Solutions to Exercise Sheet 5

Σχετικά έγγραφα
3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

Section 8.3 Trigonometric Equations

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

Problem Set 3: Solutions

Areas and Lengths in Polar Coordinates

Homework 8 Model Solution Section

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

Areas and Lengths in Polar Coordinates

2 Composition. Invertible Mappings

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

Solution Series 9. i=1 x i and i=1 x i.

Matrices and Determinants

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with

Answer sheet: Third Midterm for Math 2339

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r(t) = 3cost, 4t, 3sint

Example Sheet 3 Solutions

derivation of the Laplacian from rectangular to spherical coordinates

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr

D Alembert s Solution to the Wave Equation

Differentiation exercise show differential equation

6.3 Forecasting ARMA processes

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Srednicki Chapter 55

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

1 String with massive end-points

Section 9.2 Polar Equations and Graphs

If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2

Parametrized Surfaces

ST5224: Advanced Statistical Theory II

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

Math 6 SL Probability Distributions Practice Test Mark Scheme

If we restrict the domain of y = sin x to [ π 2, π 2

Integrals in cylindrical, spherical coordinates (Sect. 15.7)

Probability and Random Processes (Part II)

Trigonometric Formula Sheet

Approximation of distance between locations on earth given by latitude and longitude

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

Second Order Partial Differential Equations

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

The Simply Typed Lambda Calculus

Homework 3 Solutions

Second Order RLC Filters

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Uniform Convergence of Fourier Series Michael Taylor

Math221: HW# 1 solutions

4.6 Autoregressive Moving Average Model ARMA(1,1)

Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee

EE512: Error Control Coding

Quadratic Expressions

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

Spherical Coordinates

Other Test Constructions: Likelihood Ratio & Bayes Tests

Partial Differential Equations in Biology The boundary element method. March 26, 2013

= λ 1 1 e. = λ 1 =12. has the properties e 1. e 3,V(Y

Inverse trigonometric functions & General Solution of Trigonometric Equations

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Section 7.6 Double and Half Angle Formulas

Differential equations

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2

Trigonometry 1.TRIGONOMETRIC RATIOS

w o = R 1 p. (1) R = p =. = 1

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is

Statistical Inference I Locally most powerful tests

Variational Wavefunction for the Helium Atom

Problem 3.1 Vector A starts at point (1, 1, 3) and ends at point (2, 1,0). Find a unit vector in the direction of A. Solution: A = 1+9 = 3.

The Pohozaev identity for the fractional Laplacian

5.4 The Poisson Distribution.

C.S. 430 Assignment 6, Sample Solutions

HOMEWORK#1. t E(x) = 1 λ = (b) Find the median lifetime of a randomly selected light bulb. Answer:

AREAS AND LENGTHS IN POLAR COORDINATES. 25. Find the area inside the larger loop and outside the smaller loop

Finite Field Problems: Solutions

Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

( ) 2 and compare to M.

An Introduction to Signal Detection and Estimation - Second Edition Chapter II: Selected Solutions

CRASH COURSE IN PRECALCULUS

Solution to Review Problems for Midterm III

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

Statistics 104: Quantitative Methods for Economics Formula and Theorem Review

The Normal and Lognormal Distributions

Numerical Analysis FMN011

Strain gauge and rosettes

Concrete Mathematics Exercises from 30 September 2016

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

is like multiplying by the conversion factor of. Dividing by 2π gives you the

Reminders: linear functions

Similarly, we may define hyperbolic functions cosh α and sinh α from the unit hyperbola

PARTIAL NOTES for 6.1 Trigonometric Identities

Bayesian statistics. DS GA 1002 Probability and Statistics for Data Science.

Part III - Pricing A Down-And-Out Call Option

Transcript:

Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X + Y ). c. P (X Y ). (a) P (X ) =. (b) where A is the region P (X + Y ) = f(, y)ddy A A = {(, y) :, y, + y } = {(, y) :, y }. P (X + Y ) = 3y( + y)dyd =. For (c) the answer is 2, since f is symmetric in and y so P (X Y ) = P (X Y ) = 2. To do it directly, we have P (X Y ) = f(, y)ddy where B is the region B = {(, y) :, y, y} = {(, y) :, y }. B P (X Y ) = 3y( + y)dyd = 2. 4. Two points (X, Y ) and (U, V ) are chosen uniformly from the unit disc in R 2. Prove that the epectation of the square of the distance between the points is. What is the epected square of the distance between two points chosen uniformly and independently in the unit ball {(, y, z) : 2 + y 2 + z 2 }? Joint pdf of X and Y is h(, y) = π as π is the area of the disc D, and similarly the joint pdf of U and V is h(u, v) = π. So joint pdf of X, Y, U and V by independence is f(, y, u, v) = h(, y)h(u, v) = π 2 (, y), (u, v) D. The epectation E is the integral over D D of (( u) 2 + (y v) 2 )f(, y, u, v). We convert to polar coordinates: (, y) becomes (r, θ) and (u, v) becomes (s, φ). Then E = π 2 2π 2π rs[(r cos θ s cos φ) 2 + (r cos sin s sin φ) 2 ]dθdrdφds.

Note the appearance of rs for change of variable from (, y) to (r, θ) and from (u, v) to (s, φ). Now the integrand simplifies to rs(r 2 + s 2 2rs cos θ cos φ 2rs sin θ sin φ). The integral of cos θ and sin θ is zero over θ 2π so we are left with E = π 2 2π as required. 2π rs(r 2 + s 2 )dθdrdφds = π 2 4π2 (r 3 s + s 3 r) = 5. Let X be a random variable with pdf f() = 3 2 for < < and f() = otherwise. Find the pdf g(y) of the following functions Y = h(x). a. Y = X 2. b. Y = X/(X + ). c. Y = e X. d. Y > such that X 2 + Y 2 =. Solution to 5b. The formula for the pdf of g(y) is g(y) = f(h(y)) h (y) where h is the inverse of the function /( + ). The range of this function is [, 2 ] since. h(y) h(y) + = y h(y) = y y for y 2. This gives h (y) = for y 2. g(y) = 3h(y) 2 ( y) 2. ( y) 2 = 3y2 ( y) 4 7. Determine () the marginal pdfs f X and f Y, as well as (2) the conditional pdfs f Y X= and f X Y =y for the random variables X and Y with the joint pdf f(, y) given below. (3) State in each case whether X and Y are independent random variables and (4) determine E(X) and E(Y ) and E(X Y = y) and E(Y X = ). a. f(, y) = 2( + y), y. b. f(, y) = 4( y), < <, < y <. c. f(, y) = 2y( y), < <, < y <, < + y <. d. 4 f(, y) = π π(+y 2 ) e 2,, y. 2

Solution to 7c. The formulas are f X () = f(, y)dy f Y X= (y) = f(, y) f X () and similarly for f Y (y), f X Y =y () and E(X Y = y). formulas, f X () = f Y X= (y) = E(Y X = ) = E(Y X = ) = yf Y X= (y)dy The above quantities are, using the 2y( y)dy = 2( ) 3 for 6y( y) ( ) 3 for y 6y 2 ( y) ( ) 3 dy = ( ). 2 Since everything is symmetric in and y, the same formulas hold when X and Y are interchanged, so f Y (y) = 2( y) 3 y for y, f X Y =y () = 6( y)/( y) 3 for y and E(Y X = ) = 2 ( y). 8. Let Y U[, ] and let X Ep(Y ). Determine the joint pdf of X and Y and find E(X) and E(X Y 2 ). We have f(, y) = f Y (y)f X Y =y () and since f Y (y) = for y and f X Y =y () = ye y for, f(, y) = ye y for, y. Then by definition E(X) = Integrating by parts with respect to y, we get So ye y dyd. ye y dy = e ( + ). E(X) = e ( + ) d. If, then e ( + ) e ( + ) = 2/e. E(X) 2/e d = ( 2/e) d. This integral diverges, and so E(X) does not eist. Net we want to find E(X Y 2 ). Doing the inner integral as before, E(X Y 2 ) = E(X Y 2 ) = /2 ye y dyd. e /2 ( + /2) d. For 2, the numerator is at least 2/e as before, so again E(X Y 2 ) does not eist. 3

. Define a random parabola to be the graph of y = a 2 + b + c where a, b, c U[, ] are independent random variables. What is the probability that a random parabola does not intersect the -ais? The quadratic equation a 2 + b + c = has two solutions if b 2 > 4ac. If ac <, this is guaranteed to occur. The probability we want is P (ac < ) + P (b 2 > 4ac, ac > ). We know P (ac < ) = 2 since a and c are independent uniform [, ] random variables: P (ac < ) = P (a <, c > )+P (a >, c < ) = P (a < )P (c > )+P (a > )P (c < ) = 2 2 + 2 2 = 2. For the second probability, we have P (b 2 > 4ac, ac > ) = P (b 2 > 4ac, a >, c > ) + P (b 2 > 4ac, a <, c < ) = 2P (b 2 > 4ac, a >, c > ) = 4P (b > 2 ac, a >, c > ). Here we used the fact that b > 2 ac and b < 2 ac are events with the same probability. The joint pdf of a, b and c is f(a, b, c) = 8 by independence, since each has pdf 2 on [, ]. P (b > 2 ac, a >, c > ) = 8 dbdadc where Rewriting the inequalities, A = {(a, b, c) : a >, c >, b > 2 ac, a, c, b }. A = {(a, b, c) : < a, < c, 2 ac < b }. The third inequality says ac 4 or c 4a. So the region splits into two pieces: A = {(a, b, c) : < a /4, < c, 2 ac < b < } A and A 2 = {(a, b, c) : /4 < a, < c /4a, 2 ac < b < }. P (b > 2 ac, a >, c > ) = /4 2 ac 8 dbdcda+ /4 So finally, the probability of cutting the -ais in two points is /4a 2 + 4 5 + 6 ln 2 4 + 6 ln 2 =.627. 288 72 2 ac 5 + 6 ln 2 dbdcda =. 8 288 4

Solution to question 4: The unit ball (not required). For the unit ball B, the distance is (X U) 2 + (Y V ) 2 + (Z W ) 2 between the uniformly chosen points (X, Y, Z) and (U, V, W ). So the epectation is ( u) 2 + (y v) 2 + (z w) 2 f(, y, z, u, v, w)dwdvdudzdyd. (,y,z) B (u,v,w) B Here the joint pdf is f(, y, z, u, v, w) = (4π/3) 2 = 9 6π 2 for (, y, z), (u, v, w) B since the volume of the ball is 4 3π. The integral is best done in spherical co-ordinates. Recall in spherical = r cos θ sin φ, y = r sin θ sin φ, z = r cos φ. Using (r, θ, φ) for (, y, z) and (s, δ, ψ) for (u, v, w), the distance simplifies to r 2 +s 2 2rs cos φ cos ψ 2rs cos θ cos δ sin φ sin ψ 2rs sin θ sin δ sin φ sin ψ = r 2 +s 2 α β γ. For the change of variables (, y, z) to (r, θ, φ), we incur r 2 sin φ and for the change of variables (u, v, w) to (s, δ, ψ) we incur s 2 sin ψ. Integrating over θ, the terms βr 2 s 2 sin φ sin ψ and γr 2 s 2 sin φ sin ψ disappear. Integrating over φ, the term αr 2 s 2 sin φ sin ψ disappears too. The integral is 9 6π 2 2π π 2π π [r 2 + s 2 ]r 2 s 2 sin φ sin ψdθdφdrdδdψds = 6 5. So the epected distance between two uniform points in B is 6/5. 5