - \frac{8}{2} = -\frac{5}{2}

Final Answer

a. C(yzx2)ds=013(5t4)dt=332\displaystyle \int_C (yz - x^2) \, ds = \int_0^1 \sqrt{3}(5t - 4) \, dt = -\frac{3\sqrt{3}}{2}
b. CFdr=01(3t4)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 F=3+2xy,x23y2\vec{F} = \langle 3+2xy, x^2-3y^2 \rangle.
a. Show that F\vec{F} is conservative, then find a potential function for F\vec{F}.
b. Evaluate CFdr\int_C \vec{F} \cdot d\vec{r}, where CC is given by r(t)=etsint,etcost,0tπ\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 F\vec{F} is conservative and find a potential function

Let F=P,Q\vec{F} = \langle P, Q \rangle, where P=3+2xyP = 3+2xy and Q=x23y2Q = x^2-3y^2.
For F\vec{F} to be conservative on a simply connected domain (like R2\mathbb{R}^2), the condition Py=Qx\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x} must hold.

Calculate the partial derivatives:

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

Qx=x(x23y2)=2x \frac{\partial Q}{\partial x} = \frac{\partial}{\partial x}(x^2-3y^2) = 2x

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

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

  1. fx=3+2xy\frac{\partial f}{\partial x} = 3+2xy
  2. fy=x23y2\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:

fy=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)=x23y2 x^2 + g'(y) = x^2 - 3y^2

g(y)=3y2 g'(y) = -3y^2

Integrate with respect to yy:

g(y)=3y2dy=y3+C g(y) = \int -3y^2 \, dy = -y^3 + C

Thus, the potential function is:

f(x,y)=3x+x2yy3+C f(x,y) = 3x + x^2y - y^3 + C

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


b. Evaluate CFdr\int_C \vec{F} \cdot d\vec{r}

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

CFdr=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 r(t)=etsint,etcost\vec{r}(t) = \langle e^t \sin t, e^t \cos t \rangle for 0tπ0 \le t \le \pi.

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

r(0)=e0sin0,e0cos0=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):

r(π)=eπsinπ,eπcosπ=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+x2yy3f(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:

CFdr=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. F\vec{F} is conservative because Py=Qx=2x\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x} = 2x. A potential function is f(x,y)=3x+x2yy3f(x,y) = 3x + x^2y - y^3.
b. CFdr=e3π+1\displaystyle \int_C \vec{F} \cdot d\vec{r} = e^{3\pi} + 1

Q11. Conservative Vector Field

The vector field F=2xyz,x2+2y,1x\vec{F} = \langle 2xy-z, x^2+2y, 1-x \rangle is conservative.
a. Find a potential function for F\vec{F}.
b. Using the potential function from (a) evaluate CFdr\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 F\vec{F}

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

fx=2xyz,fy=x2+2y,fz=1x \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)=(2xyz)dx=x2yxz+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:

    fy=y(x2yxz+g(y,z))=x2+gy \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 fy=x2+2y\frac{\partial f}{\partial y} = x^2 + 2y, we get:

    x2+gy=x2+2y    gy=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)=2ydy=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)=x2yxz+y2+h(z) f(x, y, z) = x^2y - xz + y^2 + h(z)
  4. Differentiate with respect to zz and compare:

    fz=z(x2yxz+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 fz=1x\frac{\partial f}{\partial z} = 1 - x, we get:

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

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

    Combining all parts, the potential function is:

    f(x,y,z)=x2yxz+y2+z+C f(x, y, z) = x^2y - xz + y^2 + z + C

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


b. Evaluate CFdr\int_C \vec{F} \cdot d\vec{r}

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

CFdr=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=46+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=02+0+2=0 f(1, 0, 2) = (1)^2(0) - (1)(2) + (0)^2 + 2 = 0 - 2 + 0 + 2 = 0

Calculate the difference:

CFdr=20=2 \int_C \vec{F} \cdot d\vec{r} = 2 - 0 = 2

Final Answer

a. A potential function is f(x,y,z)=x2yxz+y2+zf(x, y, z) = x^2y - xz + y^2 + z.
b. CFdr=2\displaystyle \int_C \vec{F} \cdot d\vec{r} = 2

Q12. Green’s Theorem

Use Green’s Theorem to compute the integral Cxy3dx+x2y2dy\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:

CPdx+Qdy=D(QxPy)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 Cxy3dx+x2y2dy\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:

Qx=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:

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

4. Determine the Integrand

Subtract the partial derivatives:

QxPy=2xy23xy2=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:

0x2,0y3 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=0302xy2dxdy \iint_D (-xy^2) \, dA = \int_0^3 \int_0^2 -xy^2 \, dx \, dy

First, evaluate the inner integral with respect to xx:

02xy2dx=y2[x22]02=y2(420)=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:

032y2dy=2[y33]03=2(2730)=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

Cxy3dx+x2y2dy=18 \oint_C xy^3 \, dx + x^2y^2 \, dy = -18

Q13. Green’s Theorem

Use Green’s Theorem to evaluate C(3yesinx)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:

CPdx+Qdy=D(QxPy)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(3yesinx)dx+(7x+y4+1)dy\oint_C (3y - e^{\sin x}) \, dx + (7x + \sqrt{y^4+1}) \, dy, we identify:

P(x,y)=3yesinx,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:

Qx=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:

Py=y(3yesinx)=30=3 \frac{\partial P}{\partial y} = \frac{\partial}{\partial y}(3y - e^{\sin x}) = 3 - 0 = 3

Note that the complicated terms esinxe^{\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:

QxPy=73=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:

D4dA=4DdA \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(3yesinx)dx+(7x+y4+1)dy=36π \oint_C (3y - e^{\sin x}) \, dx + (7x + \sqrt{y^4+1}) \, dy = 36\pi

Related Content