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This is the Solved Exam of Calculus One for Engineers which includes Functions, Electronic Devices, Different Coordinate System, Domains, Average Rate, Change, Interval, Instantaneous Rate, Tangent Line etc. Key important points are: Continuous, Justification, Riemann Sum, Evaluate, Answer, Justification, Decreasing, Intervals, Values, Local Minimum Values
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y =
∫ (^) x^3
x
t^3 t^2 + 1 dt
=
∫ (^) x 3
0
t^3 t^2 + 1 dt −
∫ (^) x
0
t^3 t^2 + 1 dt
dy dx = d dx
∫ (^) x^3
0
t^3 t^2 + 1 dt − d dx
∫ (^) x
0
t^3 t^2 + 1 dt
= (x^3 )^3 (x^3 )^2 + 1 (3x^2 ) − x^3 x^2 + 1
= 3 x^11 x^6 + 1
x^3 x^2 + 1 (b) Use the product rule. y = x ln(x^2 + 10) y′^ = x ·
x^2 + 10 (2x) + ln(x^2 + 10)
2 x^2 x^2 + 10 + ln(x
(c) Use logarithmic differentiation.
y =
9 x − 1 (2x^3 + 1)^2 (x − 2)^3
ln y = ln (9x^ −^ 1)
1 / 2 (2x^3 + 1)^2 (x − 2)^3 = ln(9x − 1)^1 /^2 − ln(2x^3 + 1)^2 − ln(x − 2)^3 =
ln(9x − 1) − 2 ln(2x^3 + 1) − 3 ln(x − 2) 1 y
dy dx
9 x − 1
2 x^3 + 1 (6x^2 ) − 3 · 1 x − 2 =
2(9x − 1)
12 x^2 2 x^3 + 1
x − 2
dy dx =
9 x − 1 (2x^3 + 1)^2 (x − 2)^3
2(9x − 1) −^
12 x^2 2 x^3 + 1 −^
x − 2
dx =^5 3
√du u =
u−^1 /^2 du
=
· 2 u^1 /^2 + C
=
x^3 − 2 + C
(b) The function f (x) = x
(^6) sin x x^2 + 4 is odd because
f (−x) = (−x)^6 sin(−x) (−x)^2 + 4
x^6 (− sin x) x^2 + 4 = − x
(^6) sin x x^2 + 4 = −f (x).
Since
∫ (^) a
−a
f (x) dx = 0 for any odd function f , then
∫ (^3)
− 3
x^6 sin x x^2 + 4 dx = 0.
(c) Let u = 3x − 1 ⇒ x = (u + 1)/ 3 , du = 3 dx ⇒ du/3 = dx. ∫ x
3 x − 1 dx =
u + 1 3
u du 3 =
(u^3 /^2 + u^1 /^2 ) du
=
u^5 /^2 +
u^3 /^2
(3x − 1)^5 /^2 +
(3x − 1)^3 /^2 + C
(d) Let u = 3x − 2 , du = 3 dx. The u-limits are − 5 to − 2. ∫ (^0)
− 1
3 dx 3 x − 2
− 5
du u = ln |u|
− 5
= ln 2 − ln 5 = ln
(e) Let u = sec 2θ, du = 2 sec 2θ tan 2θ dθ. ∫ sec^2 2 θ tan 2θ dθ =^1 2
u du
=
u^2 2
sec^2 2 θ + C
Alternate solution: Let u = tan 2θ, du = 2 sec^2 2 θ dθ. ∫ sec^2 2 θ tan 2θ dθ =
u du
=
u^2 2
tan^2 2 θ + C
(Note that tan^2 2 θ + 1 = sec^2 2 θ.)
(c) False. Let u = −x, du = −dx. Then
∫ (^) b
a
f (−x) dx =
∫ (^) −b
−a
−f (u) du.
(d) False. (^) nlim→∞
∑^ n
i=
2 i n
n
0
x dx =
, where ∆x =
n and
xi = 2 i n
. The integral 2
0
x dx =
∑^ n i=
i n
n
∑^ n i=
i^2 n^3
= 1 n^3
∑^ n i=
i^2 = 1 n^3 · n(n^ + 1)(2n^ + 1) 6
= (n^ + 1)(2n^ + 1) 6 n^2 = 2 n
(^2) + 3n + 1 6 n^2
(b) (^) lim n→∞ Rn^ =^ nlim→∞
2 n^2 + 3n + 1 6 n^2 (divide by n^2 )
= (^) nlim→∞
2 + (^) n^3 + (^) n^12 6
(c) A definite integral is a limit of Riemann sums:
∫ (^) b
a
f (x) dx =
nlim→∞
∑^ n i=
f (xi) ∆x, where ∆x = b − a n and xi = a + i∆x.
For the given sum, (^) nlim→∞
∑^ n
i=
i n
n
0
x^2 dx , where ∆x =
n and xi = i n
x 2 = x 1 − f (x 1 ) f ′(x 1 )
x 3 = x 2 − f (x 2 ) f ′(x 2 ) = 1^ −^
0 =^ undefined Since f (x 2 ) = f (1) = 0, x = 1 is a root of f. Since f ′(x 2 ) = f ′(1) = 0, there is a horizontal tangent at the root.