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This is the Solved Exam of Calculus which includes Statement, Integral, Function, Graph, Right Hand Sums, Rectangles To Estimate, Definition, Derivative, Method Besides etc. Key important points are: Taylor Series, Centered, Integrated, Trigonometric Substitution, Solid of Revolution Generated, Represents The Volume, Revolving The Curve, Chart, Choices, Problem
Typology: Exams
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Name KEY Instructor Section No.
Student Number
Departmental Final Exam
Instructions:
For administrative use only:
Short Answer.
ln x dx = x ln x − x + C
∫ (^) π/ 2 0 sin^ x dx^ =^ −^ cos^ x|
π/ 2 0 = 0^ −^ (−1) = 1
tan x sec^2 x dx = 12 tan^2 x + C or 12 sec^2 x + C
2 2! +^
(2x)^3 3! +^...^ =^
n=
2 nxn n!
∫ (^) x 2 √ x^2 + 4
dx can be integrated using the trigonometric substitution x = 2 tan θ
0 2 πx
x^2 + 1 dx represents the volume of the solid of revolution generated
by revolving the curve y =
x^2 + 1 , x ∈ [ 0 , 3 ], about the y-axis.
Multiple Choice. Use the following chart to show your choices for Problems 7–13. Shade in your choice. Only this chart will be graded on these problems.
Problem 7 (a) (b) (d) (e) (f) (g) (h) (i) (j) Problem 8 (a) (b) (d) (e) (f) (g) (h) (i) (j) Problem 9 (a) (b) (c) (d) (f) (g) (h) (i) (j) Problem 10 (a) (b) (c) (d) (f) (g) (h) (i) (j) Problem 11 (b) (c) (d) (e) (f) (g) (h) (i) (j) Problem 12 (a) (b) (d) (e) (f) (g) (h) (i) (j) Problem 13 (a) (b) (c) (e) (f) (g) (h) (i) (j)
1
xp^
dx
(a) converges if 0 < p < 1 (b) converges if p = 1 (c) converges if p > 1
(d) diverges if p > 1 (e) diverges if p > 0 (f) diverges if p 6 = 1
(g) none of these
0 sin(x
(^2) ) dx is approximately
(to two digit accuracy)
(a) .96 (b) .43 (c) .31 (d) .29 (e) .12 (f).
ex^ cos x dx =
(a) ex^ sin x + C (b) ex^ cos x − ex^ sin x + C (c) ex^ sin x − ex^ sin 2x + C
(d) 12 ex^ sin x + 12 ex^ cos x + C (e) 2ex^ sin x − 2 ex^ cos x + C (f) none of the above
Answers to Problems 12 and 13 must be shaded in the chart on Page 1 to be counted.
Essay Problems Work Problems 14–24 as you would homework problems, showing your steps and justifying them.
1 − a^2 x^2 dx (a > 0). x = (^1) a sin θ, dx = (^1) a cos θ dθ,
1 − a^2 x^2 = cos θ =⇒ ∫ (^) √ 1 − a^2 x^2 dx =
cos θ · 1 a
cos θ dθ
=^1 a
cos^2 θ dθ
=
2 a
(1 + cos 2θ) dθ
=
2 a [θ^ +
2 sin 2θ] +^ C = 1 2 a
[θ + sin θ cos θ] + C
= 1 2 a
[sin−^1 (ax) + ax
1 − a^2 x^2 ] + C
s =
∫ (^) π/ 4
π/ 6
1 + cot^2 x dx =
∫ (^) π/ 4
π/ 6
csc x dx
= ln | csc x − cot x|
∣∣π/ 4 π/ 6 = ln(
2 − 1) − ln(2 −
∫ (^) π/ 2
0
sin^3 x cos^2 x dx.
∫ (^) π/ 2
0
sin^3 x cos^2 x dx =
∫ (^) π/ 2
0
sin^2 x cos^2 x sin x dx
∫ (^) π/ 2
0
(1 − cos^2 x) cos^2 x sin x dx
= −
1
(1 − u^2 )u^2 du [u = cos x, du = − sin x dx]
0
(u^2 − u^4 )du
=
3 u
5 u
5
1 0 =
Let r = 1.2 be the radius of the window. A horizontal strip a distance h below the diameter of the window has length l = 2
r^2 − h^2. Therefore the force on the window is
F =
∫ (^) r
0
wh · 2
r^2 − h^2 dh
= −w
r^2
u^1 /^2 du [u = r^2 − h^2 , du = − 2 hdh]
=^2 3
wu^3 /^2
r^2 0 =^2 3
wr^3 = 1. 152 w
∫ (^) x + 1 x^2 − 4 dx.
x + 1 x^2 − 4
x + 2
x − 2
=⇒ x + 1 = A(x − 2) + B(x + 2) = (A + B)x + 2(B − A) =⇒ A = 14 , B = 34.
Therefore ∫ x + 1 x^2 − 4
dx =
x + 2
x − 2
dx =^1 4
ln |x + 2| +^3 4
ln |x − 2 | + C
(a)
n=
nxn−^1
n=
nxn−^1 = d dx
n=
xn
= d dx
1 − x
(1 − x)^2
The geometric series converges on (− 1 , 1). At both –1 and 1, we get divergent series, so (− 1 , 1) is the interval of convergence.
(b)
n=
(−1)n^
x^3 n n!
∑^ ∞
n=
(−1)n^ x
3 n n!
n=
(−x^3 )n n!
= e−x^3.
This series converges for all x ∈ R.
nlim→∞ an^ =^ L^ ⇐⇒ ∀ >^0 ,^ ∃k^ ∈^ N^ :^ n > k^ =⇒ |an^ −^ L|^ < .
(b) Determine the limit (^) nlim→∞
1 + πn
)n (by any means).
nlim→∞
1 + π n
)n = exp
n^ lim→∞ n^ ln(1 +^ π n
= exp
n^ lim→∞
ln(1 + πn ) 1 /n
= exp
n^ lim→∞^ −(π/n
(^2) )/ ln(1 + π/n) − 1 /n^2
= exp
π (^) nlim→∞1 +^1 π/n
= eπ
Or use Theorem 117(5).
(b) Find the area inside the curve r = eθ/^2 and outside the circle r = 1 for 0 ≤ θ ≤ π.
A =
∫ (^) π 0
1 2 r^2 dθ^ −^
1 2 π^ =^
∫ (^) π 0
1 2 eθdθ^ −^
1 2 π^ =^
1 2 eθ|π 0 −^
1 2 π^ =^
1 2 eπ^ −^
1 2 −^
1 2 π.
(c) Find the slope of the polar curve r = eθ/^2 at the point [1, 0].
y = eθ/^2 sin θ =⇒ dy dθ
eθ/^2 sin θ + eθ/^2 cos θ =⇒ dy dθ
|θ=0 = 1;
x = eθ/^2 cos θ =⇒ dxdθ =^12 eθ/^2 cos θ − eθ/^2 sin θ =⇒ dxdθ |θ=0 =^12 ;
dy dx =^