Math 221 Examination 2 Spring 2013 Several Variable Calculus Instructions These problems should be viewed as essay questions. Before making a calculation, you should explain in words what your strategy is. Please write your solutions on your own paper. Each of the 10 problems counts for 10 points. 1 πβ2 1. Evaluate the iterated integral ∫0 ∫0 π₯ cos(π₯π¦) dπ¦ dπ₯. Solution. Observe that π₯ cos(π₯π¦) is the π¦-partial derivative of sin(π₯π¦). Then 1 πβ2 ∫0 ∫0 πβ2 π₯ cos(π₯π¦) dπ¦ dπ₯ = ∫0 |π¦=1 sin(π₯π¦) | dπ₯ |π¦=0 πβ2 = ∫0 (sin(π₯) − 0) dπ₯ |πβ2 = − cos(π₯) | |0 = − cos(πβ2) + cos(0) = 1. 2. Describe the solid whose volume is given by the spherical-coordinate triple integral π π ∫0 ∫0 ∫1 2 π2 sin(π) dπ dπ dπ. (You do not need to evaluate the integral.) Solution. Notice that π2 sin(π) dπ dπ dπ is dπ , the volume element, expressed in spherical coordinates. Since π goes from 1 to 2, the solid is contained in the shell between a sphere of radius 1 and a sphere of radius 2. The angle π goes from 0 to π, its maximum range, so this angle does not restrict the solid. The angle π goes from 0 to π, half its maximum range, so the solid lies in the half-space where π¦ > 0. Thus the solid is a hemisphere of radius 2 with a concentric hemisphere of radius 1 removed. The problem does not ask for the value of the integral. But that value works out to 14πβ3. March 28, 2013 Page 1 of 6 Dr. Boas Math 221 Examination 2 Spring 2013 Several Variable Calculus π¦ π₯ππ¦ dπ΄, where π· is the region in the first β¬π· quadrant bounded by the line π¦ = 0, the line π₯ = 1, and the parabola π¦ = π₯2 . 3. Evaluate the double integral π₯ Solution. The convenient method is to integrate with respect to π¦ first: π₯2 1 π¦ β¬π· π₯π dπ΄ = π₯ππ¦ dπ¦ dπ₯ ∫0 ∫0 1 |π¦=π₯ = π₯π | dπ₯ |π¦=0 ∫0 1 ( ) 2 π₯ ππ₯ − 1 dπ₯ = ∫0 1 ) π’=π₯2 1( π’ π − 1 dπ’ = ∫0 2 ]1 1[ π’ = π −π’ 0 2 ] 1[ = (π − 1) − (1 − 0) 2 π−2 = . 2 2 π¦ 4. Find the volume of the solid bounded by the cylinder π₯2 + π¦2 = 1 and the planes π§ = 0 and π₯ + π§ = 2. Solution. One method is to use cylindrical coordinates. The variable π§ goes from 0 to 2 − π₯, or 2 − π cos(π). Since the equation π₯2 + π¦2 = 1 describes a circle of radius 1, the angle π is unrestricted, and π goes from 0 to 1. Here is the iterated integral: 2π ∫0 March 28, 2013 1 ∫0 ∫0 2−π cos(π) 2π π dπ§ dπ dπ = 1 (2 − π cos(π))π dπ dπ ∫0 ]1 2π [ 1 3 2 = π − π cos(π) dπ ∫0 3 0 ] 2π [ 1 = 1 − cos(π) dπ ∫0 3 = 2π. ∫0 Page 2 of 6 Dr. Boas Math 221 Examination 2 Spring 2013 Several Variable Calculus 2 π¦2 π¦ π (π₯, π¦, π§) dπ§ dπ₯ dπ¦ as an iterated integral 5. Rewrite the integral ∫0 ∫0 ∫0 in the order dπ₯ dπ¦ dπ§. Solution. The solid lies in the first octant (since all three variables start at 0). The solid lies under the parabolic cylinder π§ = π¦2 (with axis along the π₯axis) and between the plane π₯ = π¦ and the π¦π§ plane. Also the solid stops at the plane π¦ = 2. √ Consequently, the variable π₯ goes from 0 to π¦; then π¦ goes from π§ to 2, and π§ goes from 0 to 4 (since the equation π§ = π¦2 says that π§ = 4 when π¦ = 2). Here is the iterated integral: 4 2 ∫0 ∫√π§ ∫0 π¦ π (π₯, π¦, π§) dπ₯ dπ¦ dπ§. 6. Set up an integral for the surface area of the part of the paraboloid π§ = π₯2 +π¦2 that lies between the plane π§ = 1 and the plane π§ = 4. (You do not need to evaluate the integral.) Solution. The surface area element is √ ( )2 ( )2 √ ππ§ ππ§ + = 1 + (2π₯)2 + (2π¦)2 1+ ππ₯ ππ¦ √ = 1 + 4(π₯2 + π¦2 ). Since π§ goes from 1 to 4, the surface lies over the region in the π₯π¦-plane between the circle 1 = π₯2 +π¦2 and the circle 4 = π₯2 +π¦2 (which has radius 2). Because of the circular symmetry, it is convenient to write the integral in polar coordinates: 2π 2√ 1 + 4π2 π dπ dπ. ∫0 ∫1 The problem does not ask)for the value of the integral. But the value works ( √ √ π out to 17 17 − 5 5 . 6 March 28, 2013 Page 3 of 6 Dr. Boas Math 221 Examination 2 Spring 2013 Several Variable Calculus π¦ π₯ −1 7. Let π· be the square with vertices (1, 0), (0, 1), (−1, 0), and (0, −1). Rewrite the double integral β¬π· (π₯ + π¦)5 dπ΄ as an integral with respect to dπ’ dπ£, where π’ = π₯ + π¦ and π£ = π₯ − π¦. (You do not need to evaluate the integral.) −1 Solution. Compute the Jacobian: | ππ’ | π(π’, π£) || ππ₯ = π(π₯, π¦) || ππ£ | ππ₯ | ππ’ || | 1|| ππ¦ || = ||1 ππ£ || |1 −1|| = −2. | | ππ¦ || The area-magnification factor for the change of variables is the absolute value of the Jacobian, so dπ’ dπ£ = 2 dπ₯ dπ¦, or dπ₯ dπ¦ = 21 dπ’ dπ£. The side of the square in the first quadrant of the π₯π¦-plane is part of the line π₯ + π¦ = 1, which turns into the equation π’ = 1. Similarly, the parallel side in the third quadrant turns into the equation π’ = −1. The side in the fourth quadrant is part of the line π₯ − π¦ = 1, which corresponds to π£ = 1, and the parallel side in the second quadrant corresponds to π£ = −1. Consequently, the new integral in the π’π£-plane is 1 1 ∫−1 ∫−1 1 5 π’ dπ’ dπ£. 2 The problem does not ask for the value of the integral. But the value is 0 by symmetry! 8. Find the work done by the force field πΉβ (π₯, π¦) = π¦2 π€Μ + 2π₯π¦ π₯Μ on a particle that moves in a straight line from the point (1, 2) to the point (5, 1). Solution. One method is to observe that πΉβ (π₯, π¦) = ∇(π₯π¦2 ). Therefore the work integral ∫ πΉβ ⋅ dβπ equals |(5,1) π₯π¦2 | = 5 − 4 = 1. |(1,2) Another method is to parametrize the line via π₯ = 1 + 4π‘ π¦=2−π‘ March 28, 2013 Page 4 of 6 0 ≤ π‘ ≤ 1. Dr. Boas Math 221 Examination 2 Spring 2013 Several Variable Calculus Then dπ₯ = 4 dπ‘ and dπ¦ = − dπ‘, so ∫ πΉβ ⋅ dβπ = = π¦2 dπ₯ + 2π₯π¦ dπ¦ ∫ 1 [ 1 ( 2 ) 12π‘ − 30π‘ + 12 dπ‘ ∫0 = ] (2 − π‘)2 (4) + 2(1 + 4π‘)(2 − π‘)(−1) dπ‘ ∫0 = 4 − 15 + 12 = 1. π¦ dπ when the parametric equations of πΆ are ∫πΆ π₯ = π‘2 and π¦ = 2π‘, where 0 ≤ π‘ ≤ 1. 9. Evaluate the line integral Solution. The arc length element dπ equals √ ( )2 ( )2 √ √ ( )2 dπ¦ dπ₯ + dπ‘ = 2π‘ + 22 dπ‘ = 2 π‘2 + 1 dπ‘. dπ‘ dπ‘ Therefore 1 ∫πΆ π¦ dπ = ∫0 √ )3β2 |1 4 [ 3β2 ] 4(2 4π‘ π‘2 + 1 dπ‘ = π‘ +1 2 −1 . |= |0 3 3 10. What does it mean to say that a vector field πΉβ is a conservative vector field? Solution. A conservative vector field is the same thing as a gradient vector field: there exists a function π such that πΉβ = ∇π . March 28, 2013 Page 5 of 6 Dr. Boas Math 221 Examination 2 Spring 2013 Several Variable Calculus Optional bonus problem for extra credit Find the volume of an egg whose eggshell has the equation π₯ 2 π¦2 π§ 2 + + = 1. 8 5 3 Solution. The problem asks for βπ· dπ , where π· is the region inside the surface. √ √ √ One method√ is to change variables via π₯ = π’ 8 and π¦ = π£ 5 and π§ = π€ 3. Then dπ₯ dπ¦ dπ§ = 120 dπ’ dπ£ dπ€, and the equation of the surface in the new coordinates becomes π’2 + π£2 + π€2 = 1, a sphere of radius 1. Since the volume of a ball of radius π equals 43 ππ3 , the volume of a ball of radius 1 equals 43 π. Accordingly, βπ· ( ) √ dπ = 120 34 π , or √ 8π 30 . 3 (If you forgot the formula for the volume of a ball of radius 1, then you could compute it in spherical coordinates as 2π ∫0 1 π ∫0 ∫0 π2 sin(π) dπ dπ dπ, which works out to 4πβ3.) March 28, 2013 Page 6 of 6 Dr. Boas