

Study with the several resources on Docsity
Earn points by helping other students or get them with a premium plan
Prepare for your exams
Study with the several resources on Docsity
Earn points to download
Earn points by helping other students or get them with a premium plan
Material Type: Assignment; Class: Probability with Engrg Applic; Subject: Electrical and Computer Engr; University: University of Illinois - Urbana-Champaign; Term: Fall 2002;
Typology: Assignments
1 / 2
This page cannot be seen from the preview
Don't miss anything!


(1 − x)(1 + x + x^2 +... + xn−^1 ) = (1 + x + x^2 +... + xn−^1 ) − x(1 + x + x^2 +... + xn−^1 ) = (1 + x + x^2 +... + xn−^1 ) − (x + x^2 + x^3... + xn) = 1 − xn,
which establishes the desired equation. (Another way to prove the equation is by induction on n.) (b) Since limn→∞ xn^ = 0 under the assumption |x| < 1, taking the limit as n → ∞ in both sides of the equation in part (a) yields that 1 + x + x^2 +... = (^1) −^1 x.
2 u −^ 1 =^ e
g(u), or g(u) = ln( 2 u −^ 1) for 0^ < u <^ 2.
2 can be written in the form xn^ exp(−ax^2 ), where a = ln(1.001), n = 4.
The function xn^ exp(−ax^2 ) has local extrema at the points x = ±∞, 0 , ±
n/ 2 a. In this case n = 4 and
therefore the maxima occur at x = ±
n/ 2 a = ± 44 .7325 (as can be verified by differentiating once again and checking the sign of the result at the two points); the points x = 0, ±∞ represent minima. The maximum function value (at both maxima) is 5. 4188 × 105.
(b) If f (x) = x^4 (1.001)x
2 , the function converges to infinity as |x| → ∞. Thus, f (x) is not a maximum value
of f for any finite value of x. Incidentally, carrying out the differentiation gives us x = ±
− 2 / ln(1.001) as the other solutions, which is not possible since the quantity within the “
” sign is negative.
∫ (^1)
− 1
|x| dx =
− 1
−x dx +
0
x dx =
−x^2 2
0
− 1
x^2 2
1
0
(b) Substitute y = (1 − x^2 ). Then ∫ (^1)
0
x(1 − x^2 )^11 dx = −
1
y^11 dy =
0
y^11 dy =
(c) Integrate by parts twice: ∫ (^1)
0
x^2 e−xdx = −x^2 e−x|^10 +
0
2 xe−xdx
= −e−^1 +
0
2 xe−xdx
= −e−^1 − 2 xe−x|^10 +
0
2 e−xdx
= − 3 e−^1 +
0
2 e−xdx
= − 3 e−^1 + 2(1 − e−^1 ) = 2 − 5 e−^1 ≈ 0. 1602
(d) Notice that the integrand is an odd function and therefore it has to integrate to 0 over any interval that is symmetric about the origin. In particular, the integral over the whole real line is zero.
f (x^2 )
as 2x · g(x^2 ) exp
f (x^2 )
(d) False.
g(−x) dx = −f (−x) + C (minus sign missing.) (e) False. The antiderivative of g(x^2 /2) need not be related to f (x^2 /2) at all, as can be seen by differentiating both sides of (v). For example, take f (x) = ln(1 + x) to see this. (f) True only for positive functions f (x).
∫ (^1)
0
0
max(x, y) dx dy =
0
(∫ (^) y 0 y dx
dy +
0
1 y x dx
dy
0 y
(^2) dy + ∫^1 0
1 −y^2 2 dy^ =^
1 3 +^
1 3 =^
2
(b) f (x, y) = (x^2 + y^2 )−^4 , over the region D = {(x, y) : x^2 + y^2 > 1 }. Changing to polar coordinates (x = r cos θ, y = r sin θ), the above integral can be reduced to
∫ ∫
D
(x^2 + y^2 )−^4 =
1
∫ (^2) π
0
r−^8 · r drdθ = 2π
1
r−^7 dr = π/ 3 ,
where the two-dimensional differential dx dy transforms to r dr dθ.
|f ′′| over the interval is |f ′′(− 0 .5)| = 4. Therefore, we can take M = 4. (Any larger value of M would also work.) (c) Note that n ln(1 + a n ) = nf ( a n ) ≈ nP ( a n ) = a. That is, the limit is a. To do a more careful job, we can bound the rate of convergence as follows. If n ≥ 2 a then | a n | ≤ 0 .5 so Taylor’s Inequality with M = 4 yields
|n ln(1 +
a n
) − a| = n|f (
a n
a n
≤ n
a n
)^2 if n ≥ 2 a
2 a^2 n
(d) Using the hint,
a n
)n^ = exp(ln((1 +
a n
)n))
= exp(n ln(1 +
a n
(1) → exp(a)
The limit (1) is justified because the argument of the exp function converges as shown in part (c), and the exp function is continuous.