MATH2715: Statistical Methods

Size: px
Start display at page:

Download "MATH2715: Statistical Methods"

Transcription

1 MATH275: Statistical Methods Exercises III (based on lectres 5-6, work week 4, hand in lectre Mon 23 Oct) ALL qestions cont towards the continos assessment for this modle. Q. If X has a niform distribtion oer the interal (0,), proe that U = log X has an exponential distribtion with mean one. Hint: X has probability density fnction f X (x) = for 0 < x <. Find the probability density fnction of U. Q2. (a) If X has a niform distribtion oer the interal (0, ), obtain the probability density fnction of U = X 2. (b) If X has a niform distribtion oer the interal ( 2,+ 2 ), obtain the probability density fnction of U = X 2. Hint: Is this a mapping? Q3. A non-negatie random ariable X has probability density fnction f X (x) = e x, x > 0. Derie the probability density fnction f U () of U = log X. Sketch this fnction f U (). Hint: Don t forget that yo shold always specify the range of a probability density fnction. To sketch f U () yo cold look at what happens for large and small and check for trning points. Yo cold also try sbstitting different nmerical ales for. Q4. Sppose that X has an exponential distribtion with parameter λ = 2. (a) Find the probability density fnction of U = + X. (b) Obtain the mean of U. Hint: Recall that if Z N(0,) with probability density fnction f Z (z) = e 2 z2, defined for < z <, then E[Z 2 ] = Var[Z] + {E[Z]} 2 = =. (c) Simlate 000 ales of X and hence generate 000 ales of U. What is the mean of yor simlated U ales? Hint: R commands: x=rexp(000,0.5) # Pts 000 exponential(lambda=0.5) ales into x. =sqrt(x) Q5. Sppose that random ariables X and Y are independent standard normal random ariables. (a) If U = X 2 + Y 2 and V = X/Y, obtain the joint probability density fnction f UV (,). Hint: To find the Jacobian notice that J = (x, y) (, ) = (,) (x, y). Is the mapping (x,y) (,) a mapping? (b) Proe that U and V are independent. Hint: Show that f UV (,) factorises as f U ()f V () where f U () and f V () are recognisable probability density fnctions. 24

2 Backgrond Notes: Lectre 5: Fnctions of a random ariable Example Power of wind trbines 24 For a wind with instantaneos speed V the power is P = 2 λv 3 where λ is the density of the air 25. Typically windspeeds are aeraged oer a day and the aerage daily windspeed U is sch that U can be modelled as a normal distribtion. The power P aailable to a wind trbine typically satisfies P U 5/2. Example Income in UK 26 Incomes U are sch that X = log U is well-modelled by a normal distribtion; see figre 0. Freqency per interal of Millions per interal of width one nit Income before tax (ponds) log 0 (Income before tax) Figre 0: (left) histogram of income before tax , (right) histogram of log 0 (income). Reasons for transforming random ariables A common goal in transforming ariables is to indce symmetry and homogeneity in the error distribtion a transformation designed to achiee one prpose...often also helps to achiee another. 28 Backgrond Notes: Lectre 6: Fnctions of two random ariables Jacobian of a transformation Consider the transformation = (x, y) and = (x, y) which maps R xy in the (x,y) plane into the rectanglar region R with area in the (,) plane; see figre. 24 Sorce: Haslett, J. and Raftery, A.E. (989) Space-time modelling with long-memory dependence: assessing Ireland s wind power, Applied Statistics, 38, Imagine a nit area in space and let λ be the density of the air. For a wind with speed blowing perpendiclar to the area, a olme of air eqal to will be moed in nit time. The mass of air that moes will eqal m = λ. The kinetic energy of this moing mass eqals 2 m2 = 2 λ3 and per nit time the power deeloped will eqal 2 λ3. 26 Sorce: Inland reene, 27 Sorce: Kettl, S. (99) Acconting for heteroscedasticity in the transform both sides regression model, Applied Statistics, 40, Sorce: Kendall, M. and Start, A. (976, p.95) The Adanced Theory of Statistics, olme III (3rd edition), Griffin, London. 25

3 Y A (x,y) C R xy B V + R X Figre : Mapping R xy to R. + U The determinant J = (x,y) (,) = is referred to as a Jacobian 29 and the area R xy can be shown 30 to satisfy R xy J. It can be shown that (, ) (x,y) = = ( ) (x,y) = (, ) J. For example, if = x/y and = y, then x = and y = so that (x,y) (,) = (, ) (x,y) = /y x/y 2 = /y = /. 0 0 = while 29 Carl Jacobi (804-85) was a German mathematician who worked extensiely with determinants. 30 In figre, let point A map to (, ) and B map to ( +, ) so A has x-coordinate x(, ) while B has x-coordinate x(+, ) where x = x(,) and y = y(, ) denotes the inerse transformation from the (, ) plane to the (x,y) plane. Since = lim x( +, ) x(,) 0 it follows that the x-difference of A and B is B is y( +, ) y(, ). Hence the ector AB satisfies AB = x( +, ) x(, ). Similarly the y-difference of A and ««i + j where i and j are nit ectors in the x and y directions respectiely. Similarly ««AC = i + j. For small and, R xy will be approximately a parallelogram with area AB AC where denotes a ector prodct. Ths the area of R xy is gien by AB AC (x,y) = (, ). 26

4 Frther reading for lectres 5 and 6 Rice, J.A. (995) Mathematical Statistics and Data Analysis (2nd edition), section 2.3, 3.6, 4.. Hogg, R.V., McKean, J.W. and Craig, A.T. (2005) Introdction to Mathematical Statistics (6th edition), sections.7, 2.2, 2.7, 3.3. Larsen, R.J. and Marx, M.L. (200) An Introdction to Mathematical Statistics and its Applications (5th edition), sections 3.8, 7.3. Miller, I. and Miller, M. (2004) John E. Frend s Mathematical Statistics with Applications, sections 6.3, 7.3,

5 MATH275: Statistical Methods Worked Examples III Worked Example: A random nmber between 0 and is a ale niformly distribted between 0 and. Sppose yo hae aailable a seqence of sch random nmbers. Sggest how yo cold generate a seqence of ales haing an exponential distribtion with parameter λ, mean µ = /λ. Answer: Here X niform(0,) so f X (x) = for 0 < x <. exponential(λ) so that f U () = λe λ for > 0. Ths f U () = f X (x) dx d = λe λ, > 0, We want to hae U so we reqire dx d = λe λ x = e λ. The reqired transformation is ths = log x. λ Worked Example: If X niform(0,), find the probability density fnction of U = X. Answer: The mapping x is. if x, f X (x) = for 0 < x < and F X (x) = x if 0 < x <, 0 if x 0. Range of U: 0 < x < = 0 < <. Using cmlatie distribtion fnction: { } F U () = pr{u } = pr X = pr { X 2} = F X ( 2 ) = 2 for 0 < <. f U () = df U() = 2 for 0 < <. d Direct approach: = x so x = 2 and dx d = 2. Ths f U() = f X (x) dx d = 2. The reslt of a simlation 3 of 2000 ales U = X is plotted in figre 2(left) and the histogram shows the U ales hae a probability density fnction f U () = 2. Worked Example: If X niform(,), find the probability density fnction of U = X 2. 3 Sitable R code is: x=rnif(2000) # Pt 2000 niform(0,) ales into x. =sqrt(x) # =sqrt(x). hist(x,breaks=00) # Histogram of x with 00 interals. hist(,breaks=00) # Histogram of with 00 interals. 28

6 Freqency per interal of width Freqency per interal of width Figre 2: (left) histogram of 2000 simlated U = X ales for X niform(0,) and probability density fnction of U; (right) histogram of 2000 simlated U = X 2 ales for X niform(,) and probability density fnction of U. Answer: f X (x) = 2 for < x < and F X(x) = Range of U: Since < x <, range of U satisfies 0 < <. Using cmlatie distribtion fnction approach: if x, 2 + 2x if < x <, 0 if x. F U () = pr{u } = pr { X 2 } = pr { < X } = F X ( ) F X ( ) =. f U () = df U() d = 2 for 0 <. Direct approach: The mapping x is not. Both x = and x = + gie the same -ale. Ths split the range of X into {x < 0} and {x > 0}. Since = x 2, then x = ± and dx d = ± 2 2. f U () = f X (x = ) dx d +f X (x = + ) dx x= d = x= = 2. The reslt of a simlation 32 of 2000 ales U = X 2 is plotted in figre 2(right) and the histogram shows the U ales hae probability density fnction f U () = /2. Worked Example: Sppose X N(0, ). Use the cmlatie distribtion fnction approach to obtain the distribtion of U = X 2. Answer: Here F U () = pr{u } = pr { X 2 } = pr { X } ; 29

7 f X (x) X ~ N(0,) = x 2 x = - /2 0 x = + /2 x - /2 0 /2 x Figre 3: (left) U if X ; (right) shaded region is pr{ X }. see figre 3. Since X N(0,), so pr{a < X b} = F U () = b a f X (x)dx = b a e 2 x2 dx e 2 x2 dx = 2 e 2 x2 dx, 0 sing symmetry. Differentiating nder the integral 33 gies f U () = df U() d = 2 e 2 ( ) 2 ( ) 2 2 = e 2, > Sitable R code is: x=rnif(2000,-,) # Pt 000 niform(-,) ales into x. =x^2 # =x^2 hist(,breaks=c(0:00)*0.0)) # Histogram of with 00 interals. 33 Sppose that G() = Z b a g(x,) dx where a and b are fnctions of and g(x,) is a fnction of x and. Then dg() d = g(b,) db Z da b g(a,) d d + g(x, ) dx. a This is sometimes known as the Liebnitz integral rle. Z 2 Example: G() = e x dx dg() Z 2 = e 3 2 (e 0) + xe x dx. Z d Example: G() = e x f(x)dx dg() Z = xe x f(x)dx on writing g(x,) = e x f(x) and noting that d the integration limits Z do not depend on. b Example: G() = e 2 x2 dx dg() = e 2 b2 db with g(x,) = e 2 x2 and noting that g d d = 0. Z To proe the formla for differentiation nder the integral sppose G (x,) = g(x,)dx so G (x, ) = g(x,). Then 2 G (x, ) = 2 G (x,) «G (x, ) = «G (x,) = g(x,). Z Integrating with respect to x gies G (x,) g(x,) = dx. This reslt implies: () Z Z Z g(x,) g(x,)dx = dx, and (2), as a definite integral, G (b, ) G (a, ) b g(x, ) = dx. 30 a

8 Worked Example: Use the cmlatie distribtion approach to derie the probability density fnction of U = e X when X N(µ,σ 2 ). Answer: Here X N(µ,σ 2 ) and U = e X, = e x. Ths pr{u } = pr { e X } { = pr{x log } = pr Z log µ } ( ) log µ = Φ σ σ where Z = X µ σ N(0,) and Φ(z) = pr{z z}. Hence F U () = log µ z0 = σ z= e 2 z2 dz and, recalling differentiation nder an integral with dz 0 d = σ, f U () = df U() d = e 2 z2 0 dz 0 d = exp { (log µ) 2 2σ 2 } σ, > 0, Worked Example: If a random ariable X has probability density fnction f X (x) and cmlatie distribtion fnction F X (x), proe that U = F X (x) niform(0,). Answer: Since U = F X (x), then d dx = df X(x) = f X (x) so f U () = f X (x) dx dx d = f X(x) d =. dx Since 0 F X (x) it follows that 0 and so U niform(0,). Worked Example: If X,Y ind niform(0, ), find the probability density fnction of U = X/Y. Answer: Since X and Y are independent, f XY (x,y) = f X (x)f Y (y) = for 0 < x,y <. Let = x/y, = y. Inerse transformation is y =, x = y = and the Jacobian is J = (x,y) (,) = = 0 =. Considering now the definite integral G() = dg() d = G (b, ) b Z b a g(x,) dx, it follows that G() = G (b,) G (a, ). Hence db d + G (b, ) G (a, ) da a d G (a, ) = g(b, ) db d + G (b, ) g(a,) da d G (a,) = g(b,) db d g(a,)da d + ( ) Z b a g(x, ) dx. The reslt ( ) follows from obtaining the total deriatie of G (b, ) and G (a, ). Recall that for a fnction f(x, y) f(x, y) f(x, y) with x = x() and y = y() both fnctions of, then = f(x, y) +. Writing f(x, y) = G (b, ) gies G (b, ) = G (b, ) b b + G (b, ) = G (b, ) b b + G (b, ). Similarly G (a, ) can be obtained. 3

9 Clearly this is a mapping 34. Ths f UV (,) = f XY (x,y) J = =. Range of (U,V ): Clearly = x/y satisfies 0 < <. 0 < y < = 0 < <. 0 < x < = 0 < < = 0 < < /. For to satisfy both constraints 0 < < and 0 < < / we need 0 < < min(,/). Ths if 0 < <, then 0 < < whereas if > then 0 < < /. This gies the region (,) where f UV (,) is defined. Figre 4(left) shows the region where (x, y) is defined while figre 4(right) shows the corresponding region in the (,) plane. The defined region in the (,) plane depends on whether < or >. It can be seen that the mapping (x,y) (,) is a mapping. Figre 5(left) shows 2000 simlated ales of (,). y =0.5 =0.5 = =2 = =0.5 =0.5 = =2 = x Figre 4: showing region where (left) (X,Y ) defined, (right) (U,V ) defined, together with lines showing = 2,,2,4 and = 2. A different way to obtain the range of (,) is to notice that = x/y implies y = x/. This is the eqation of a straight line with slope /; see figre 4(left). (a) If 0 < <, then this line passes throgh the origin (x,y) = (0,0) and has slope (/) >. Ths this line intersects the nit sqare defining the (x,y)-region at (x,y) = (,). Along this line y takes all ales between 0 and. Hence for 0 < <, it follows that 0 < <. (b) Now consider the case >. In this case the line y = x/ has slope (/) <. This line again passes throgh the origin (x, y) = (0, 0) and intersects the nit sqare defining the (x, y)-region at (x,y) = (,/). Along this line y only takes ales between 0 and /. Hence for the case >, it follows that 0 < < /. Probability density fnction of U: Notice that the region of integration with respect to depends on the ale of. d = 2 if 0 <, f U () = f UV (,)d = =0 / d = 2 2 if >. =0 34 Each (x, y) pair maps to a single (, ) pair. By inspection a particlar (, ) pair cn only originate from a specific (x,y) pair. 32

10 A simlation stdy generated 2000 ales of (U,V ), as shown in figre 5(left). 35 The histogram in figre 5(right) show the U ales hae a distribtion with a long tail. Concentrating on the interal 0 < < 5 it is seen that the histogram of ales is approximately constant for < and then decays as / 2 for > Freqency per interal of width Figre 5: (left) 2000 random ales of (,); (right) histogram of simlated ales and probability density fnction of U. Worked Example: If X, Y are niformly distribted inside the nit circle, find the probability density fnction of U = X/Y. Answer: f XY (x,y) = π for x2 + y 2 <. Let = x/y, = y. Inerse transformation is y =, x = y = and the Jacobian is J = (x,y) (,) = = 0 =. The mapping is a mapping eerywhere except for when y = 0. Since these points map to ±, they do not case a problem. Hence f UV (,) = f XY (x,y) J = π. Range of (U,V ): Notice = x/y satisfies < < whilst x 2 + y 2 < = < = 2 < + 2 = + 2 < < Sitable R code is: x=rnif(2000) # Pt 2000 niform(0,) ales into x. y=rnif(2000) # Pt 2000 niform(0,) ales into y. =x/y; =y # =x/y, =y. plot([<5],[<5],xlab="",ylab="") # Plot (,) locations for cases with <5. hist(,breaks=000) # Histogram of with 000 interals. hist(,breaks=c((0:50)*0.,max()+),xlim=c(0,5)) # Specify break locations. 33

11 Probability density fnction of U: f U () = f UV (,)d = = = =0 0 π d = [ 2 π d = 2 = + 2 ] + 2 =0 ( ) π d + = + 2 =0 π( + 2 ). π d For a simlation stdy 36 of 2000 ales of (U,V ), figre 6(left) shows the distribtion of (X,Y ) whilst figre 6(right) shows the distribtion of (U,V ). A histogram of U wold show that the Cachy distribtion U has a long tail. y x Figre 6: (left) 2000 points niformly distribted oer nit circle, (right) mapping to (, )-plane shows density of (U,V ) increases as increases, so f UV (,). Worked Example: If X has a standard normal distribtion and Y, independent of X, has probability density fnction { ye 2 y2 if y > 0, f Y (y) = 0 if y 0, 36 Sitable R code is: xx=rnif(5000,-,) # Pt 5000 niform(-,) ales into xx. yy=rnif(5000,-,) # Pt 5000 niform(-,) ales into yy. x=xx[xx^2+yy^2<] # Set x and y to only contain ales y=yy[xx^2+yy^2<] # of xx,yy lying in region xx^2+yy^2<. x=x[:2000] # Make x contain first 2000 ales of x. y=y[:2000] # x and y now contain jst 2000 points. =x/y # =x/y. =y hist(,breaks=000) # Histogram of with 000 interals. hist(,breaks=000,xlim=c(-5,5)) plot(xx,yy,xlab="x",ylab="y") # Plot shows (xx,yy) points niformly. plot(,,xlim=c(-5,5),xlab="",ylab="") # Plot shows (,) distribtion. 34

12 show that U = X/Y has probability density fnction f U () = What is E[U]? Answer: As X and Y are independent, their joint probability density fnction is 2( + 2, < <. ) 3/2 f XY (x,y) = f X (x)f Y (y) = e 2 x2 ye 2 y2 = ye 2 (x2 +y 2), < x <, y > 0. For the transformation = x/y, = y, so x = and y =, the Jacobian is J = (x,y) (,) = = 0 =. Inspection shows this is a mapping. Hence, with x 2 + y 2 = () = 2 ( + 2 ), f UV (,) = f XY (x,y) J = ye 2 (x2 +y 2) = 2 e 2 (+2 ) 2. Range of U and V : Since < x < + and y > 0 it follows that < < + and > 0. y = =0 =0.5 = = = =0 =0.5 = = x Figre 7: showing region where (left) (X,Y ) defined, (right) (U,V ) defined, together with lines showing =, 2,,2. Recall that < x < while y > 0. Probability density fnction of U: f U () = =0 f UV (,)d = =0 2 e 2 (+2 ) 2 d. Approach : Notice if W N(0,σ 2 ), then E[W] = 0 so σ 2 = E[W 2 ] = Hence f U () = w=0 =0 Approach 2: σ 2 w2 e w2 2σ 2 dw = σ2 f U () = 2 e 2 (+2 ) 2 d = σ 2. Now pt σ2 = so that + 2 =0 w= σ 2 2 e 2 2σ 2 d = σ3 2 = Pt z = 2 ( + 2 ) 2 so dz d = ( + 2 ), = z=0 2z + 2 e z σ 2 w2 e w2 2σ 2 dw. 2( + 2 ) 3/2. 2z ( + 2 ), d = dz 2z( + 2 ) = π( + 2 ) 3/2 z=0 dz 2z( + 2 ) z 2 e z dz 35

13 Recall the gamma fnction Γ(k) = z=0 z k e z dz with Γ ( ) 3 2 = 2 Γ( ) 2 = 2 π = π( + 2 ) 3/2 Γ ( ) 3 2 = 2( + 2, < <. ) 3/2 Mean of U: E[U] = 0 as f U () is symmetric abot zero. Worked Example: If X niform(, ) and Y niform(0, ) are independent random ariables, what is the probability density fnction of U = XY? Answer: f X (x) = 2 for < x < and f Y (y) = for 0 < y <. As X and Y are independent, their joint probability density fnction is f XY (x,y) = f X (x)f Y (y) = 2 for < x < and 0 < y <. The transformation = xy and = y has inerse x = / and y =. The Jacobian J satisfies J = (x,y) (,) = (x,y) (,) = = / / 2 0 It is perhaps easier to ealate the Jacobian J by considering instead (, ) (x,y) = = y x 0 = y. =. The Jacobian then satisfies J = (x,y) (,) = ( ) (,) = (x, y) y. Inspection shows this is a mapping. Hence f UV (,) = f XY (x,y) J = 0.5 y = 2. Range of U and V : 0 < y < = 0 < <. < x < = y < xy < +y = < < < + < +. If > 0, then 0 < < <. If < 0, then < < < 0 so < <. Figre 8(left) shows 000 simlated ales of (,). Probability density fnction of U: Notice the region of integration with respect to depends on the particlar ale of. f U () = f UV (,)d = = 2 d = [ 2 log ] = = 2 log( ) if < < 0, 2 d = [ 2 log ] = = 2 log() if 0 < <. = Clearly f U () = 2 log( ) = log( / ) for < < A more direct approach wold notice that < < if > 0 whilst < < if < 0. Ths we hae < < so that f U() = Z = f UV (, ) d = 2 log( ). 36

14 Freq. per interal Figre 8: (left) 000 simlated ales of (, ); (right) histogram of ales and probability density fnction of U. A simlation stdy 38 yields a plot of the (U,V ) region in figre 8(left). The histogram in figre 8(right) show the U ales together with the probability density fnction of U. Worked Example: Sppose that X and Y are independent standard normal random ariables. Let U = X 2 + Y 2 and V = Y. Obtain the marginal probability density fnction of U. Answer: As X and Y are independent, their joint probability density fnction is f XY (x,y) = f X (x)f Y (y) = e 2 x2 e 2 y2 = e 2 (x2 +y 2 ) for < x < + and < y < +. The transformation = x 2 + y 2 and = y satisfies x = ± 2 and y =. It is ths not a transformation; both (x,y) and ( x,y) map to the same ale (,). It is easier to ealate the Jacobian J by considering instead (, ) (x,y) = = 2x 2y 0 = 2x. The Jacobian then satisfies J = (x,y) (,) = ( ) (,) = (x, y) 2x = ± Sitable R code is: x=rnif(000,-,) # Pt 000 niform(-,) ales into x. y=rnif(000) # Pt 000 niform(0,) ales into y. =x*y # =x*y. =y # =y. plot(,,xlab="",ylab="",main="") # Plot of simlated (,) ales. hist(,breaks=c(-50:50)*0.02,xlab="",ylab="freq. per interal 0.02",main="") cre(000*0.02*(log(sqrt(/abs(x)))),-,,add=true) # Add pdf of U. 37

15 Since both (x,y) and ( x,y) map to the same ale (,), f UV (,) = f XY (x,y) f XY ( x,y) 2 2 = e 2 (x2 +y 2) e 2 (( x)2 +y 2) 2 2 = 2 e 2 (x2 +y 2) 2 2 = e 2 2. Range of U and V : It crdely appears that > 0 and < < +. More careflly, 2 = x 2 < so < < +. Alternatiely, consider the geometrical interpretation of the transformation. Ths = x 2 + y 2 defines a circle in the x-y plane with centre (0,0) and radis. For this circle, the y ales range between + and. Ths with = y we hae < < +. Figre 9 shows the reslts of plotting simlated ales of (X,Y ) in the - plane Figre 9: showing (U,V ) plotted for 000 random pairs (X,Y ) where U = X 2 + Y 2, V = Y and X, Y are independent standard normal random ariables. 39 R code is: x=rnorm(000) # Generate 000 ales x as N(0,). y=rnorm(000) =x 2+y 2; =y # The mapping sed. plot(,) # Plot against. 38

16 Probability density fnction of U: Here 40 f U () = f UV (,)d = + = + = e 2 = e 2 for > 0, so U exponential(λ = 2 ). e 2 2 d = d 2 [ sin ] + = = e 2 [ 2 π ( 2 π)] = 2 e 2 Worked Example: Sppose that X and Y are independent random ariables each haing a niform distribtion on the interal (0,). Let U = X 2 + Y 2 and V = X/Y. Obtain the marginal probability density fnction of V. Show that the marginal probability density fnction of U is a constant for. Answer: f X (x) = for 0 < x < and f Y (y) = for 0 < y <. As X and Y are independent, their joint probability density fnction is f XY (x,y) = f X (x)f Y (y) = for 0 < x < and 0 < y <. The transformation = x 2 + y 2 and = x/y satisfies x = y so = 2 y 2 + y 2. It is easier to ealate the Jacobian J by considering instead (, ) (x,y) = = 2x 2y /y x/y 2 = 2(x2 /y 2 ) 2 = 2(x 2 + y 2 )/y 2. The Jacobian then satisfies J = (x,y) (,) = ( ) (,) = (x, y) Inspection shows this is a mapping. Hence f UV (,) = f XY (x,y) J = Range of U and V : Clearly 0 < < 2 and 0 < <. y 2 2(x 2 + y 2 ) = 2( + 2 ). 2( + 2 ). More careflly, consider the region defined by = x 2 + y 2 in the x-y plane. This is a qarter circle only if 0 < < and along this qarter circle = x/y can take any ale in the interal 0 < <. Howeer, for < < 2 the qarter circle intersects the nit sqare making p the allowed (x,y)-region at (x,y) = (,) and at (x,y) = (, ) since = x 2 + y 2. For this ale of, the range of satisfies < < (/ ). Figre 20(left) shows the case = 0.6 for which 0 < < and also the case =.2 for which < < The lower limit corresponds to the case (x, y) = (0.447, ) and the pper limit to the case (x, y) = (, 0.447). The ineqality < gies < + 2 and this can only hold if < since < 2, so 0 < < + 2 if 0 < <. Similarly the ineqality < (/ ) gies < + 2 and this can only hold if > since < 2, so 0 < < + 2 if < <. Z 40 Recall that dx a2 x = x 2 sin a. 39

17 y =0.6 = Freq. per interal x Figre 20: (left) showing range of for different in (x,y)-plane; (centre) region where (,) is defined in (,)-plane; (right) histogram of ales and probability density fnction of V. An alternatie way to obtain the range of for gien is as follows. Since = x/y it follows that y = x/ is the eqation of a straight line throgh the origin (x,y) = (0,0) with slope /. (a) If 0 < <, then the line has slope (/) >. This line intersects the nit sqare making p (x,y)-region at (x,y) = (,) so that = + 2. In this case takes ales in the interal 0 < < + 2. (b) If >, then the line has slope (/) <. This line intersects the nit sqare making p the (x,y)-region at (x,y) = (,/) so that = + 2. In this case takes ales in the interal 0 < < + 2. Probability density fnction of V : Depending on the particlar ale of, the integration limits for change. + 2 [ ] f V () = f UV (,)d = =0 2( + 2 ) d = + 2 2( + 2 = if 0 < <, ) = [ ] 2( + 2 ) d = + 2 2( + 2 = ) 2 2 if < <. =0 A simlation stdy 4 yields the histogram in figre 20(right) which shows the ales together with the probability density fnction of V. Figre 20(centre) shows the region where (, ) is defined. Probability density fnction of U: In the case <, f U () = f UV (,)d = =0 =0 2( + 2 ) d = [ 2 tan () ] 0 = π 4. Strictly to answer the qestion posed it is only necessary to show that the integration does not inole. It was not necessary to ealate the integral! 4 Sitable R code is: x=rnif(2000) # Pt 000 niform(0,) ales into x. y=rnif(2000) # Pt 000 niform(0,) ales into y. =x^2+y^2; =x/y plot([<4],[<4],xlab="",ylab="") # Plot (,) ales for <4. # Add histogram of ales for <0. hist([<0],breaks=c(0:00)*0.,xlab="",ylab="freq. per interal 0.",main="") lines(c(0,),c(00,00)) # Add pdf of V for <. cre(2000*0.*(/(2*x^2)),,0,add=true) # Add pdf of V for >. 40

18 MATH275: Statistical Methods Examples Class III, week 4 The qestions below will be looked at in Examples Class III held in week 4. Q. If X is niformly distribted oer ( 2 π, ), show that U = tan X has a Cachy42 distribtion. 43 Q2. Random ariables X and Y are independent and each has an exponential distribtion with parameter λ. Consider the transformation U = X/Y and V = Y. Obtain the probability density fnction of U = X/Y. 42 Agstin-Lois Cachy ( ) was a French mathematician who became associated with what is now known as the Cachy distribtion throgh his work on the density in 853. Properties of the Cachy distribtion had howeer been discssed earlier by Poisson in 824 whilst examining properties of the Least Sqares method. 43 Link with lectres: in the lectres the ratio of two independent N(0,) ariables gae a Cachy distribtion. Ths if X, Y ind N(0,) and (X, Y ) defines a point in the plane, then in polar co-ordinates this point satisfies (R,Θ) = ( X 2 + Y 2,tan (X/Y )) where Θ is measred clockwise from the y-axis; compare this with qestion 5 of exercises III. Hence tan Θ = X/Y Cachy. In the lectres the random ariable Θ wold hae a niform( π, π) distribtion and the mapping (X, Y ) (U = X 2 + Y 2, V = X/Y ) is not a mapping. In this examples class qestion, howeer, the range of Θ is ( π, π) and this ensres we hae a mapping

MATH2715: Statistical Methods

MATH2715: Statistical Methods MATH275: Statistical Methods Exercises VI (based on lectre, work week 7, hand in lectre Mon 4 Nov) ALL qestions cont towards the continos assessment for this modle. Q. The random variable X has a discrete

More information

Vectors in Rn un. This definition of norm is an extension of the Pythagorean Theorem. Consider the vector u = (5, 8) in R 2

Vectors in Rn un. This definition of norm is an extension of the Pythagorean Theorem. Consider the vector u = (5, 8) in R 2 MATH 307 Vectors in Rn Dr. Neal, WKU Matrices of dimension 1 n can be thoght of as coordinates, or ectors, in n- dimensional space R n. We can perform special calclations on these ectors. In particlar,

More information

We automate the bivariate change-of-variables technique for bivariate continuous random variables with

We automate the bivariate change-of-variables technique for bivariate continuous random variables with INFORMS Jornal on Compting Vol. 4, No., Winter 0, pp. 9 ISSN 09-9856 (print) ISSN 56-558 (online) http://dx.doi.org/0.87/ijoc.046 0 INFORMS Atomating Biariate Transformations Jeff X. Yang, John H. Drew,

More information

MATH2715: Statistical Methods

MATH2715: Statistical Methods MATH2715: Statistical Methods Exercises V (based on lectures 9-10, work week 6, hand in lecture Mon 7 Nov) ALL questions count towards the continuous assessment for this module. Q1. If X gamma(α,λ), write

More information

1 The space of linear transformations from R n to R m :

1 The space of linear transformations from R n to R m : Math 540 Spring 20 Notes #4 Higher deriaties, Taylor s theorem The space of linear transformations from R n to R m We hae discssed linear transformations mapping R n to R m We can add sch linear transformations

More information

Graphs and Networks Lecture 5. PageRank. Lecturer: Daniel A. Spielman September 20, 2007

Graphs and Networks Lecture 5. PageRank. Lecturer: Daniel A. Spielman September 20, 2007 Graphs and Networks Lectre 5 PageRank Lectrer: Daniel A. Spielman September 20, 2007 5.1 Intro to PageRank PageRank, the algorithm reportedly sed by Google, assigns a nmerical rank to eery web page. More

More information

Change of Variables. (f T) JT. f = U

Change of Variables. (f T) JT. f = U Change of Variables 4-5-8 The change of ariables formla for mltiple integrals is like -sbstittion for single-ariable integrals. I ll gie the general change of ariables formla first, and consider specific

More information

MATH2715: Statistical Methods

MATH2715: Statistical Methods MATH2715: Statistical Methods Exercises IV (based on lectures 7-8, work week 5, hand in lecture Mon 30 Oct) ALL questions count towards the continuous assessment for this module. Q1. If a random variable

More information

Lesson 81: The Cross Product of Vectors

Lesson 81: The Cross Product of Vectors Lesson 8: The Cross Prodct of Vectors IBHL - SANTOWSKI In this lesson yo will learn how to find the cross prodct of two ectors how to find an orthogonal ector to a plane defined by two ectors how to find

More information

Reduction of over-determined systems of differential equations

Reduction of over-determined systems of differential equations Redction of oer-determined systems of differential eqations Maim Zaytse 1) 1, ) and Vyachesla Akkerman 1) Nclear Safety Institte, Rssian Academy of Sciences, Moscow, 115191 Rssia ) Department of Mechanical

More information

Change of Variables. f(x, y) da = (1) If the transformation T hasn t already been given, come up with the transformation to use.

Change of Variables. f(x, y) da = (1) If the transformation T hasn t already been given, come up with the transformation to use. MATH 2Q Spring 26 Daid Nichols Change of Variables Change of ariables in mltiple integrals is complicated, bt it can be broken down into steps as follows. The starting point is a doble integral in & y.

More information

EE2 Mathematics : Functions of Multiple Variables

EE2 Mathematics : Functions of Multiple Variables EE2 Mathematics : Fnctions of Mltiple Variables http://www2.imperial.ac.k/ nsjones These notes are not identical word-for-word with m lectres which will be gien on the blackboard. Some of these notes ma

More information

Lecture 3. (2) Last time: 3D space. The dot product. Dan Nichols January 30, 2018

Lecture 3. (2) Last time: 3D space. The dot product. Dan Nichols January 30, 2018 Lectre 3 The dot prodct Dan Nichols nichols@math.mass.ed MATH 33, Spring 018 Uniersity of Massachsetts Janary 30, 018 () Last time: 3D space Right-hand rle, the three coordinate planes 3D coordinate system:

More information

Math 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation:

Math 263 Assignment #3 Solutions. 1. A function z = f(x, y) is called harmonic if it satisfies Laplace s equation: Math 263 Assignment #3 Soltions 1. A fnction z f(x, ) is called harmonic if it satisfies Laplace s eqation: 2 + 2 z 2 0 Determine whether or not the following are harmonic. (a) z x 2 + 2. We se the one-variable

More information

u P(t) = P(x,y) r v t=0 4/4/2006 Motion ( F.Robilliard) 1

u P(t) = P(x,y) r v t=0 4/4/2006 Motion ( F.Robilliard) 1 y g j P(t) P(,y) r t0 i 4/4/006 Motion ( F.Robilliard) 1 Motion: We stdy in detail three cases of motion: 1. Motion in one dimension with constant acceleration niform linear motion.. Motion in two dimensions

More information

The Cross Product of Two Vectors in Space DEFINITION. Cross Product. u * v = s ƒ u ƒƒv ƒ sin ud n

The Cross Product of Two Vectors in Space DEFINITION. Cross Product. u * v = s ƒ u ƒƒv ƒ sin ud n 12.4 The Cross Prodct 873 12.4 The Cross Prodct In stdying lines in the plane, when we needed to describe how a line was tilting, we sed the notions of slope and angle of inclination. In space, we want

More information

The Brauer Manin obstruction

The Brauer Manin obstruction The Braer Manin obstrction Martin Bright 17 April 2008 1 Definitions Let X be a smooth, geometrically irredcible ariety oer a field k. Recall that the defining property of an Azmaya algebra A is that,

More information

Turbulence and boundary layers

Turbulence and boundary layers Trblence and bondary layers Weather and trblence Big whorls hae little whorls which feed on the elocity; and little whorls hae lesser whorls and so on to iscosity Lewis Fry Richardson Momentm eqations

More information

Math 116 First Midterm October 14, 2009

Math 116 First Midterm October 14, 2009 Math 116 First Midterm October 14, 9 Name: EXAM SOLUTIONS Instrctor: Section: 1. Do not open this exam ntil yo are told to do so.. This exam has 1 pages inclding this cover. There are 9 problems. Note

More information

m = Average Rate of Change (Secant Slope) Example:

m = Average Rate of Change (Secant Slope) Example: Average Rate o Change Secant Slope Deinition: The average change secant slope o a nction over a particlar interval [a, b] or [a, ]. Eample: What is the average rate o change o the nction over the interval

More information

3.3 Operations With Vectors, Linear Combinations

3.3 Operations With Vectors, Linear Combinations Operations With Vectors, Linear Combinations Performance Criteria: (d) Mltiply ectors by scalars and add ectors, algebraically Find linear combinations of ectors algebraically (e) Illstrate the parallelogram

More information

Math 4A03: Practice problems on Multivariable Calculus

Math 4A03: Practice problems on Multivariable Calculus Mat 4A0: Practice problems on Mltiariable Calcls Problem Consider te mapping f, ) : R R defined by fx, y) e y + x, e x y) x, y) R a) Is it possible to express x, y) as a differentiable fnction of, ) near

More information

Math 144 Activity #10 Applications of Vectors

Math 144 Activity #10 Applications of Vectors 144 p 1 Math 144 Actiity #10 Applications of Vectors In the last actiity, yo were introdced to ectors. In this actiity yo will look at some of the applications of ectors. Let the position ector = a, b

More information

Higher Maths A1.3 Recurrence Relations - Revision

Higher Maths A1.3 Recurrence Relations - Revision Higher Maths A Recrrence Relations - Revision This revision pack covers the skills at Unit Assessment exam level or Recrrence Relations so yo can evalate yor learning o this otcome It is important that

More information

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL

UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL 8th International DAAAM Baltic Conference "INDUSTRIAL ENGINEERING - 19-1 April 01, Tallinn, Estonia UNCERTAINTY FOCUSED STRENGTH ANALYSIS MODEL Põdra, P. & Laaneots, R. Abstract: Strength analysis is a

More information

6.4 VECTORS AND DOT PRODUCTS

6.4 VECTORS AND DOT PRODUCTS 458 Chapter 6 Additional Topics in Trigonometry 6.4 VECTORS AND DOT PRODUCTS What yo shold learn ind the dot prodct of two ectors and se the properties of the dot prodct. ind the angle between two ectors

More information

MAT389 Fall 2016, Problem Set 6

MAT389 Fall 2016, Problem Set 6 MAT389 Fall 016, Problem Set 6 Trigonometric and hperbolic fnctions 6.1 Show that e iz = cos z + i sin z for eer comple nmber z. Hint: start from the right-hand side and work or wa towards the left-hand

More information

Exercise 4. An optional time which is not a stopping time

Exercise 4. An optional time which is not a stopping time M5MF6, EXERCICE SET 1 We shall here consider a gien filtered probability space Ω, F, P, spporting a standard rownian motion W t t, with natral filtration F t t. Exercise 1 Proe Proposition 1.1.3, Theorem

More information

ON THE PERFORMANCE OF LOW

ON THE PERFORMANCE OF LOW Monografías Matemáticas García de Galdeano, 77 86 (6) ON THE PERFORMANCE OF LOW STORAGE ADDITIVE RUNGE-KUTTA METHODS Inmaclada Higeras and Teo Roldán Abstract. Gien a differential system that inoles terms

More information

Section 7.4: Integration of Rational Functions by Partial Fractions

Section 7.4: Integration of Rational Functions by Partial Fractions Section 7.4: Integration of Rational Fnctions by Partial Fractions This is abot as complicated as it gets. The Method of Partial Fractions Ecept for a few very special cases, crrently we have no way to

More information

Lecture 2: CENTRAL LIMIT THEOREM

Lecture 2: CENTRAL LIMIT THEOREM A Theorist s Toolkit (CMU 8-859T, Fall 3) Lectre : CENTRAL LIMIT THEOREM September th, 3 Lectrer: Ryan O Donnell Scribe: Anonymos SUM OF RANDOM VARIABLES Let X, X, X 3,... be i.i.d. random variables (Here

More information

SUBJECT:ENGINEERING MATHEMATICS-I SUBJECT CODE :SMT1101 UNIT III FUNCTIONS OF SEVERAL VARIABLES. Jacobians

SUBJECT:ENGINEERING MATHEMATICS-I SUBJECT CODE :SMT1101 UNIT III FUNCTIONS OF SEVERAL VARIABLES. Jacobians SUBJECT:ENGINEERING MATHEMATICS-I SUBJECT CODE :SMT0 UNIT III FUNCTIONS OF SEVERAL VARIABLES Jacobians Changing ariable is something e come across er oten in Integration There are man reasons or changing

More information

SECTION 6.7. The Dot Product. Preview Exercises. 754 Chapter 6 Additional Topics in Trigonometry. 7 w u 7 2 =?. 7 v 77w7

SECTION 6.7. The Dot Product. Preview Exercises. 754 Chapter 6 Additional Topics in Trigonometry. 7 w u 7 2 =?. 7 v 77w7 754 Chapter 6 Additional Topics in Trigonometry 115. Yo ant to fly yor small plane de north, bt there is a 75-kilometer ind bloing from est to east. a. Find the direction angle for here yo shold head the

More information

ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 2 LINEAR IMPULSE AND MOMENTUM

ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 2 LINEAR IMPULSE AND MOMENTUM ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D5 TUTORIAL LINEAR IMPULSE AND MOMENTUM On copletion of this ttorial yo shold be able to do the following. State Newton s laws of otion. Define linear

More information

Direct linearization method for nonlinear PDE s and the related kernel RBFs

Direct linearization method for nonlinear PDE s and the related kernel RBFs Direct linearization method for nonlinear PDE s and the related kernel BFs W. Chen Department of Informatics, Uniersity of Oslo, P.O.Box 1080, Blindern, 0316 Oslo, Norway Email: wenc@ifi.io.no Abstract

More information

Figure 1 Probability density function of Wedge copula for c = (best fit to Nominal skew of DRAM case study).

Figure 1 Probability density function of Wedge copula for c = (best fit to Nominal skew of DRAM case study). Wedge Copla This docment explains the constrction and properties o a particlar geometrical copla sed to it dependency data rom the edram case stdy done at Portland State University. The probability density

More information

Spring, 2008 CIS 610. Advanced Geometric Methods in Computer Science Jean Gallier Homework 1, Corrected Version

Spring, 2008 CIS 610. Advanced Geometric Methods in Computer Science Jean Gallier Homework 1, Corrected Version Spring, 008 CIS 610 Adanced Geometric Methods in Compter Science Jean Gallier Homework 1, Corrected Version Febrary 18, 008; De March 5, 008 A problems are for practice only, and shold not be trned in.

More information

Sources of Non Stationarity in the Semivariogram

Sources of Non Stationarity in the Semivariogram Sorces of Non Stationarity in the Semivariogram Migel A. Cba and Oy Leangthong Traditional ncertainty characterization techniqes sch as Simple Kriging or Seqential Gassian Simlation rely on stationary

More information

THE DIFFERENTIAL GEOMETRY OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE

THE DIFFERENTIAL GEOMETRY OF REGULAR CURVES ON A REGULAR TIME-LIKE SURFACE Dynamic Systems and Applications 24 2015 349-360 TH DIFFRNTIAL OMTRY OF RULAR CURVS ON A RULAR TIM-LIK SURFAC MIN OZYILMAZ AND YUSUF YAYLI Department of Mathematics ge Uniersity Bornoa Izmir 35100 Trkey

More information

STEP Support Programme. STEP III Hyperbolic Functions: Solutions

STEP Support Programme. STEP III Hyperbolic Functions: Solutions STEP Spport Programme STEP III Hyperbolic Fnctions: Soltions Start by sing the sbstittion t cosh x. This gives: sinh x cosh a cosh x cosh a sinh x t sinh x dt t dt t + ln t ln t + ln cosh a ln ln cosh

More information

Second-Order Wave Equation

Second-Order Wave Equation Second-Order Wave Eqation A. Salih Department of Aerospace Engineering Indian Institte of Space Science and Technology, Thirvananthapram 3 December 016 1 Introdction The classical wave eqation is a second-order

More information

PHASE PLANE DIAGRAMS OF DIFFERENCE EQUATIONS. 1. Introduction

PHASE PLANE DIAGRAMS OF DIFFERENCE EQUATIONS. 1. Introduction PHASE PLANE DIAGRAMS OF DIFFERENCE EQUATIONS TANYA DEWLAND, JEROME WESTON, AND RACHEL WEYRENS Abstract. We will be determining qalitatie featres of a discrete dynamical system of homogeneos difference

More information

The Linear Quadratic Regulator

The Linear Quadratic Regulator 10 The Linear Qadratic Reglator 10.1 Problem formlation This chapter concerns optimal control of dynamical systems. Most of this development concerns linear models with a particlarly simple notion of optimality.

More information

Study on the Mathematic Model of Product Modular System Orienting the Modular Design

Study on the Mathematic Model of Product Modular System Orienting the Modular Design Natre and Science, 2(, 2004, Zhong, et al, Stdy on the Mathematic Model Stdy on the Mathematic Model of Prodct Modlar Orienting the Modlar Design Shisheng Zhong 1, Jiang Li 1, Jin Li 2, Lin Lin 1 (1. College

More information

Low-emittance tuning of storage rings using normal mode beam position monitor calibration

Low-emittance tuning of storage rings using normal mode beam position monitor calibration PHYSIAL REVIEW SPEIAL TOPIS - AELERATORS AND BEAMS 4, 784 () Low-emittance tning of storage rings sing normal mode beam position monitor calibration A. Wolski* Uniersity of Lierpool, Lierpool, United Kingdom

More information

A Blue Lagoon Function

A Blue Lagoon Function Downloaded from orbit.dt.dk on: Oct 11, 2018 A Ble Lagoon Fnction Markorsen, Steen Pblication date: 2007 Link back to DTU Orbit Citation (APA): Markorsen, S., (2007). A Ble Lagoon Fnction General rights

More information

Sibuya s Measure of Local Dependence

Sibuya s Measure of Local Dependence Versão formatada segndo a reista Estadistica 5/dez/8 Sibya s Measre of Local Dependence SUMAIA ABDEL LATIF () PEDRO ALBERTO MORETTIN () () School of Arts, Science and Hmanities Uniersity of São Palo, Ra

More information

L 1 -smoothing for the Ornstein-Uhlenbeck semigroup

L 1 -smoothing for the Ornstein-Uhlenbeck semigroup L -smoothing for the Ornstein-Uhlenbeck semigrop K. Ball, F. Barthe, W. Bednorz, K. Oleszkiewicz and P. Wolff September, 00 Abstract Given a probability density, we estimate the rate of decay of the measre

More information

Velocity and Accceleration in Different Coordinate system

Velocity and Accceleration in Different Coordinate system Velocity & cceleration in different coordinate system Chapter Velocity and ccceleration in Different Coordinate system In physics basic laws are first introdced for a point partile and then laws are etended

More information

Bayes and Naïve Bayes Classifiers CS434

Bayes and Naïve Bayes Classifiers CS434 Bayes and Naïve Bayes Classifiers CS434 In this lectre 1. Review some basic probability concepts 2. Introdce a sefl probabilistic rle - Bayes rle 3. Introdce the learning algorithm based on Bayes rle (ths

More information

ANOVA INTERPRETING. It might be tempting to just look at the data and wing it

ANOVA INTERPRETING. It might be tempting to just look at the data and wing it Introdction to Statistics in Psychology PSY 2 Professor Greg Francis Lectre 33 ANalysis Of VAriance Something erss which thing? ANOVA Test statistic: F = MS B MS W Estimated ariability from noise and mean

More information

Online Stochastic Matching: New Algorithms and Bounds

Online Stochastic Matching: New Algorithms and Bounds Online Stochastic Matching: New Algorithms and Bonds Brian Brbach, Karthik A. Sankararaman, Araind Sriniasan, and Pan X Department of Compter Science, Uniersity of Maryland, College Park, MD 20742, USA

More information

Digital Image Processing. Lecture 8 (Enhancement in the Frequency domain) Bu-Ali Sina University Computer Engineering Dep.

Digital Image Processing. Lecture 8 (Enhancement in the Frequency domain) Bu-Ali Sina University Computer Engineering Dep. Digital Image Processing Lectre 8 Enhancement in the Freqenc domain B-Ali Sina Uniersit Compter Engineering Dep. Fall 009 Image Enhancement In The Freqenc Domain Otline Jean Baptiste Joseph Forier The

More information

Discontinuous Fluctuation Distribution for Time-Dependent Problems

Discontinuous Fluctuation Distribution for Time-Dependent Problems Discontinos Flctation Distribtion for Time-Dependent Problems Matthew Hbbard School of Compting, University of Leeds, Leeds, LS2 9JT, UK meh@comp.leeds.ac.k Introdction For some years now, the flctation

More information

CONTENTS. INTRODUCTION MEQ curriculum objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4

CONTENTS. INTRODUCTION MEQ curriculum objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4 CONTENTS INTRODUCTION MEQ crriclm objectives for vectors (8% of year). page 2 What is a vector? What is a scalar? page 3, 4 VECTOR CONCEPTS FROM GEOMETRIC AND ALGEBRAIC PERSPECTIVES page 1 Representation

More information

Characterizations of probability distributions via bivariate regression of record values

Characterizations of probability distributions via bivariate regression of record values Metrika (2008) 68:51 64 DOI 10.1007/s00184-007-0142-7 Characterizations of probability distribtions via bivariate regression of record vales George P. Yanev M. Ahsanllah M. I. Beg Received: 4 October 2006

More information

CS 450: COMPUTER GRAPHICS VECTORS SPRING 2016 DR. MICHAEL J. REALE

CS 450: COMPUTER GRAPHICS VECTORS SPRING 2016 DR. MICHAEL J. REALE CS 45: COMPUTER GRPHICS VECTORS SPRING 216 DR. MICHEL J. RELE INTRODUCTION In graphics, we are going to represent objects and shapes in some form or other. First, thogh, we need to figre ot how to represent

More information

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students

BLOOM S TAXONOMY. Following Bloom s Taxonomy to Assess Students BLOOM S TAXONOMY Topic Following Bloom s Taonomy to Assess Stdents Smmary A handot for stdents to eplain Bloom s taonomy that is sed for item writing and test constrction to test stdents to see if they

More information

Friedel-pair based indexing method for 3DXRD

Friedel-pair based indexing method for 3DXRD riedel-pair based indexing method for 3DXD Marcin Moscicki, Haroldo Pinto, Thomas Lippmann, András Borbély, Anke. Pyzalla 3 Max-Planck-Institt für Eisenforschng GmbH, Max-Planck-Str.,4037 Düsseldorf,Germany

More information

Minimum-Latency Beaconing Schedule in Multihop Wireless Networks

Minimum-Latency Beaconing Schedule in Multihop Wireless Networks This fll text paper was peer reiewed at the direction of IEEE Commnications Society sbject matter experts for pblication in the IEEE INFOCOM 009 proceedings Minimm-Latency Beaconing Schedle in Mltihop

More information

Concept of Stress at a Point

Concept of Stress at a Point Washkeic College of Engineering Section : STRONG FORMULATION Concept of Stress at a Point Consider a point ithin an arbitraril loaded deformable bod Define Normal Stress Shear Stress lim A Fn A lim A FS

More information

Formal Methods for Deriving Element Equations

Formal Methods for Deriving Element Equations Formal Methods for Deriving Element Eqations And the importance of Shape Fnctions Formal Methods In previos lectres we obtained a bar element s stiffness eqations sing the Direct Method to obtain eact

More information

Chem 4501 Introduction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics. Fall Semester Homework Problem Set Number 10 Solutions

Chem 4501 Introduction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics. Fall Semester Homework Problem Set Number 10 Solutions Chem 4501 Introdction to Thermodynamics, 3 Credits Kinetics, and Statistical Mechanics Fall Semester 2017 Homework Problem Set Nmber 10 Soltions 1. McQarrie and Simon, 10-4. Paraphrase: Apply Eler s theorem

More information

Lecture 17 Errors in Matlab s Turbulence PSD and Shaping Filter Expressions

Lecture 17 Errors in Matlab s Turbulence PSD and Shaping Filter Expressions Lectre 7 Errors in Matlab s Trblence PSD and Shaping Filter Expressions b Peter J Sherman /7/7 [prepared for AERE 355 class] In this brief note we will show that the trblence power spectral densities (psds)

More information

SIMULATION OF TURBULENT FLOW AND HEAT TRANSFER OVER A BACKWARD-FACING STEP WITH RIBS TURBULATORS

SIMULATION OF TURBULENT FLOW AND HEAT TRANSFER OVER A BACKWARD-FACING STEP WITH RIBS TURBULATORS THERMAL SCIENCE, Year 011, Vol. 15, No. 1, pp. 45-55 45 SIMULATION OF TURBULENT FLOW AND HEAT TRANSFER OVER A BACKWARD-FACING STEP WITH RIBS TURBULATORS b Khdheer S. MUSHATET Mechanical Engineering Department,

More information

Numerical Model for Studying Cloud Formation Processes in the Tropics

Numerical Model for Studying Cloud Formation Processes in the Tropics Astralian Jornal of Basic and Applied Sciences, 5(2): 189-193, 211 ISSN 1991-8178 Nmerical Model for Stdying Clod Formation Processes in the Tropics Chantawan Noisri, Dsadee Skawat Department of Mathematics

More information

3 2D Elastostatic Problems in Cartesian Coordinates

3 2D Elastostatic Problems in Cartesian Coordinates D lastostatic Problems in Cartesian Coordinates Two dimensional elastostatic problems are discssed in this Chapter, that is, static problems of either plane stress or plane strain. Cartesian coordinates

More information

Workshop on Understanding and Evaluating Radioanalytical Measurement Uncertainty November 2007

Workshop on Understanding and Evaluating Radioanalytical Measurement Uncertainty November 2007 1833-3 Workshop on Understanding and Evalating Radioanalytical Measrement Uncertainty 5-16 November 007 Applied Statistics: Basic statistical terms and concepts Sabrina BARBIZZI APAT - Agenzia per la Protezione

More information

CHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES. George P. Yanev

CHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES. George P. Yanev Pliska Std. Math. Blgar. 2 (211), 233 242 STUDIA MATHEMATICA BULGARICA CHARACTERIZATIONS OF EXPONENTIAL DISTRIBUTION VIA CONDITIONAL EXPECTATIONS OF RECORD VALUES George P. Yanev We prove that the exponential

More information

Visualisations of Gussian and Mean Curvatures by Using Mathematica and webmathematica

Visualisations of Gussian and Mean Curvatures by Using Mathematica and webmathematica Visalisations of Gssian and Mean Cratres by Using Mathematica and webmathematica Vladimir Benić, B. sc., (benic@grad.hr), Sonja Gorjanc, Ph. D., (sgorjanc@grad.hr) Faclty of Ciil Engineering, Kačićea 6,

More information

ON THE SHAPES OF BILATERAL GAMMA DENSITIES

ON THE SHAPES OF BILATERAL GAMMA DENSITIES ON THE SHAPES OF BILATERAL GAMMA DENSITIES UWE KÜCHLER, STEFAN TAPPE Abstract. We investigate the for parameter family of bilateral Gamma distribtions. The goal of this paper is to provide a thorogh treatment

More information

The Real Stabilizability Radius of the Multi-Link Inverted Pendulum

The Real Stabilizability Radius of the Multi-Link Inverted Pendulum Proceedings of the 26 American Control Conference Minneapolis, Minnesota, USA, Jne 14-16, 26 WeC123 The Real Stabilizability Radis of the Mlti-Link Inerted Pendlm Simon Lam and Edward J Daison Abstract

More information

A Single Species in One Spatial Dimension

A Single Species in One Spatial Dimension Lectre 6 A Single Species in One Spatial Dimension Reading: Material similar to that in this section of the corse appears in Sections 1. and 13.5 of James D. Mrray (), Mathematical Biology I: An introction,

More information

The Faraday Induction Law and Field Transformations in Special Relativity

The Faraday Induction Law and Field Transformations in Special Relativity Apeiron, ol. 10, No., April 003 118 The Farada Indction Law and Field Transformations in Special Relatiit Aleander L. Kholmetskii Department of Phsics, elars State Uniersit, 4, F. Skorina Aene, 0080 Minsk

More information

L = 2 λ 2 = λ (1) In other words, the wavelength of the wave in question equals to the string length,

L = 2 λ 2 = λ (1) In other words, the wavelength of the wave in question equals to the string length, PHY 309 L. Soltions for Problem set # 6. Textbook problem Q.20 at the end of chapter 5: For any standing wave on a string, the distance between neighboring nodes is λ/2, one half of the wavelength. The

More information

Derivation of 2D Power-Law Velocity Distribution Using Entropy Theory

Derivation of 2D Power-Law Velocity Distribution Using Entropy Theory Entrop 3, 5, -3; doi:.339/e54 Article OPEN ACCESS entrop ISSN 99-43 www.mdpi.com/jornal/entrop Deriation of D Power-Law Velocit Distribtion Using Entrop Theor Vija P. Singh,, *, stao Marini 3 and Nicola

More information

Setting The K Value And Polarization Mode Of The Delta Undulator

Setting The K Value And Polarization Mode Of The Delta Undulator LCLS-TN-4- Setting The Vale And Polarization Mode Of The Delta Undlator Zachary Wolf, Heinz-Dieter Nhn SLAC September 4, 04 Abstract This note provides the details for setting the longitdinal positions

More information

Vectors. Vectors ( 向量 ) Representation of Vectors. Special Vectors. Equal vectors. Chapter 16

Vectors. Vectors ( 向量 ) Representation of Vectors. Special Vectors. Equal vectors. Chapter 16 Vectors ( 向量 ) Chapter 16 2D Vectors A vector is a line which has both magnitde and direction. For example, in a weather report yo may hear a statement like the wind is blowing at 25 knots ( 海浬 ) in the

More information

Part II. Martingale measres and their constrctions 1. The \First" and the \Second" fndamental theorems show clearly how \mar tingale measres" are impo

Part II. Martingale measres and their constrctions 1. The \First and the \Second fndamental theorems show clearly how \mar tingale measres are impo Albert N. Shiryaev (Stelov Mathematical Institte and Moscow State University) ESSENTIALS of the ARBITRAGE THEORY Part I. Basic notions and theorems of the \Arbitrage Theory" Part II. Martingale measres

More information

Math 1. 2-hours test May 13, 2017

Math 1. 2-hours test May 13, 2017 Math. -hors test May, 7 JE/JKL.5.7 Problem restart:with(plots): A fnction f of two real variables is for x, y, given by f:=(x,y)-y/(x^+y^); f x, y y x y f(x,y); y x y (.) (.) Qestion In the x, y plane

More information

Technical Note. ODiSI-B Sensor Strain Gage Factor Uncertainty

Technical Note. ODiSI-B Sensor Strain Gage Factor Uncertainty Technical Note EN-FY160 Revision November 30, 016 ODiSI-B Sensor Strain Gage Factor Uncertainty Abstract Lna has pdated or strain sensor calibration tool to spport NIST-traceable measrements, to compte

More information

Lecture 9: 3.4 The Geometry of Linear Systems

Lecture 9: 3.4 The Geometry of Linear Systems Lectre 9: 3.4 The Geometry of Linear Systems Wei-Ta Ch 200/0/5 Dot Prodct Form of a Linear System Recall that a linear eqation has the form a x +a 2 x 2 + +a n x n = b (a,a 2,, a n not all zero) The corresponding

More information

Complex Tire-Ground Interaction Simulation: Recent Developments Of An Advanced Shell Theory Based Tire Model

Complex Tire-Ground Interaction Simulation: Recent Developments Of An Advanced Shell Theory Based Tire Model . ozdog and W. W. Olson Complex Tire-Grond Interaction Simlation: ecent eelopments Of n danced Shell Theory ased Tire odel EFEECE: ozdog. and Olson W. W. Complex Tire-Grond Interaction Simlation: ecent

More information

FEA Solution Procedure

FEA Solution Procedure EA Soltion Procedre (demonstrated with a -D bar element problem) EA Procedre for Static Analysis. Prepare the E model a. discretize (mesh) the strctre b. prescribe loads c. prescribe spports. Perform calclations

More information

Modelling, Simulation and Control of Quadruple Tank Process

Modelling, Simulation and Control of Quadruple Tank Process Modelling, Simlation and Control of Qadrple Tan Process Seran Özan, Tolgay Kara and Mehmet rıcı,, Electrical and electronics Engineering Department, Gaziantep Uniersity, Gaziantep, Trey bstract Simple

More information

A New Approach to Direct Sequential Simulation that Accounts for the Proportional Effect: Direct Lognormal Simulation

A New Approach to Direct Sequential Simulation that Accounts for the Proportional Effect: Direct Lognormal Simulation A ew Approach to Direct eqential imlation that Acconts for the Proportional ffect: Direct ognormal imlation John Manchk, Oy eangthong and Clayton Detsch Department of Civil & nvironmental ngineering University

More information

Primary dependent variable is fluid velocity vector V = V ( r ); where r is the position vector

Primary dependent variable is fluid velocity vector V = V ( r ); where r is the position vector Chapter 4: Flids Kinematics 4. Velocit and Description Methods Primar dependent ariable is flid elocit ector V V ( r ); where r is the position ector If V is known then pressre and forces can be determined

More information

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS SUBAREA I. COMPETENCY 1.0 UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS MECHANICS Skill 1.1 Calculating displacement, aerage elocity, instantaneous elocity, and acceleration in a gien frame of reference

More information

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls

Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis Functional Response and Feedback Controls Hindawi Pblishing Corporation Discrete Dynamics in Natre and Society Volme 2008 Article ID 149267 8 pages doi:101155/2008/149267 Research Article Permanence of a Discrete Predator-Prey Systems with Beddington-DeAngelis

More information

QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING

QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Jornal of the Korean Statistical Society 2007, 36: 4, pp 543 556 QUANTILE ESTIMATION IN SUCCESSIVE SAMPLING Hosila P. Singh 1, Ritesh Tailor 2, Sarjinder Singh 3 and Jong-Min Kim 4 Abstract In sccessive

More information

Linear System Theory (Fall 2011): Homework 1. Solutions

Linear System Theory (Fall 2011): Homework 1. Solutions Linear System Theory (Fall 20): Homework Soltions De Sep. 29, 20 Exercise (C.T. Chen: Ex.3-8). Consider a linear system with inpt and otpt y. Three experiments are performed on this system sing the inpts

More information

FRTN10 Exercise 12. Synthesis by Convex Optimization

FRTN10 Exercise 12. Synthesis by Convex Optimization FRTN Exercise 2. 2. We want to design a controller C for the stable SISO process P as shown in Figre 2. sing the Yola parametrization and convex optimization. To do this, the control loop mst first be

More information

Linear Strain Triangle and other types of 2D elements. By S. Ziaei Rad

Linear Strain Triangle and other types of 2D elements. By S. Ziaei Rad Linear Strain Triangle and other tpes o D elements B S. Ziaei Rad Linear Strain Triangle (LST or T6 This element is also called qadratic trianglar element. Qadratic Trianglar Element Linear Strain Triangle

More information

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : , PK K I N E M A T I C S Syllabs : Frame of reference. Motion in a straight line : Position-time graph, speed and velocity. Uniform and non-niform motion, average speed and instantaneos velocity. Uniformly

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com . Two smooth niform spheres S and T have eqal radii. The mass of S is 0. kg and the mass of T is 0.6 kg. The spheres are moving on a smooth horizontal plane and collide obliqely. Immediately before the

More information

Artificial Noise Revisited: When Eve Has more Antennas than Alice

Artificial Noise Revisited: When Eve Has more Antennas than Alice Artificial Noise Reisited: When e Has more Antennas than Alice Shiyin Li Yi Hong and manele Viterbo CS Department Monash Uniersity Melborne VIC 3800 Astralia mail: shiyin.li yi.hong emanele.iterbo@monash.ed

More information

MTH739U/P: Topics in Scientific Computing Autumn 2016 Week 6

MTH739U/P: Topics in Scientific Computing Autumn 2016 Week 6 MTH739U/P: Topics in Scientific Computing Autumn 16 Week 6 4.5 Generic algorithms for non-uniform variates We have seen that sampling from a uniform distribution in [, 1] is a relatively straightforward

More information

Lecture Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2

Lecture Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2 BIJU PATNAIK UNIVERSITY OF TECHNOLOGY, ODISHA Lectre Notes On THEORY OF COMPUTATION MODULE - 2 UNIT - 2 Prepared by, Dr. Sbhend Kmar Rath, BPUT, Odisha. Tring Machine- Miscellany UNIT 2 TURING MACHINE

More information

Microscopic Properties of Gases

Microscopic Properties of Gases icroscopic Properties of Gases So far we he seen the gas laws. These came from observations. In this section we want to look at a theory that explains the gas laws: The kinetic theory of gases or The kinetic

More information