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Course: M 151, Fall 2009
School: Texas A&M
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Practice M151B Problems for Final Exam Calculators will not be allowed on the exam. Unjustified answers will not receive credit. On the exam you will be given the following identities: n(n + 1) ; k= 2 k=1 n n(n + 1)(2n + 1) k = ; 6 k=1 2 n n k3 = k=1 n(n + 1) 2 2 . 1. Compute each of the following limits: 1a. x2 lim - x2 x . + 3x - 10 1 1b. x0 lim xesin( x ) . 1c. x sin x . x0 (1 - ex )2 lim x 1d....

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Practice M151B Problems for Final Exam Calculators will not be allowed on the exam. Unjustified answers will not receive credit. On the exam you will be given the following identities: n(n + 1) ; k= 2 k=1 n n(n + 1)(2n + 1) k = ; 6 k=1 2 n n k3 = k=1 n(n + 1) 2 2 . 1. Compute each of the following limits: 1a. x2 lim - x2 x . + 3x - 10 1 1b. x0 lim xesin( x ) . 1c. x sin x . x0 (1 - ex )2 lim x 1d. lim [(x + 1)1/3 - x1/3 ]. ab. Show that 1e. The geometric mean of two positive real numbers a and b is defined as ab = lim ( x a1/x + b1/x x ) . 2 2a. Find a value for c that makes the given function continuous at all points. f (x) = sin x , x c, x=0 . x=0 2b. Determine whether or not your function from (2a) is differentiable at x = 0. If it is differentiable at this point, compute its derivative there. 3. Find an equation for the line that is tangent to the graph of f (x) = at the point x = 0. 4. Suppose the angle of elevation of the Sun is decreasing at a rate of .25 rad/hr. How fast is the shadow cast by a 400 ft tall building increasing when the angle of elevation of the Sun is ? 6 1 xex 1 + x2 5. Suppose f (x) is continuous on the interval [a, b] and differentiable on the interval (a, b). Show that if f (x) = x for all x (a, b), then there exists some value c (0, 1) so that f (b) - f (a) = c(b - a). 6. Let f (x) = x1/3 (x + 3)2/3 , 6a. Locate the critical points of f and determine the intervals on which f is increasing and the intervals on which f is decreasing. 6b. Locate the possible inflection points for f and determine the intervals on which f is concave up and the intervals on which it is concave down. 6c. Evaluate f at the critical points and at the possible inflection points, and determine the boundary behavior of f by computing limits as x . - < x < . 6d. Use your information from Parts a-c to sketch a graph of this function. 7. Find the side-lengths that maximize the area of an isosceles triangle with given perimeter P = 10. (An isosceles triangle is a triangle with two sidelengths equal.) 8. Find all fixed points for the recursion equation 1 3 an+1 = an + . 4 an 1 Sketch a graph of the function f (a) = 3 a+ a , and use the method of cobwebbing to determine 4 1 whether or not one of these fixed points will be achieved from the starting value a0 = 2 . 9. Find all fixed points for the recursion equation xt+1 = 1 + 2 xt and determine whether or not each is asymptotically stable or unstable. 10. Suppose a function f (x) is continuous on the interval [0, 1] and that you are given the following table of values: x f (x) 1/8 1/2 3/8 1/3 5/8 -1 7/8 -2 Table 1: Values of f (x) for Problem 1. Use an appropriate Riemann sum to approximate 11. Use the method of Riemann sums to evaluate 2 1 0 f (x)dx. x + x2 dx. 1 2 12. Evaluate the following indefinite integrals. 12a. ex cos(ex )dx. 12b. 12b. cos-1 xdx. 13. Evaluate the following definite integrals. 13a. 1 3 x dx 1+x 4 x2 dx. 1 + x3 13b. 0 x sec2 xdx. 16. Suppose the base of a certain solid is the region in the xy-plane between the line y = x and the parabola y = x2 . Find the volume of the solid created if every cross section is a right isosceles triangle with hypotenuse in the xy-plane perpendicular to the x-axis. 15. Find the volume obtained when the region between the graphs of y = ex and y = e-x , x [0, 2], is rotated about the x-axis. 14. Find the area of the region bounded by the graphs of y = x4 and y = 20 - x2 . Solutions 1a. We have x2 lim - x2 where we have observed that x - 2 is negative for x to the left of 2. -|x|e xesin( x ) |x|e. We have x0 1 x x = lim = -, - (x - 2)(x + 5) + 3x - 10 x2 1b. We apply the Squeeze Theorem in this case, using the inequality lim -|x|e = lim |x|e = 0, x0 and so according to the Squeeze Theorem x0 lim xesin( x ) = 0. 3 1 1c. We apply L'Hospital's Rule twice, sin x + x cos x sin x + x cos x x sin x = lim = lim x )2 x )(-ex ) x0 2(1 - e x0 x0 (1 - e 2e2x - 2ex 2 cos x - x sin x = lim = 1. x0 4e2x - 2ex lim 1d. This limit has the indeterminate form - , so the first thing we do is rearrange it 0 into an expression with the form 0 . We have 1 lim (x + 1)1/3 - x1/3 = lim x1/3 [(1 + )1/3 - 1] x x x 1 1 1 1 (1 + x )1/3 - 1 (1 + x )-2/3 (- x2 ) 3 = lim = lim x x x-1/3 - 1 x-4/3 3 1 -2/3 1 = 0. = lim (1 + ) x x x2/3 1e. We observe that this limit has the general form 1 , and so we can apply L'Hospital's rule. We have x lim ( a1/x +b1/x a1/x +b1/x x a1/x + b1/x x ) ) 2 2 = lim ex ln( ) = lim eln( x x 2 = elimx x ln( In order to compute this limit, we write ln( a a1/x + b1/x lim x ln( ) = lim x x 2 = lim x a1/x 1/x +b1/x a1/x +b1/x ) 2 . 2 1 x ) = 1 1 (a1/x ln a + b1/x ln b) = (ln a + ln b), 1/x +b 2 0 as x . The limit is 1 1/2 = e 2 ln(ab) = eln(ab) = ab. 1 x 2 ( 1 a1/x (ln a)(- x12 ) a1/x +b1/x 2 lim x - x12 + 1 b1/x (ln b)(- x12 )) 2 where in this last step we have used that e 2 (ln a+ln b) 2a. Since 1 sin x = 1, x0 x we can make this function continuous at all points by choosing c = 1. lim 2b. Since the function is separately defined at x = 0, we must proceed from the definition of differentiation. We compute f (0) = lim sin h -1 f (0 + h) - f (0) = lim h h0 h0 h h cos h - 1 - sin h sin h - h = lim = lim = 0, = lim h0 h0 h0 h2 2h 2 4 where the last two steps both used L'Hospital's rule. We conclude that this function is differentiable at x = 0, and that f (0) = 0. 3. First, f (x) = (1 + x2 )(ex + xex ) - xex (2x) f (0) = 1, (1 + x2 )2 which is the slope of the tangent line. Using f (0) = 0 and the general point-slope form y - f (a) = f (a)(x - a), we conclude y = x. 4. First, observe that what we know is d = -.25 rad/hr and what we want to know is dt where x is the length of the shadow (see the diagram). dx , dt We see that the relation between and x is tan = 400 . x Upon taking a derivative of this equation with respect to t, we obtain sec2 400 dx d =- 2 , dt x dt 1 cos2 6 where we can now fix = , so that sec2 = 6 Combining these observations, we have = 1 3 4 = 4 , while x = 3 400 tan 6 = 400 3. x2 d 4 dx =- sec2 = -3(400)(-.25) = +400 dt ft/hr. 400 dt 6 3 5. According to the Mean Value Theorem there exists some value c (a, b) so that f (b) - f (a) = f (c). b-a In this case f (c) = c, and so we conclude f (b) - f (a) = c f (b) - f (a) = c(b - a). b-a 5 6a. The derivative of f (x) is f (x) = x+1 , x2/3 (x + 3)1/3 from which we find the critical points x = -3, -1, 0. We see that f is increasing on (-, -3] [-1, ) and decreasing on [-3, -1]. 6b. The second derivative of f (x) is 2 , + 3)4/3 f (x) = - x5/3 (x 6c. Evaluating f at the critical points, possible inflection points, and at the endpoints, we have: f (-3) = 0 f (-1) = - 22/3 f (0) = 0 x- from which we find that the possible inflection points are x = 0, -3. We see that f is concave up on (-, -3) (-3, 0) and concave down on (0, ). lim x1/3 (x + 3)2/3 = - x lim x1/3 (x + 3)2/3 = + . 6d. Your plot should look something like this: 7. Let y denote the length of the sides of equal length, and let x denote the length of the side between them. Then the perimeter is 1 10 = 2y + x y = 5 - x. 2 6 By the Pythagorean Theorem, the height of such a triangle is h = area to be maximized is 1 y 2 - 4 x2 , and so the 1 1 1 1 1 1 A = x y 2 - x2 A(x) = x (5 - x)2 - x2 = x 25 - 5x, 2 4 2 2 4 2 0 x 5. (The upper limit of 5 is clear both because a value of x larger than this would put a negative number under the radical, and because the single side cannot be more than half the perimeter.) In order to maximize A(x), we compute 25 - 15 x 2 4 . A (x) = 25 - 5x The critical values are x = 10 , 5, where we observe that x = 5 is also a boundary value. 3 Checking A(x) at the critical and boundary values, we find A(0) = 0 A( 5 10 )= 3 3 A(5) = 0. 25 25 = 3 3 3 10 3 We conclude that the maximum area is 3253 and the side-lengths are x = 1 5 - 2 ( 10 ) = 10 . That is, an equilateral triangle. 3 3 and y = 8. The fixed points solve 1 1 1 3 a = a + a = a2 = 4. 4 a 4 a We conclude that the fixed points are 2. In order to use cobwebbing, we must sketch a graph of the function 3 1 f (a) = a + . 4 a First, setting 1 3 f (a) = - 2 = 0, 4 a 2 2 we find that the critical points are a = 3 , 0. The function is increasing on (-, - 3 ] 2 2 2 [ 3 , ) and decreasing on [- 3 , 3 ]. Next, f (a) = 2 , a3 and so the only possible point of inflection is a = 0. The function is concave down on (-, 0) 7 and concave up on (0, ). Finally, 1 3 lim ( a + ) = - a- 4 a 2 f (- ) = - 3 3 1 3 lim ( a + ) = - x0- 4 a 3 1 lim+ ( a + ) = + x0 4 a 2 f( ) = 3 3 3 1 lim ( a + ) = a- 4 a The plot of this function and the cobwebbing are depicted below. We conclude n lim an = 2. 9. In order to find the fixed points, we solve 2 x=1+ , x which becomes (upon multiplication by x) x2 - x - 2 = (x - 2)(x + 1) = 0, 2 and the fixed points are x = -1, 2. In order to check for stability we set f (x) = 1 + x , and compute 2 f (x) = - 2 . x 8 We have f (-1) = - 2 -1 is unstable 1 f (2) = - 2 is stable. 2 10. Since no value for f (x) is given at either x = 0 or at x = 1, we cannot take a Riemann sum with left or right endpoints. We see, however, that the values of x are precisely the midpoints 1 1 of the subintervals in the partition P = [0, 4 , 2 , 3 , 1]. The most reasonable Riemann sum is 4 4 f (ck )xk , k=1 where the ck are the interval midpoints. That is, 1 13 1 1 f (ck )xk = ( + - 1 - 2) = - . 2 3 4 24 k=1 11. In this case x = n b-a n 4 = 2-1 n 1 = n , and we use right endpoints xk = 1 + kx. We have An = k=1 n [(1 + kx) + (1 + kx)2 ]x k k2 1 k ) + (1 + 2 + 2 )] = [(1 + n n n n k=1 1 = n 1 1+ 2 n k=1 n 1 k+ n k=1 n 2 1+ 2 n k=1 n 1 k+ 3 n k=1 n n k2 k=1 1 n(n + 1) 2 n(n + 1) 1 n(n + 1)(2n + 1) = 1+...

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Texas A&M - M - 151
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HPH !U!czPP0PxPPPU7cg rr5cPuUPscuvvggoc2cSrzvugcPPvcg PP7PPgPP7P cSS c PPgPP7PPg P c 7PPgPP7PPg UcPu0PcUgWPvcr2ugc PPec PPgPP7PPgPP 7PducPc2cSrF r7g 2uFg
University of Toronto - STA - 247
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University of Toronto - STA - 247
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University of Toronto - STA - 247
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CSU East Bay - STATISTICS - 39104910
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GWU - SEAS - 211
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CSU East Bay - STATISTICS - 39104910
Statistics 3900/4950 Regression Project Find a dataset of interest to you that can be analyzed using multiple linear regression techniques. The data set should have one quantitative dependent variable Y and at least 2 independent quantitative variables X.
Princeton - PHYS - 301
1 Physics 301: Solutions to Homework No. 12, John D. Naud 1. The thermal diusivity, D is given by D = K/C, where K is the thermal conductivity and C is the heat capacity per unit volume. Consider the element Selenium (Se) which is an insulating solid at r
BU - MATH - 242
MA 242 Extra problem on row equivalence Using the handout distributed in class on September 6: (a) For each system of equations, form its augmented matrix.September 8, 2006(b) Group these ten matrices according to row equivalence. In other words, two ma
Princeton - PHYS - 301
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Princeton - PHYS - 301
Physics 30116-Dec-1999 24-1To Do Have a Good Holiday, find some time to study a little physics, and come back from break relaxed, refreshed, and ready to go! The 3R's of higher education?The Diffusion of a One Dimensional Bump When we looked at a one d
Princeton - PHYS - 301
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Princeton - PHYS - 301
Physics 301Homework No. 12Due: NeverH12-11. You may recall that I mentioned the (thermal) diffusivity for an insulating solid might be the speed of sound in the solid times the distance between atoms. Look up the thermal conductivity, specific heat (y
Princeton - PHYS - 301
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Princeton - PHYS - 301
Physics 30114-Dec-1999 23-1Reading K&amp;K Chapter 15.High Vacuum Statistical Mechanics As weve mentioned, when the pressure is less than about a millionth of an atmosphere at room temperature, the mean free path becomes long enough that its comparable to
Princeton - PHYS - 301
1 Physics 301: Solutions to Homework No. 11, John D. Naud 1.(a) Let p0 be the momentum of one of the spheres before collision. Since the total momentum is zero in the center of mass frame the other sphere must have momentum -p0 before collision. The momen
Princeton - PHYS - 301
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Princeton - PHYS - 301
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Princeton - PHYS - 301
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Princeton - PHYS - 301
Physics 301Homework No. 11Due 16-Dec-1999 (Thursday)H11-11. Some fun with cross sections. (a) Consider elastic scattering of two hard spheres of radius a as in the lecture notes, but this time in the center of mass frame. Show that d = a2 , d so the s