Machine Learning and Rendering

Size: px
Start display at page:

Download "Machine Learning and Rendering"

Transcription

1 East Building, Balloom BC nvidia.com/siggaph2018 Machine Leaning and Rendeing Alex Kelle, Diecto of Reseach

2 Machine Leaning and Rendeing Couse web page at 14:00 Fom Machine Leaning to Gaphics and back Alexande Kelle, NVIDIA 14:40 Robust & Efficient Light Tanspot by Machine Leaning Jaoslav Křivánek, Chales Univesity, Pague 15:15 Deep Leaning fo Light Tanspot Simulation Jan Novàk, Disney Reseach 16:05 Neual Realtime Rendeing in Image Space Anton Kaplanyan, Facebook Reality Labs 16:40 Deep Realtime Rendeing Maco Salvi, NVIDIA 2

3 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw S 2 (x) P Camea 3

4 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw S 2 (x) Z cosq y = V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy P Camea 3

5 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw P Camea S 2 (x) Z cosq y = V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy Z Z = V (x 0,y)d x (x 0 )L i (x 0,w)f (w,x 0 cosq y,w)cosq x 0 V V x 0 y 2 dx0 dy L 3

6 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw P Camea S 2 (x) Z cosq y = V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy Z Z = V (x 0 c,y) lim B (x x 0 ) V V (x)!0 p(x) 2 L i (x 0,w)f (w,x 0 cosq y,w)cosq x 0 x 0 y 2 dx0 dy L 3

7 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw P Camea S 2 (x) = Z cosq y V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy = Z Z lim V (x 0,y) c B(x x 0 ) (x)!0 V V p(x) 2 L i (x 0,w)f (w,x 0 cosq,w)cosq x 0 y x 0 y 2 dx0 dy L 3

8 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw P Camea S 2 (x) Z cosq y = V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy Z Z c = lim B (x h(y,w)) (x)!0 V S 2 (y) p(x) 2 L i (h(y,w),w)f (w,h(y,w),w)cosq y dwdy L 3

9 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw P Camea S 2 (x) Z cosq y = V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy Z Z c = lim B (x h(y,w)) (x)!0 V S 2 (y) p(x) 2 L i (h(y,w),w)f (w,h(y,w),w)cosq y dwdy Z = L i (x,w)f (w,x,w)cosq x dw S 2 (x) L 3

10 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw P Camea S 2 (x) Z cosq y = V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy Z Z c = lim B (x h(y,w)) (x)!0 V S 2 (y) p(x) 2 L i (h(y,w),w)f (w,h(y,w),w)cosq y dwdy Z R B(x) = lim )L i (x 0,w)dx 0! R S 2 (x) (x)!0 B(x) w(x,x0 )dx 0 f (w,x,w)cosq x dw L 3

11 Moden Path Tacing Light tanspot simulation ways to fomulate the adiance L eflected in a suface point x L (x,w ) Z = L i (x,w)f (w,x,w)cosq x dw P Camea S 2 (x) Z cosq y = V (x,y)l i (x,w)f (w,x,w)cosq x V x y 2 dy Z Z c = lim B (x h(y,w)) (x)!0 V S 2 (y) p(x) 2 L i (h(y,w),w)f (w,h(y,w),w)cosq y dwdy Z R B(x) = lim )L i (x 0,w)dx 0 (x)!0 S 2 (x) RB(x) w(x,x0 )dx 0 f (w,x,w)cosq x dw L 3

12 Moden Path Tacing Light tanspot simulation path tacing: Stating paths fom camea and iteating scatteing and ay tacing bad fo small light souces, good fo lage light souces P P P 4

13 Moden Path Tacing Light tanspot simulation path tacing with next event estimation by shadow ays (dashed lines) good fo small light souces, bad fo close light souces P P P P P 4

14 Moden Path Tacing Light tanspot simulation light tacing, i.e. paths stating fom the light souce connected to the camea can captue some caustics, whee path tacing and next event estimation do not wok P P P P P P P P 4

15 Moden Path Tacing Light tanspot simulation all obvious ways to geneate light tanspot paths which ones ae good? P P P P P P P P P 4

16 Moden Path Tacing Light tanspot simulation bidiectional path tacing, optimally combining all techniques by weighting each contibution  l i=0 w l,i = 1 fo path length l 1, l 2 N w 1,1 P +w 1,0 P +w 2,2 P +w 2,1 P +w 2,0 P +w 3,3 P +w 3,2 P +w 3,1 P +w 3,0 P 4

17 Moden Path Tacing Light tanspot simulation bidiectional path tacing, optimally combining all techniques by weighting each contibution  l i=0 w l,i = 1 fo path length l 1, l 2 N w 1,1 P +w 1,0 P +w 2,2 P +w 2,1 P +w 2,0 P +w 3,3 P +w 3,2 P +w 3,1 P +w 3,0 P poblem of insufficient techniques, fo example, if only one wl,i 6= 0 4

18 Moden Path Tacing Numeical intego-appoximation Monte Calo methods Z g(y)= f (y,x)dx [0,1) s 5

19 Moden Path Tacing Numeical intego-appoximation Monte Calo methods Z g(y)= f (y,x)dx 1 [0,1) s n n  f (y,x i ) i=1 unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes 5

20 Moden Path Tacing Numeical intego-appoximation Monte Calo methods Z g(y)= f (y,x)dx 1 [0,1) s n n  f (y,x i ) i=1 unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes 5

21 Moden Path Tacing Numeical intego-appoximation Monte Calo methods Z g(y)= f (y,x)dx 1 [0,1) s n n  f (y,x i ) i=1 unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes 5

22 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes 5

23 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes 5

24 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes quasi-monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) 5

25 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes quasi-monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) much moe unifom coelated samples x i ealized by low-discepancy sequences, which ae pogessive Latin-hypecube samples 5

26 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes quasi-monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) much moe unifom coelated samples x i ealized by low-discepancy sequences, which ae pogessive Latin-hypecube samples 5

27 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes quasi-monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) much moe unifom coelated samples x i ealized by low-discepancy sequences, which ae pogessive Latin-hypecube samples 5

28 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes quasi-monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) much moe unifom coelated samples x i ealized by low-discepancy sequences, which ae pogessive Latin-hypecube samples 5

29 Moden Path Tacing Numeical intego-appoximation Monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) unifom, independent, unpedictable andom samples x i simulated by pseudo-andom numbes quasi-monte Calo methods g(y)= Z [0,1) s f (y,x)dx 1 n n  i=1 f (y,x i ) much moe unifom coelated samples x i ealized by low-discepancy sequences, which ae pogessive Latin-hypecube samples 5

30 Moden Path Tacing Pushbutton paadigm deteministic may impove speed of convegence epoducible and simple to paallelize 6

31 Moden Path Tacing Pushbutton paadigm deteministic may impove speed of convegence epoducible and simple to paallelize unbiased zeo diffeence between expectation and mathematical object not sufficient fo convegence 6

32 Moden Path Tacing Pushbutton paadigm deteministic may impove speed of convegence epoducible and simple to paallelize biased allows fo amelioating the poblem of insufficient techniques can temendously incease efficiency 6

33 Moden Path Tacing Pushbutton paadigm deteministic may impove speed of convegence epoducible and simple to paallelize biased allows fo amelioating the poblem of insufficient techniques can temendously incease efficiency consistent eo vanishes with inceasing set of samples no pesistent atifacts intoduced by algoithm I Quasi-Monte Calo image synthesis in a nutshell I The Iay light tanspot simulation and endeing system 6

34 Moden Path Tacing Pushbutton paadigm deteministic may impove speed of convegence epoducible and simple to paallelize biased allows fo amelioating the poblem of insufficient techniques can temendously incease efficiency consistent eo vanishes with inceasing set of samples no pesistent atifacts intoduced by algoithm I Quasi-Monte Calo image synthesis in a nutshell I The Iay light tanspot simulation and endeing system 6

35 Reconstuction fom noisy input: Massively paallel path space filteing (link)

36 Fom Machine Leaning to Gaphics

37 Machine Leaning Taxonomy unsupevised leaning fom unlabeled data examples: clusteing, auto-encode netwoks 9

38 Machine Leaning Taxonomy unsupevised leaning fom unlabeled data examples: clusteing, auto-encode netwoks semi-supevised leaning by ewads example: einfocement leaning 9

39 Machine Leaning Taxonomy unsupevised leaning fom unlabeled data examples: clusteing, auto-encode netwoks semi-supevised leaning by ewads example: einfocement leaning supevised leaning fom labeled data examples: suppot vecto machines, decision tees, atificial neual netwoks 9

40 Reinfocement Leaning Goal: maximize ewad state tansition yields ewad t+1 (a t s t ) 2 R Agent s t s t+1 t+1 (a t s t ) a t Envionment 10

41 Reinfocement Leaning Goal: maximize ewad state tansition yields ewad t+1 (a t s t ) 2 R Agent s t s t+1 t+1 (a t s t ) a t lean a policy pt to select an action a t 2 A(s t ) given the cuent state s t 2 S Envionment 10

42 Reinfocement Leaning Goal: maximize ewad state tansition yields ewad t+1 (a t s t ) 2 R Agent s t s t+1 t+1 (a t s t ) a t lean a policy pt to select an action a t 2 A(s t ) given the cuent state s t 2 S Envionment maximizing the discounted cumulative ewad V (s t ) Â g k t+1+k (a t+k s t+k ), whee 0 < g < 1 k=0 10

43 Reinfocement Leaning Q-Leaning [Watkins 1989] leans optimal action selection policy fo any given Makov decision pocess Q 0 (s,a) = (1 a) Q(s,a)+a (s,a)+g V (s 0 ) fo a leaning ate a 2 [0,1] 11

44 Reinfocement Leaning Q-Leaning [Watkins 1989] leans optimal action selection policy fo any given Makov decision pocess Q 0 (s,a) = (1 a) Q(s,a)+a (s,a)+g V (s 0 ) fo a leaning ate a 2 [0,1] with the following options fo the discounted cumulative ewad 8 max a 0 2A Q(s 0,a 0 ) conside best action in next state s 0 >< V (s 0 ) >: 11

45 Reinfocement Leaning Q-Leaning [Watkins 1989] leans optimal action selection policy fo any given Makov decision pocess Q 0 (s,a) = (1 a) Q(s,a)+a (s,a)+g V (s 0 ) fo a leaning ate a 2 [0,1] with the following options fo the discounted cumulative ewad 8 max a 0 2A Q(s 0,a 0 ) conside best action in next state s 0 >< V (s 0 ) Â a 0 2A p(s 0,a 0 )Q(s 0,a 0 ) policy weighted aveage ove discete action space >: 11

46 Reinfocement Leaning Q-Leaning [Watkins 1989] leans optimal action selection policy fo any given Makov decision pocess Q 0 (s,a) = (1 a) Q(s,a)+a (s,a)+g V (s 0 ) fo a leaning ate a 2 [0,1] with the following options fo the discounted cumulative ewad 8 max a 0 2A Q(s 0,a 0 ) conside best action in next state s 0 >< V (s 0 ) Â a 0 2A p(s 0,a 0 )Q(s 0,a 0 ) policy weighted aveage ove discete action space >: R A p(s0,a 0 )Q(s 0,a 0 )da 0 policy weighted aveage ove continuous action space 11

47 Reinfocement Leaning Maximize ewad by leaning impotance sampling online adiance integal equation L(x,w) = L e (x,w) + R S 2 +(x) f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i 12

48 Reinfocement Leaning Maximize ewad by leaning impotance sampling online stuctual equivalence of integal equation and Q-leaning L(x,w) = L e (x,w) + R S+(x) 2 f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i Q 0 (s,a) =(1 a)q(s,a)+a (s,a) + g R A p(s 0,a 0 ) Q(s 0,a 0 ) da 0 12

49 Reinfocement Leaning Maximize ewad by leaning impotance sampling online stuctual equivalence of integal equation and Q-leaning L(x,w) = L e (x,w) + R S+(x) 2 f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i Q 0 (s,a) = (1 a)q(s,a)+a (s,a) + g R A p(s 0,a 0 ) Q(s 0,a 0 ) da 0 12

50 Reinfocement Leaning Maximize ewad by leaning impotance sampling online stuctual equivalence of integal equation and Q-leaning L(x,w) = L e (x,w) + R S+(x) 2 f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i Q 0 (s,a) = (1 a)q(s,a)+a (s,a) + g R A p(s 0,a 0 ) Q(s 0,a 0 ) da 0 12

51 Reinfocement Leaning Maximize ewad by leaning impotance sampling online stuctual equivalence of integal equation and Q-leaning L(x,w) = L e (x,w) + R S+(x) 2 f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i Q 0 (s,a) = (1 a)q(s,a)+a (s,a) + g R A p(s 0,a 0 ) Q(s 0,a 0 ) da 0 12

52 Reinfocement Leaning Maximize ewad by leaning impotance sampling online stuctual equivalence of integal equation and Q-leaning L(x,w) = L e (x,w) + R S+(x) 2 f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i Q 0 (s,a) = (1 a)q(s,a)+a (s,a) + g R A p(s 0,a 0 ) Q(s 0,a 0 ) da 0 12

53 Reinfocement Leaning Maximize ewad by leaning impotance sampling online stuctual equivalence of integal equation and Q-leaning L(x,w) = L e (x,w) + R S+(x) 2 f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i Q 0 (s,a) =(1 a)q(s,a)+a (s,a) + g R A p(s 0,a 0 ) Q(s 0,a 0 ) da 0 gaphics example: leaning the incident adiance Z Q 0 (x,w)=(1 a)q(x,w)+a L e (y, w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i 12

54 Reinfocement Leaning Maximize ewad by leaning impotance sampling online stuctual equivalence of integal equation and Q-leaning L(x,w) = L e (x,w) + R S+(x) 2 f s (w i,x,w)cosq i L(h(x,w i ), w i ) dw i Q 0 (s,a) =(1 a)q(s,a)+a (s,a) + g R A p(s 0,a 0 ) Q(s 0,a 0 ) da 0 gaphics example: leaning the incident adiance Z Q 0 (x,w)=(1 a)q(x,w)+a L e (y, w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i to be used as a policy fo selecting an action w in state x to each the next state y := h(x,w) the leaning ate a is the only paamete left I Technical Note: Q-Leaning 12

55 Reinfocement Leaning Online algoithm fo guiding light tanspot paths Function pathtace(camea,scene) thoughput 1 ay setuppimayray(camea) fo i 0 to do y,n intesect(scene, ay) if isenvionment(y) then etun thoughput getradiancefomenvionment(ay,y) else if isaealight(y) etun thoughput getradiancefomaealight(ay,y) w,p w,f s samplebsdf(y,n) thoughput thoughput f s cos(n,w) / p w ay y, w 13

56 Reinfocement Leaning Online algoithm fo guiding light tanspot paths Function pathtace(camea,scene) thoughput 1 ay fo i y,n setuppimayray(camea) 0 to do if i > 0 then intesect(scene, ay) Q 0 (x,w)=(1 if isenvionment(y) then a)q(x,w)+a L e (y, w)+ RS 2+(y) f s(w i,y, w)cosq i Q(y,w i )dw i etun thoughput getradiancefomenvionment(ay,y) else if isaealight(y) w,p w,f s etun thoughput getradiancefomaealight(ay,y) thoughput ay y, w samplescatteingdiectionpopotionaltoq(y) thoughput f s cos(n,w) / p w 13

57 appoximate solution Q stoed on discetized hemisphees acoss scene suface

58 2048 paths taced with BRDF impotance sampling in a scene with challenging visibility

59 Path tacing with online einfocement leaning at the same numbe of paths

60 Metopolis light tanspot at the same numbe of paths

61 Reinfocement Leaning Guiding paths to whee the value Q comes fom shote expected path length damatically educed numbe of paths with zeo contibution vey efficient online leaning by leaning Q fom Q 18

62 Reinfocement Leaning Guiding paths to whee the value Q comes fom shote expected path length damatically educed numbe of paths with zeo contibution vey efficient online leaning by leaning Q fom Q diections fo eseach epesentation of value Q: data stuctues fom games impotance sampling popotional to the integand, i.e. the poduct of policy g p times value Q I On-line leaning of paametic mixtue models fo light tanspot simulation I Poduct impotance sampling fo light tanspot path guiding I Fast poduct impotance sampling of envionment maps I Leaning light tanspot the einfoced way I Pactical path guiding fo efficient light-tanspot simulation 18

63 Fom Gaphics back to Machine Leaning

64 Atificial Neual Netwoks in a Nutshell Supevised leaning of high dimensional function appoximation input laye a0, L 1 hidden layes, and output laye a L a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 20

65 Atificial Neual Netwoks in a Nutshell Supevised leaning of high dimensional function appoximation input laye a0, L 1 hidden layes, and output laye a L a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 n l ectified linea units (ReLU) a l,i =max{0,âw l,j,i a l 1,j } in laye l 20

66 Atificial Neual Netwoks in a Nutshell Supevised leaning of high dimensional function appoximation input laye a0, L 1 hidden layes, and output laye a L a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 n l ectified linea units (ReLU) a l,i =max{0,âw l,j,i a l 1,j } in laye l backpopagating the eo d l 1,i = Â al,j >0 d l,j w l,j,i 20

67 Atificial Neual Netwoks in a Nutshell Supevised leaning of high dimensional function appoximation input laye a0, L 1 hidden layes, and output laye a L a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 n l ectified linea units (ReLU) a l,i =max{0,âw l,j,i a l 1,j } in laye l backpopagating the eo d l 1,i = Â al,j >0 d l,j w l,j,i, update weights w 0 l,j,i = w l,j,i ld l,j a l 1,i if a l,j > 0 20

68 Atificial Neual Netwoks in a Nutshell Supevised leaning of high dimensional function appoximation example achitectues classifie I Multilaye feedfowad netwoks ae univesal appoximatos I Appoximation capabilities of multilaye feedfowad netwoks I Univesal appoximation bounds fo supepositions of a sigmoidal function 21

69 Atificial Neual Netwoks in a Nutshell Supevised leaning of high dimensional function appoximation example achitectues classifie geneato I Multilaye feedfowad netwoks ae univesal appoximatos I Appoximation capabilities of multilaye feedfowad netwoks I Univesal appoximation bounds fo supepositions of a sigmoidal function 21

70 Atificial Neual Netwoks in a Nutshell Supevised leaning of high dimensional function appoximation example achitectues classifie geneato auto-encode I Multilaye feedfowad netwoks ae univesal appoximatos I Appoximation capabilities of multilaye feedfowad netwoks I Univesal appoximation bounds fo supepositions of a sigmoidal function 21

71 Efficient Taining of Atificial Neual Netwoks Using an integal equation fo supevised leaning Q-leaning Q 0 (x,w)=(1 a)q(x,w)+a L e (y, Z w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i 22

72 Efficient Taining of Atificial Neual Netwoks Using an integal equation fo supevised leaning Q-leaning Q 0 (x,w)=(1 a)q(x,w)+a L e (y, Z w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i fo a = 1 yields the esidual, i.e. loss Z Q := Q(x,w) L e (y, w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i 22

73 Efficient Taining of Atificial Neual Netwoks Using an integal equation fo supevised leaning Q-leaning Q 0 (x,w)=(1 a)q(x,w)+a L e (y, Z w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i fo a = 1 yields the esidual, i.e. loss Z Q := Q(x,w) L e (y, w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i supevised leaning algoithm light tanspot paths geneated by a low discepancy sequence fo online taining 22

74 Efficient Taining of Atificial Neual Netwoks Using an integal equation fo supevised leaning Q-leaning Q 0 (x,w)=(1 a)q(x,w)+a L e (y, Z w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i fo a = 1 yields the esidual, i.e. loss Z Q := Q(x,w) L e (y, w)+ f s (w i,y, S+(y) 2 w)cosq i Q(y,w i )dw i supevised leaning algoithm light tanspot paths geneated by a low discepancy sequence fo online taining lean weights of an atificial neual netwok fo Q(x, n) by back-popagating loss of each path I A machine leaning diven sky model I Global illumination with adiance egession Functions I Machine leaning and integal equations I Neual impotance sampling 22

75 Efficient Taining of Atificial Neual Netwoks Leaning fom noisy/sampled labeled data find set of weights q of an atificial neual netwok f to minimize summed loss L using clean tagets y i and data ˆx i distibuted accoding to ˆx p(ˆx y i ) agmin q ÂL(f q (ˆx i ),y i ) i 23

76 Efficient Taining of Atificial Neual Netwoks Leaning fom noisy/sampled labeled data find set of weights q of an atificial neual netwok f to minimize summed loss L using clean tagets y i and data ˆx i distibuted accoding to ˆx p(ˆx y i ) agmin q ÂL(f q (ˆx i ),y i ) i using tagets ŷ i distibuted accoding to ŷ p(ŷ) instead agmin q ÂL(f q (ˆx i ),ŷ i ) i 23

77 Efficient Taining of Atificial Neual Netwoks Leaning fom noisy/sampled labeled data find set of weights q of an atificial neual netwok f to minimize summed loss L using clean tagets y i and data ˆx i distibuted accoding to ˆx p(ˆx y i ) agmin q ÂL(f q (ˆx i ),y i ) i using tagets ŷ i distibuted accoding to ŷ p(ŷ) instead agmin q ÂL(f q (ˆx i ),ŷ i ) i allows fo much faste taining of atificial neual netwoks used in simulations amounts to leaning integation and intego-appoximation I Noise2Noise: Leaning image estoation without clean data 23

78 Example Applications of Atificial Neual Netwoks in Rendeing Leaning fom noisy/sampled labeled data denoising quasi-monte Calo endeed images noisy tagets computed 2000 faste than clean tagets 24

79 Example Applications of Atificial Neual Netwoks in Rendeing Sampling accoding to a distibution given by obseved data geneative advesaial netwok (GAN) I image souce I Tutoial on GANs 25

80 Example Applications of Atificial Neual Netwoks in Rendeing Sampling accoding to a distibution given by obseved data geneative advesaial netwok (GAN) I image souce I Tutoial on GANs 25

81 Example Applications of Atificial Neual Netwoks in Rendeing Sampling accoding to a distibution given by obseved data geneative advesaial netwok (GAN) I image souce I Tutoial on GANs 25

82 Example Applications of Atificial Neual Netwoks in Rendeing Sampling accoding to a distibution given by obseved data geneative advesaial netwok (GAN) update geneato G using qg  m i=1 log(1 D(G(x i ))) I image souce I Tutoial on GANs 25

83 Example Applications of Atificial Neual Netwoks in Rendeing Sampling accoding to a distibution given by obseved data geneative advesaial netwok (GAN) update disciminato D (k times) using qd 1 m  m i=1 [log D(x i )+log(1 D(G(x i )))] update geneato G using qg  m i=1 log(1 D(G(x i ))) I image souce I Tutoial on GANs 25

84 Example Applications of Atificial Neual Netwoks in Rendeing Sampling accoding to a distibution given by obseved data Celebity GAN I Pogessive gowing of GANs fo impoved quality, stability, and vaiation 26

85 Example Applications of Atificial Neual Netwoks in Rendeing Replacing simulations by leaned pedictions fo moe efficiency much faste simulation of paticipating media hieachical stencil of volume densities as input to the neual netwok I Deep scatteing: Rendeing atmospheic clouds with adiance-pedicting neual netwoks I Leaning paticle physics by example: Acceleating science with geneative advesaial netwoks 27

86 Neual Netwoks linea in Time and Space

87 Neual Netwoks linea in Time and Space Complexity the bain about neve cells with to up to 10 4 connections to othes 29

88 Neual Netwoks linea in Time and Space Complexity the bain about neve cells with to up to 10 4 connections to othes atificial neual netwoks numbe of neual units L n = Â n l whee n l is the numbe of neuons in laye l l=1 29

89 Neual Netwoks linea in Time and Space Complexity the bain about neve cells with to up to 10 4 connections to othes atificial neual netwoks numbe of neual units L n = Â n l whee n l is the numbe of neuons in laye l l=1 numbe of weights L n w = Â n l 1 n l l=1 29

90 Neual Netwoks linea in Time and Space Complexity the bain about neve cells with to up to 10 4 connections to othes atificial neual netwoks numbe of neual units L n = Â n l whee n l is the numbe of neuons in laye l l=1 numbe of weights L n w = Â c n l l=1 constain to constant numbe c of weights pe neuon 29

91 Neual Netwoks linea in Time and Space Complexity the bain about neve cells with to up to 10 4 connections to othes atificial neual netwoks numbe of neual units L n = Â n l whee n l is the numbe of neuons in laye l l=1 numbe of weights L n w = Â c n l = c n l=1 constain to constant numbe c of weights pe neuon to each complexity linea in n 29

92 Neual Netwoks linea in Time and Space Sampling popotional to the weights of the tained neual units patition of unit inteval by sums Pk := Â k j=1 w j of nomalized absolute weights 0 w 1 w 2 w m 1 P 0 P 1 P 2 P m 1 P m 30

93 Neual Netwoks linea in Time and Space Sampling popotional to the weights of the tained neual units patition of unit inteval by sums Pk := Â k j=1 w j of nomalized absolute weights 0 w 1 w 2 w m 1 P 0 P 1 P 2 P m 1 P m using a unifom andom vaiable x 2 [0,1) to select input i, P i 1 apple x < P i satisfying Pob({P i 1 apple x < P i })= w i 30

94 Neual Netwoks linea in Time and Space Sampling popotional to the weights of the tained neual units patition of unit inteval by sums Pk := Â k j=1 w j of nomalized absolute weights 0 w 1 w 2 w m 1 P 0 P 1 P 2 P m 1 P m using a unifom andom vaiable x 2 [0,1) to select input i, P i 1 apple x < P i satisfying Pob({P i 1 apple x < P i })= w i in fact deivation of quantization to tenay weights in { 1,0,+1} intege weights esult fom neuons efeenced moe than once elation to dop connect and dop out 30

95 Neual Netwoks linea in Time and Space Sampling popotional to the weights of the tained neual units Test Accuacy 0.6 LeNet on MNIST 0.4 LeNet on CIFAR-10 AlexNet on CIFAR Top-5 Accuacy AlexNet on ILSVRC12 Top-1 Accuacy AlexNet on ILSVRC Pecent of fully connected layes sampled 31

96 Neual Netwoks linea in Time and Space Sampling paths though netwoks complexity bounded by numbe of paths times depth L of netwok 32

97 Neual Netwoks linea in Time and Space Sampling paths though netwoks complexity bounded by numbe of paths times depth L of netwok application afte taining backwads andom walks using sampling popotional to the weights of a neuon compession and quantization by impotance sampling 32

98 Neual Netwoks linea in Time and Space Sampling paths though netwoks complexity bounded by numbe of paths times depth L of netwok application afte taining backwads andom walks using sampling popotional to the weights of a neuon compession and quantization by impotance sampling application befoe taining unifom (bidiectional) andom walks to connect inputs and outputs spase fom scatch 32

99 Neual Netwoks linea in Time and Space Sampling paths though netwoks spase fom scatch a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 33

100 Neual Netwoks linea in Time and Space Sampling paths though netwoks spase fom scatch a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 33

101 Neual Netwoks linea in Time and Space Sampling paths though netwoks spase fom scatch a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 guaanteed connectivity I Monte Calo methods and neual netwoks 33

102 Neual Netwoks linea in Time and Space Sampling paths though netwoks spase fom scatch a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 guaanteed connectivity I Monte Calo methods and neual netwoks 33

103 Neual Netwoks linea in Time and Space Sampling paths though netwoks spase fom scatch a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 guaanteed connectivity I Monte Calo methods and neual netwoks 33

104 Neual Netwoks linea in Time and Space Sampling paths though netwoks spase fom scatch a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 guaanteed connectivity I Monte Calo methods and neual netwoks 33

105 Neual Netwoks linea in Time and Space Sampling paths though netwoks spase fom scatch a 0,0 a L,0 a 1,0 a 2,0 a 0,1 a L,1 a 1,1 a 2,1 a 0,2 a L,2. a 1,2. a 2,2.. a 0,n0 1 a L,nL 1 a 1,n1 1 a 2,n2 1 guaanteed connectivity and coveage I Monte Calo methods and neual netwoks 33

106 Neual Netwoks linea in Time and Space Test accuacy fo 4 laye feedfowad netwok (784/300/300/10) tained spase fom scatch Test Accuacy MNIST Fashion MNIST Numbe of pe pixel paths though netwok 34

107 Fom Machine Leaning to Gaphics and back Summay light tanspot and einfocement leaning descibed by same integal equation lean whee adiance comes fom neual netwoks esults of linea complexity by path tacing tenaization and quantization of tained atificial neual netwoks spase fom scatch taining 35

MULTILAYER PERCEPTRONS

MULTILAYER PERCEPTRONS Last updated: Nov 26, 2012 MULTILAYER PERCEPTRONS Outline 2 Combining Linea Classifies Leaning Paametes Outline 3 Combining Linea Classifies Leaning Paametes Implementing Logical Relations 4 AND and OR

More information

Path Tracing. Monte Carlo Path Tracing

Path Tracing. Monte Carlo Path Tracing Page 1 Monte Calo Path Tacing Today Path tacing Random wals and Maov chains Adjoint equations Light ay tacing Bidiectional ay tacing Next Heni Wann Jensen Iadiance caching Photon mapping Path Tacing Page

More information

4/18/2005. Statistical Learning Theory

4/18/2005. Statistical Learning Theory Statistical Leaning Theoy Statistical Leaning Theoy A model of supevised leaning consists of: a Envionment - Supplying a vecto x with a fixed but unknown pdf F x (x b Teache. It povides a desied esponse

More information

Chapter 8: Generalization and Function Approximation

Chapter 8: Generalization and Function Approximation Chapte 8: Genealization and Function Appoximation Objectives of this chapte: Look at how expeience with a limited pat of the state set be used to poduce good behavio ove a much lage pat. Oveview of function

More information

Value Prediction with FA. Chapter 8: Generalization and Function Approximation. Adapt Supervised Learning Algorithms. Backups as Training Examples [ ]

Value Prediction with FA. Chapter 8: Generalization and Function Approximation. Adapt Supervised Learning Algorithms. Backups as Training Examples [ ] Chapte 8: Genealization and Function Appoximation Objectives of this chapte:! Look at how expeience with a limited pat of the state set be used to poduce good behavio ove a much lage pat.! Oveview of function

More information

Regularization. Stephen Scott and Vinod Variyam. Introduction. Outline. Machine. Learning. Problems. Measuring. Performance.

Regularization. Stephen Scott and Vinod Variyam. Introduction. Outline. Machine. Learning. Problems. Measuring. Performance. leaning can geneally be distilled to an optimization poblem Choose a classifie (function, hypothesis) fom a set of functions that minimizes an objective function Clealy we want pat of this function to

More information

Numerical Integration

Numerical Integration MCEN 473/573 Chapte 0 Numeical Integation Fall, 2006 Textbook, 0.4 and 0.5 Isopaametic Fomula Numeical Integation [] e [ ] T k = h B [ D][ B] e B Jdsdt In pactice, the element stiffness is calculated numeically.

More information

A Deep Convolutional Neural Network Based on Nested Residue Number System

A Deep Convolutional Neural Network Based on Nested Residue Number System A Deep Convolutional Neual Netwok Based on Nested Residue Numbe System Hioki Nakahaa Ehime Univesity, Japan Tsutomu Sasao Meiji Univesity, Japan Abstact A pe-tained deep convolutional neual netwok (DCNN)

More information

MONTE CARLO STUDY OF PARTICLE TRANSPORT PROBLEM IN AIR POLLUTION. R. J. Papancheva, T. V. Gurov, I. T. Dimov

MONTE CARLO STUDY OF PARTICLE TRANSPORT PROBLEM IN AIR POLLUTION. R. J. Papancheva, T. V. Gurov, I. T. Dimov Pliska Stud. Math. Bulga. 14 (23), 17 116 STUDIA MATHEMATICA BULGARICA MOTE CARLO STUDY OF PARTICLE TRASPORT PROBLEM I AIR POLLUTIO R. J. Papancheva, T. V. Guov, I. T. Dimov Abstact. The actual tanspot

More information

Directed Regression. Benjamin Van Roy Stanford University Stanford, CA Abstract

Directed Regression. Benjamin Van Roy Stanford University Stanford, CA Abstract Diected Regession Yi-hao Kao Stanfod Univesity Stanfod, CA 94305 yihaoao@stanfod.edu Benjamin Van Roy Stanfod Univesity Stanfod, CA 94305 bv@stanfod.edu Xiang Yan Stanfod Univesity Stanfod, CA 94305 xyan@stanfod.edu

More information

Temporal-Difference Learning

Temporal-Difference Learning .997 Decision-Making in Lage-Scale Systems Mach 17 MIT, Sping 004 Handout #17 Lectue Note 13 1 Tempoal-Diffeence Leaning We now conside the poblem of computing an appopiate paamete, so that, given an appoximation

More information

COMP Parallel Computing SMM (3) OpenMP Case Study: The Barnes-Hut N-body Algorithm

COMP Parallel Computing SMM (3) OpenMP Case Study: The Barnes-Hut N-body Algorithm COMP 633 - Paallel Computing Lectue 8 Septembe 14, 2017 SMM (3) OpenMP Case Study: The Banes-Hut N-body Algoithm Topics Case study: the Banes-Hut algoithm Study an impotant algoithm in scientific computing»

More information

Identification of the degradation of railway ballast under a concrete sleeper

Identification of the degradation of railway ballast under a concrete sleeper Identification of the degadation of ailway ballast unde a concete sleepe Qin Hu 1) and Heung Fai Lam ) 1), ) Depatment of Civil and Achitectual Engineeing, City Univesity of Hong Kong, Hong Kong SAR, China.

More information

Prediction of Motion Trajectories Based on Markov Chains

Prediction of Motion Trajectories Based on Markov Chains 2011 Intenational Confeence on Compute Science and Infomation Technology (ICCSIT 2011) IPCSIT vol. 51 (2012) (2012) IACSIT Pess, Singapoe DOI: 10.7763/IPCSIT.2012.V51.50 Pediction of Motion Tajectoies

More information

Green s function Monte Carlo algorithms for elliptic problems

Green s function Monte Carlo algorithms for elliptic problems Mathematics and Computes in Simulation 63 (2003) 587 604 Geen s function Monte Calo algoithms fo elliptic poblems I.T. Dimov, R.Y. Papancheva Cental Laboatoy fo Paallel Pocessing, Depatment of Paallel

More information

Linear Program for Partially Observable Markov Decision Processes. MS&E 339B June 9th, 2004 Erick Delage

Linear Program for Partially Observable Markov Decision Processes. MS&E 339B June 9th, 2004 Erick Delage Linea Pogam fo Patiall Obsevable Makov Decision Pocesses MS&E 339B June 9th 2004 Eick Delage Intoduction Patiall Obsevable Makov Decision Pocesses Etension of the Makov Decision Pocess to a wold with uncetaint

More information

CSCE 478/878 Lecture 4: Experimental Design and Analysis. Stephen Scott. 3 Building a tree on the training set Introduction. Outline.

CSCE 478/878 Lecture 4: Experimental Design and Analysis. Stephen Scott. 3 Building a tree on the training set Introduction. Outline. In Homewok, you ae (supposedly) Choosing a data set 2 Extacting a test set of size > 3 3 Building a tee on the taining set 4 Testing on the test set 5 Repoting the accuacy (Adapted fom Ethem Alpaydin and

More information

Performance Loss Bounds for Approximate Value Iteration with State Aggregation

Performance Loss Bounds for Approximate Value Iteration with State Aggregation MATHEMATICS OF OPERATIONS RESEARCH Vol. 31, No. 2, May 2006, pp. 234 244 issn 0364-765X eissn 1526-5471 06 3102 0234 infoms doi 10.1287/moo.1060.0188 2006 INFORMS Pefomance Loss Bounds fo Appoximate Value

More information

Rydberg-Rydberg Interactions

Rydberg-Rydberg Interactions Rydbeg-Rydbeg Inteactions F. Robicheaux Aubun Univesity Rydbeg gas goes to plasma Dipole blockade Coheent pocesses in fozen Rydbeg gases (expts) Theoetical investigation of an excitation hopping though

More information

Classical Worm algorithms (WA)

Classical Worm algorithms (WA) Classical Wom algoithms (WA) WA was oiginally intoduced fo quantum statistical models by Pokof ev, Svistunov and Tupitsyn (997), and late genealized to classical models by Pokof ev and Svistunov (200).

More information

biologically-inspired computing lecture 9 Informatics luis rocha 2015 INDIANA UNIVERSITY biologically Inspired computing

biologically-inspired computing lecture 9 Informatics luis rocha 2015 INDIANA UNIVERSITY biologically Inspired computing luis ocha 25 lectue 9 -inspied luis ocha 25 Sections I485/H4 couse outlook Assignments: 35% Students will complete 4/5 assignments based on algoithms pesented in class Lab meets in I (West) 9 on Lab Wednesdays

More information

Structured Prediction with Adversarial Constraint Learning

Structured Prediction with Adversarial Constraint Learning Stuctued Pediction with Advesaial Constaint Leaning Hongyu Ren Peking Univesity hy@pku.edu.cn Russell Stewat Stanfod Univesity stewat@cs.stanfod.edu Jiaming Song Stanfod Univesity tsong@cs.stanfod.edu

More information

MAPPING LARGE PARALLEL SIMULATION PROGRAMS TO MULTICOMPUTER SYSTEMS

MAPPING LARGE PARALLEL SIMULATION PROGRAMS TO MULTICOMPUTER SYSTEMS A.Tentne (ed.): High Pefomance Computing 1994, Poc. of the SCS Simulation Multiconfeence 1994, San Diego, 11.-15. Apil 1994. S. 285-290. MAPPING LARGE PARALLEL SIMULATION PROGRAMS TO MULTICOMPUTER SYSTEMS

More information

Interaction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r)

Interaction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r) Supplementay mateial fo Inteaction of Feedfowad and Feedback Steams in Visual Cotex in a Fiing-Rate Model of Columna Computations Tobias Bosch and Heiko Neumann Institute fo Neual Infomation Pocessing

More information

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in

More information

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS DOING PHYIC WITH MTLB COMPUTTIONL OPTIC FOUNDTION OF CLR DIFFRCTION THEORY Ian Coope chool of Physics, Univesity of ydney ian.coope@sydney.edu.au DOWNLOD DIRECTORY FOR MTLB CRIPT View document: Numeical

More information

Kunming, , R.P. China. Kunming, , R.P. China. *Corresponding author: Jianing He

Kunming, , R.P. China. Kunming, , R.P. China. *Corresponding author: Jianing He Applied Mechanics and Mateials Online: 2014-04-28 ISSN: 1662-7482, Vol. 540, pp 92-95 doi:10.4028/www.scientific.net/amm.540.92 2014 Tans Tech Publications, Switzeland Reseach on Involute Gea Undecutting

More information

THE STUDY AND IMPROVEMENT OF X-BAND ATTENUATION ESTIMATION USING DUAL POLARIMETRIC RADAR TECHNIQUES

THE STUDY AND IMPROVEMENT OF X-BAND ATTENUATION ESTIMATION USING DUAL POLARIMETRIC RADAR TECHNIQUES THE STUDY AND IMPROVEMENT OF X-BAND ATTENUATION ESTIMATION USING DUAL POLARIMETRIC RADAR TECHNIQUES Yuxiang Liu Advisos: V.N. Bingi and V. Chandaseka Decembe 4, 006 T ct } ) ( ) ( 4 ln exp{ ), ( 1 0 1

More information

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS

COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS Pogess In Electomagnetics Reseach, PIER 73, 93 105, 2007 COMPUTATIONS OF ELECTROMAGNETIC FIELDS RADIATED FROM COMPLEX LIGHTNING CHANNELS T.-X. Song, Y.-H. Liu, and J.-M. Xiong School of Mechanical Engineeing

More information

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India

More information

PAPER 39 STOCHASTIC NETWORKS

PAPER 39 STOCHASTIC NETWORKS MATHEMATICAL TRIPOS Pat III Tuesday, 2 June, 2015 1:30 pm to 4:30 pm PAPER 39 STOCHASTIC NETWORKS Attempt no moe than FOUR questions. Thee ae FIVE questions in total. The questions cay equal weight. STATIONERY

More information

Bayesian Congestion Control over a Markovian Network Bandwidth Process

Bayesian Congestion Control over a Markovian Network Bandwidth Process Bayesian Congestion Contol ove a Makovian Netwok Bandwidth Pocess Paisa Mansouifad,, Bhaska Kishnamachai, Taa Javidi Ming Hsieh Depatment of Electical Engineeing, Univesity of Southen Califonia, Los Angeles,

More information

Information Retrieval Advanced IR models. Luca Bondi

Information Retrieval Advanced IR models. Luca Bondi Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the

More information

C e f paamete adaptation f (' x) ' ' d _ d ; ; e _e K p K v u ^M() RBF NN ^h( ) _ obot s _ s n W ' f x x xm xm f x xm d Figue : Block diagam of comput

C e f paamete adaptation f (' x) ' ' d _ d ; ; e _e K p K v u ^M() RBF NN ^h( ) _ obot s _ s n W ' f x x xm xm f x xm d Figue : Block diagam of comput A Neual-Netwok Compensato with Fuzzy Robustication Tems fo Impoved Design of Adaptive Contol of Robot Manipulatos Y.H. FUNG and S.K. TSO Cente fo Intelligent Design, Automation and Manufactuing City Univesity

More information

AP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws.

AP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws. AP-C WEP 1. Wok a. Calculate the wok done by a specified constant foce on an object that undegoes a specified displacement. b. Relate the wok done by a foce to the aea unde a gaph of foce as a function

More information

Outline. Reinforcement Learning. What is RL? Reinforcement learning is learning what to do so as to maximize a numerical reward signal

Outline. Reinforcement Learning. What is RL? Reinforcement learning is learning what to do so as to maximize a numerical reward signal Otine Reinfocement Leaning Jne, 005 CS 486/686 Univesity of Wateoo Rsse & Novig Sect.-. What is einfocement eaning Tempoa-Diffeence eaning Q-eaning Machine Leaning Spevised Leaning Teache tes eane what

More information

An extended target tracking method with random finite set observations

An extended target tracking method with random finite set observations 4th Intenational Confeence on Infomation Fusion Chicago Illinois USA July 5-8 0 An extended taget tacing method with andom finite set obsevations Hongyan Zhu Chongzhao Han Chen Li Dept. of Electonic &

More information

Chapter 13 Gravitation

Chapter 13 Gravitation Chapte 13 Gavitation In this chapte we will exploe the following topics: -Newton s law of gavitation, which descibes the attactive foce between two point masses and its application to extended objects

More information

Coarse Mesh Radiation Transport Code COMET Radiation Therapy Application*

Coarse Mesh Radiation Transport Code COMET Radiation Therapy Application* Coase Mesh Radiation Tanspot Code COMT Radiation Theapy Application* Fazad Rahnema Nuclea & Radiological ngineeing and Medical Physics Pogams Geogia Institute of Technology Computational Medical Physics

More information

Alignment of the ZEUS Micro- Vertex Detector Using Cosmic Tracks

Alignment of the ZEUS Micro- Vertex Detector Using Cosmic Tracks Alignment of the ZEUS Mico- Vetex etecto Using Cosmic acks akanoi Kohno (Univesity of Oxfod), ZEUS MV Goup Intenational Wokshop on Advanced Computing and Analysis echniques in Physics Reseach (ACA5) ESY,

More information

Analysis of spatial correlations in marked point processes

Analysis of spatial correlations in marked point processes Analysis of spatial coelations in maked point pocesses with application to micogeogaphic economical data Joint wok with W. Bachat-Schwaz, F. Fleische, P. Gabanik, V. Schmidt and W. Walla Stefanie Eckel

More information

A Machine Learned Model of a Hybrid Aircraft

A Machine Learned Model of a Hybrid Aircraft 1 A Machine Leaned Model of a Hybid Aicaft Bandon Jones, Kevin Jenkins CS229 Machine Leaning, Fall 2016, Stanfod Univesity I. INTRODUCTION Aicaft development pogams ely on aicaft dynamic models fo flight

More information

Macro Theory B. The Permanent Income Hypothesis

Macro Theory B. The Permanent Income Hypothesis Maco Theoy B The Pemanent Income Hypothesis Ofe Setty The Eitan Beglas School of Economics - Tel Aviv Univesity May 15, 2015 1 1 Motivation 1.1 An econometic check We want to build an empiical model with

More information

Empirical Prediction of Fitting Densities in Industrial Workrooms for Ray Tracing. 1 Introduction. 2 Ray Tracing using DRAYCUB

Empirical Prediction of Fitting Densities in Industrial Workrooms for Ray Tracing. 1 Introduction. 2 Ray Tracing using DRAYCUB Empiical Pediction of Fitting Densities in Industial Wokooms fo Ray Tacing Katina Scheebnyj, Muay Hodgson Univesity of Bitish Columbia, SOEH-MECH, Acoustics and Noise Reseach Goup, 226 East Mall, Vancouve,

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

Gradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function

Gradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function Intenational Confeence on Infomation echnology and Management Innovation (ICIMI 05) Gadient-based Neual Netwok fo Online Solution of Lyapunov Matix Equation with Li Activation unction Shiheng Wang, Shidong

More information

Gauss Law. Physics 231 Lecture 2-1

Gauss Law. Physics 231 Lecture 2-1 Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

More information

Numerical solution of diffusion mass transfer model in adsorption systems. Prof. Nina Paula Gonçalves Salau, D.Sc.

Numerical solution of diffusion mass transfer model in adsorption systems. Prof. Nina Paula Gonçalves Salau, D.Sc. Numeical solution of diffusion mass tansfe model in adsoption systems Pof., D.Sc. Agenda Mass Tansfe Mechanisms Diffusion Mass Tansfe Models Solving Diffusion Mass Tansfe Models Paamete Estimation 2 Mass

More information

Conjugate Gradient Methods. Michael Bader. Summer term 2012

Conjugate Gradient Methods. Michael Bader. Summer term 2012 Gadient Methods Outlines Pat I: Quadatic Foms and Steepest Descent Pat II: Gadients Pat III: Summe tem 2012 Pat I: Quadatic Foms and Steepest Descent Outlines Pat I: Quadatic Foms and Steepest Descent

More information

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology Electomagnetic scatteing Gaduate Couse Electical Engineeing (Communications) 1 st Semeste, 1390-1391 Shaif Univesity of Technology Geneal infomation Infomation about the instucto: Instucto: Behzad Rejaei

More information

1 Explicit Explore or Exploit (E 3 ) Algorithm

1 Explicit Explore or Exploit (E 3 ) Algorithm 2.997 Decision-Making in Lage-Scale Systems Mach 3 MIT, Sping 2004 Handout #2 Lectue Note 9 Explicit Exploe o Exploit (E 3 ) Algoithm Last lectue, we studied the Q-leaning algoithm: [ ] Q t+ (x t, a t

More information

Lead field theory and the spatial sensitivity of scalp EEG Thomas Ferree and Matthew Clay July 12, 2000

Lead field theory and the spatial sensitivity of scalp EEG Thomas Ferree and Matthew Clay July 12, 2000 Lead field theoy and the spatial sensitivity of scalp EEG Thomas Feee and Matthew Clay July 12, 2000 Intoduction Neuonal population activity in the human cotex geneates electic fields which ae measuable

More information

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Study Rev. Adv. on -D Mate. shock Sci. wave 33 (13) pessue 111-118 model in mico scale lase shock peening 111 STUDY ON -D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Y.J. Fan 1, J.Z. Zhou,

More information

Welcome to Physics 272

Welcome to Physics 272 Welcome to Physics 7 Bob Mose mose@phys.hawaii.edu http://www.phys.hawaii.edu/~mose/physics7.html To do: Sign into Masteing Physics phys-7 webpage Registe i-clickes (you i-clicke ID to you name on class-list)

More information

MONTE CARLO SIMULATION OF FLUID FLOW

MONTE CARLO SIMULATION OF FLUID FLOW MONTE CARLO SIMULATION OF FLUID FLOW M. Ragheb 3/7/3 INTRODUCTION We conside the situation of Fee Molecula Collisionless and Reflective Flow. Collisionless flows occu in the field of aefied gas dynamics.

More information

Physics 235 Chapter 5. Chapter 5 Gravitation

Physics 235 Chapter 5. Chapter 5 Gravitation Chapte 5 Gavitation In this Chapte we will eview the popeties of the gavitational foce. The gavitational foce has been discussed in geat detail in you intoductoy physics couses, and we will pimaily focus

More information

7.2. Coulomb s Law. The Electric Force

7.2. Coulomb s Law. The Electric Force Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat

More information

A Markov Decision Approach for the Computation of Testability of RTL Constructs

A Markov Decision Approach for the Computation of Testability of RTL Constructs A Makov Decision Appoach fo the Computation of Testability of RTL Constucts José Miguel Fenandes Abstact In the analysis of digital cicuits, to study testability estimation measues, dissipated powe and

More information

INTRODUCTION. 2. Vectors in Physics 1

INTRODUCTION. 2. Vectors in Physics 1 INTRODUCTION Vectos ae used in physics to extend the study of motion fom one dimension to two dimensions Vectos ae indispensable when a physical quantity has a diection associated with it As an example,

More information

Internet Appendix for A Bayesian Approach to Real Options: The Case of Distinguishing Between Temporary and Permanent Shocks

Internet Appendix for A Bayesian Approach to Real Options: The Case of Distinguishing Between Temporary and Permanent Shocks Intenet Appendix fo A Bayesian Appoach to Real Options: The Case of Distinguishing Between Tempoay and Pemanent Shocks Steven R. Genadie Gaduate School of Business, Stanfod Univesity Andey Malenko Gaduate

More information

arxiv: v1 [physics.gen-ph] 18 Aug 2018

arxiv: v1 [physics.gen-ph] 18 Aug 2018 Path integal and Sommefeld quantization axiv:1809.04416v1 [physics.gen-ph] 18 Aug 018 Mikoto Matsuda 1, and Takehisa Fujita, 1 Japan Health and Medical technological college, Tokyo, Japan College of Science

More information

Gauss s Law Simulation Activities

Gauss s Law Simulation Activities Gauss s Law Simulation Activities Name: Backgound: The electic field aound a point chage is found by: = kq/ 2 If thee ae multiple chages, the net field at any point is the vecto sum of the fields. Fo a

More information

Experience Selection in Deep Reinforcement Learning for Control

Experience Selection in Deep Reinforcement Learning for Control Jounal of Machine Leaning Reseach 19 (2018) 1-56 Submitted 3/17; Revised 07/18; Published 08/18 Expeience Selection in Deep Reinfocement Leaning fo Contol Tim de Buin Jens Kobe Cognitive Robotics Depatment

More information

Stellar Structure and Evolution

Stellar Structure and Evolution Stella Stuctue and Evolution Theoetical Stella odels Conside each spheically symmetic shell of adius and thickness d. Basic equations of stella stuctue ae: 1 Hydostatic equilibium π dp dp d G π = G =.

More information

PHYS 172: Modern Mechanics. Summer Lecture 4 The Momentum Principle & Predicting Motion Read

PHYS 172: Modern Mechanics. Summer Lecture 4 The Momentum Principle & Predicting Motion Read PHYS 172: Moden Mechanics Summe 2010 Δp sys = F net Δt ΔE = W + Q sys su su ΔL sys = τ net Δt Lectue 4 The Momentum Pinciple & Pedicting Motion Read 2.6-2.9 READING QUESTION #1 Reading Question Which of

More information

Web-based Supplementary Materials for. Controlling False Discoveries in Multidimensional Directional Decisions, with

Web-based Supplementary Materials for. Controlling False Discoveries in Multidimensional Directional Decisions, with Web-based Supplementay Mateials fo Contolling False Discoveies in Multidimensional Diectional Decisions, with Applications to Gene Expession Data on Odeed Categoies Wenge Guo Biostatistics Banch, National

More information

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D.

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D. Reseach Design - - Topic 7 Multiple Regession & Multiple Coelation: Two Pedictos 009 R.C. Gadne, Ph.D. Geneal Rationale and Basic Aithmetic fo two pedictos Patial and semipatial coelation Regession coefficients

More information

1D2G - Numerical solution of the neutron diffusion equation

1D2G - Numerical solution of the neutron diffusion equation DG - Numeical solution of the neuton diffusion equation Y. Danon Daft: /6/09 Oveview A simple numeical solution of the neuton diffusion equation in one dimension and two enegy goups was implemented. Both

More information

Computational Methods of Solid Mechanics. Project report

Computational Methods of Solid Mechanics. Project report Computational Methods of Solid Mechanics Poject epot Due on Dec. 6, 25 Pof. Allan F. Bowe Weilin Deng Simulation of adhesive contact with molecula potential Poject desciption In the poject, we will investigate

More information

The Substring Search Problem

The Substring Search Problem The Substing Seach Poblem One algoithm which is used in a vaiety of applications is the family of substing seach algoithms. These algoithms allow a use to detemine if, given two chaacte stings, one is

More information

An Exact Solution of Navier Stokes Equation

An Exact Solution of Navier Stokes Equation An Exact Solution of Navie Stokes Equation A. Salih Depatment of Aeospace Engineeing Indian Institute of Space Science and Technology, Thiuvananthapuam, Keala, India. July 20 The pincipal difficulty in

More information

International Journal of Mathematical Archive-3(12), 2012, Available online through ISSN

International Journal of Mathematical Archive-3(12), 2012, Available online through  ISSN Intenational Jounal of Mathematical Achive-3(), 0, 480-4805 Available online though www.ijma.info ISSN 9 504 STATISTICAL QUALITY CONTROL OF MULTI-ITEM EOQ MOEL WITH VARYING LEAING TIME VIA LAGRANGE METHO

More information

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012

Stanford University CS259Q: Quantum Computing Handout 8 Luca Trevisan October 18, 2012 Stanfod Univesity CS59Q: Quantum Computing Handout 8 Luca Tevisan Octobe 8, 0 Lectue 8 In which we use the quantum Fouie tansfom to solve the peiod-finding poblem. The Peiod Finding Poblem Let f : {0,...,

More information

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1

AST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1 Please ead this fist... AST S: The oigin and evolution of the Univese Intoduction to Mathematical Handout This is an unusually long hand-out and one which uses in places mathematics that you may not be

More information

Kinetic Simulation of Air Flow Around Hollow Cylinder Flare Configuration

Kinetic Simulation of Air Flow Around Hollow Cylinder Flare Configuration 3nd AIAA Fluid Dynamics Confeence and Exhibit 4-6 June 00, St. Louis, Missoui AIAA 00-399 Kinetic Simulation of Ai Flow Aound Hollow Cylinde Flae Configuation Valeiy M. Tenishev * Depatment of Atmospheic,

More information

EVOLUTIONARY COMPUTING FOR METALS PROPERTIES MODELLING

EVOLUTIONARY COMPUTING FOR METALS PROPERTIES MODELLING EVOLUTIONARY COMPUTING FOR METALS PROPERTIES MODELLING M.F. Abbod*, M. Mahfouf, D.A. Linkens and Sellas, C.M. IMMPETUS Institute fo Micostuctue and Mechanical Popeties Engineeing, The Univesity of Sheffield

More information

Lecture 8 - Gauss s Law

Lecture 8 - Gauss s Law Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.

More information

Revision of Lecture Eight

Revision of Lecture Eight Revision of Lectue Eight Baseband equivalent system and equiements of optimal tansmit and eceive filteing: (1) achieve zeo ISI, and () maximise the eceive SNR Thee detection schemes: Theshold detection

More information

Geometry and statistics in turbulence

Geometry and statistics in turbulence Geomety and statistics in tubulence Auoe Naso, Univesity of Twente, Misha Chetkov, Los Alamos, Bois Shaiman, Santa Babaa, Alain Pumi, Nice. Tubulent fluctuations obey a complex dynamics, involving subtle

More information

Review for Midterm-1

Review for Midterm-1 Review fo Midtem-1 Midtem-1! Wednesday Sept. 24th at 6pm Section 1 (the 4:10pm class) exam in BCC N130 (Business College) Section 2 (the 6:00pm class) exam in NR 158 (Natual Resouces) Allowed one sheet

More information

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum

2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum 2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known

More information

Section 11. Timescales Radiation transport in stars

Section 11. Timescales Radiation transport in stars Section 11 Timescales 11.1 Radiation tanspot in stas Deep inside stas the adiation eld is vey close to black body. Fo a black-body distibution the photon numbe density at tempeatue T is given by n = 2

More information

3.1 Random variables

3.1 Random variables 3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated

More information

6 Matrix Concentration Bounds

6 Matrix Concentration Bounds 6 Matix Concentation Bounds Concentation bounds ae inequalities that bound pobabilities of deviations by a andom vaiable fom some value, often its mean. Infomally, they show the pobability that a andom

More information

Velocimetry Techniques and Instrumentation

Velocimetry Techniques and Instrumentation AeE 344 Lectue Notes Lectue # 05: elocimety Techniques and Instumentation D. Hui Hu Depatment of Aeospace Engineeing Iowa State Univesity Ames, Iowa 500, U.S.A Methods to Measue Local Flow elocity - Mechanical

More information

An Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications

An Adaptive Neural-Network Model-Following Speed Control of PMSM Drives for Electric Vehicle Applications Poceedings of the 9th WSEAS Intenational Confeence on Applied Mathematics, Istanbul, Tuey, May 27-29, 2006 (pp412-417) An Adaptive Neual-Netwo Model-Following Speed Contol of PMSM Dives fo Electic Vehicle

More information

This is a very simple sampling mode, and this article propose an algorithm about how to recover x from y in this condition.

This is a very simple sampling mode, and this article propose an algorithm about how to recover x from y in this condition. 3d Intenational Confeence on Multimedia echnology(icm 03) A Simple Compessive Sampling Mode and the Recovey of Natue Images Based on Pixel Value Substitution Wenping Shao, Lin Ni Abstact: Compessive Sampling

More information

Chapter 4. Newton s Laws of Motion. Newton s Law of Motion. Sir Isaac Newton ( ) published in 1687

Chapter 4. Newton s Laws of Motion. Newton s Law of Motion. Sir Isaac Newton ( ) published in 1687 Chapte 4 Newton s Laws of Motion 1 Newton s Law of Motion Si Isaac Newton (1642 1727) published in 1687 2 1 Kinematics vs. Dynamics So fa, we discussed kinematics (chaptes 2 and 3) The discussion, was

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.

More information

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions

More information

Multi-Objective Optimization Algorithms for Finite Element Model Updating

Multi-Objective Optimization Algorithms for Finite Element Model Updating Multi-Objective Optimization Algoithms fo Finite Element Model Updating E. Ntotsios, C. Papadimitiou Univesity of Thessaly Geece Outline STRUCTURAL IDENTIFICATION USING MEASURED MODAL DATA Weighted Modal

More information

TELE4652 Mobile and Satellite Communications

TELE4652 Mobile and Satellite Communications Mobile and Satellite Communications Lectue 3 Radio Channel Modelling Channel Models If one was to walk away fom a base station, and measue the powe level eceived, a plot would like this: Channel Models

More information

Analytical Expressions for Positioning Uncertainty Propagation in Networks of Robots

Analytical Expressions for Positioning Uncertainty Propagation in Networks of Robots Analytical Expessions fo Positioning Uncetainty Popagation in Netwoks of Robots Ioannis M Rekleitis and Stegios I Roumeliotis Abstact In this pape we pesent an analysis of the positioning uncetainty incease

More information

Conservative Averaging Method and its Application for One Heat Conduction Problem

Conservative Averaging Method and its Application for One Heat Conduction Problem Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem

More information

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1) EM- Coulomb s law, electic field, potential field, supeposition q ' Electic field of a point chage ( ') E( ) kq, whee k / 4 () ' Foce of q on a test chage e at position is ee( ) Electic potential O kq

More information

Forecasting Agricultural Commodity Prices Using Multivariate Bayesian Machine Learning. Andres M. Ticlavilca, Dillon M. Feuz, and Mac McKee

Forecasting Agricultural Commodity Prices Using Multivariate Bayesian Machine Learning. Andres M. Ticlavilca, Dillon M. Feuz, and Mac McKee Foecasting Agicultual Commodity Pices Using Multivaiate Bayesian Machine Leaning Regession by Andes M. Ticlavilca, Dillon M. Feuz, and Mac McKee Suggested citation fomat: Ticlavilca, A. M., Dillon M. Feuz

More information

Physics 181. Assignment 4

Physics 181. Assignment 4 Physics 181 Assignment 4 Solutions 1. A sphee has within it a gavitational field given by g = g, whee g is constant and is the position vecto of the field point elative to the cente of the sphee. This

More information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information

Title. Author(s)Y. IMAI; T. TSUJII; S. MOROOKA; K. NOMURA. Issue Date Doc URL. Type. Note. File Information Title CALCULATION FORULAS OF DESIGN BENDING OENTS ON TH APPLICATION OF THE SAFETY-ARGIN FRO RC STANDARD TO Autho(s)Y. IAI; T. TSUJII; S. OROOKA; K. NOURA Issue Date 013-09-1 Doc URL http://hdl.handle.net/115/538

More information

Course Outline. ECE 178: Image Processing REVIEW. Relationship between pixels. Connected components. Distance Measures. Linear systems-review

Course Outline. ECE 178: Image Processing REVIEW. Relationship between pixels. Connected components. Distance Measures. Linear systems-review ECE 78: Image Pocessing REVIEW Lectue #2 Mach 3, 23 Couse Outline! Intoduction! Digital Images! Image Tansfoms! Sampling and Quantization! Image Enhancement! Image/Video Coding JPEG MPEG Mach 3, 23 Mach

More information

Goodness-of-fit for composite hypotheses.

Goodness-of-fit for composite hypotheses. Section 11 Goodness-of-fit fo composite hypotheses. Example. Let us conside a Matlab example. Let us geneate 50 obsevations fom N(1, 2): X=nomnd(1,2,50,1); Then, unning a chi-squaed goodness-of-fit test

More information