Meta-Learning and Universality

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Meta-Learning and Universality"

Transcript

1 Meta-Learning and Universality Conference paper at ICLR 2018 Chelsea Finn & Sergey Levine (US Berkeley) Youngseok Yoon

2 Contents The Universality in Meta-Learning Model Construct (Pre-update) Single gradient step and Post-update Show universality from model Experiments Conclusion

3 The Universality in Meta-Learning What is the universality in Meta-Learning? Universality in Neural Network: Approximate any function ff: xx yy Universality in Meta-Learning: Approximate any function ff: xx, yy kk, xx yy Input: The training data xx, yy kk, and Test data xx. In this presentation, only show about kk = 1 case. Our model to verify Universality: MAML: ff ; θθ ff( ; θθ ), θθ = θθ αα θθ L tttttttttttt, ff ; θθ Update model ff( ; θθ) using gradient update

4 Model Construct (Pre-update) Our model: Deep neural network with ReLU, MAML training.

5 Model Construct (Pre-update) Construct model ff ; θθ with ReLU If we assume inputs and all pre-synaptic activations are nonnegative, then deep ReLU act like deep linear networks. (1) ff ; θθ = ff oooooo NN ii=1 WW ii φφ ; θθ ffff, θθ bb ; θθ oooooo

6 Single gradient step and Post-update WWii L = aa ii bb ii 1 aa ii : the error gradient with respect to the pre-synaptic activations at layer ii bb ii 1 : the forward post-synaptic activations at layer ii 1 ffffffffffffff WW ii+1 bb ii 1 WW ii aa ii WW ii 1

7 Single gradient step and Post-update let zz = Then, NN ii=1 WW ii φφ xx; θθ ffff, θθ bb, zz L = ee(xx, yy) WWii L = aa ii bb ii 1 = WW ii 1 WW NN 1 ee xx, yy jj=ii+1 WW jj φφ xx; θθ ffff, θθ bb = ii 1 jj=1 WW jj ee xx, yy φφ xx; NN θθffff, θθ bb jj=ii+1 WW jj ffffffffffffff WW ii+1 bb ii 1 WW ii aa ii WW ii 1

8 Single gradient step and Post-update let zz = Then, NN ii=1 WW ii φφ xx; θθ ffff, θθ bb, zz L = ee(xx, yy) WWii L = aa ii bb ii 1 = WW ii 1 WW NN 1 ee xx, yy jj=ii+1 WW jj φφ xx; θθ ffff, θθ bb = ii 1 jj=1 WW jj ee xx, yy φφ xx; NN θθffff, θθ bb jj=ii+1 WW jj Therefore, post-update value of NN ii=1 NN ii=1 NN WW ii αασ ii=1 ii 1 jj=1 WW jj WW NN ii = ii=1 ii 1 WW jj ee xx, yy φφ xx; θθffff, θθ bb jj=ii+1 NN jj=1 WW ii αα WWii L WW ii 1 jj jj=1 WW jj OO αα 2

9 Single gradient step and Post-update Post-update value of NN ii=1 NN ii=1 NN WW ii αασ ii=1 ii 1 jj=1 WW jj jj=1 WW NN ii = ii=1 WW ii αα WWii L ii 1 WW jj ee xx, yy φφ xx; θθffff, θθ bb jj=ii+1 NN WW ii 1 jj jj=1 WW jj OO αα 2 Now, post-update value of zz when xx input into ff ; θθ NN zz = ii=1 WW ii φφ xx ; θθ ffff, θθ bb = NN ii=1 WW ii φφ xx ; θθ ffff, θθ bb NN ii 1 WW jj ee xx, yy φφ xx; NN θθffff, θθ bb jj=ii+1 αασ ii=1 ii 1 jj=1 WW jj And, ff xx ; θθ jj=1 = ff oooooo zz ; θθ oooooo WW ii 1 jj jj=1 WW jj φφ xx ; θθ ffff, θθ bb

10 Show universality from model How to show universality from post-updated model?

11 Show universality from model Use independently control information flow from xx, from yy, from xx by multiplexing forward information from xx and backward information from yy Decomposing WW ii, φφ and error gradient into three parts, WW ii WW ii WW ii 0, φφ ; θθ ffff, θθ bb 0 0 ww ii φφ ; θθ ffff, θθ bb 00, zz L yy, ff xx; θθ θθ bb 00 ee yy ee yy 2

12 Show universality from model xx θθ ffff, θθ bb WW NN WW ii WW 1 zz ff oooooo yy xx θθ ffff, θθ bb φφ 00 θθ bb WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz ff oooooo yy

13 Show universality from model Then, before the gradient update, zz = zz zz zz = NN WW ii φφ(xx; θθ ffff, θθ bb ) ii= Hence, represent the middle one of after gradient update, zz zz = NN ii=1 φφ xx; θθ ffff, θθ bb 00 θθ bb WW ii WW ii ww ii NN jj=ii+1 φφ xx; θθ ffff, θθ bb 00 θθ bb WW jj WW jj ww jj NN αασ ii=1 ii 1 jj=1 ii 1 jj=1 WW jj 0 0 ii 1 0 WW jj 0 jj=1 0 0 ww jj WW jj 0 0 φφ xx ; θθ ffff, θθ bb 0 WW jj ww jj θθ bb WW jj WW jj ww jj 00 ee yy ee yy zz NN = αασ ii=1 ii 1 jj=1 WW jj ii 1 jj=1 WW jj ee yy φφ xx; θθ ffff, θθ bb jj=ii+1 NN ii 1 WW jj jj=1 WW jj φφ xx ; θθ ffff, θθ bb

14 Show universality from model yy = ff oooooo zz; θθ oooooo and zz = 0 xx θθ ffff, θθ bb φφ 00 θθ bb WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz ff oooooo yy zz NN = αασ ii=1 ii 1 jj=1 WW jj ii 1 jj=1 WW jj ee yy φφ xx; θθ ffff, θθ bb jj=ii+1 = αασ NN ii=1 AA ii ee yy φφ xx; θθ ffff, θθ bb BBii BB ii φφ xx ; θθ ffff, θθ bb (3) NN ii 1 WW jj jj=1 WW jj φφ xx ; θθ ffff, θθ bb xx θθ ffff, θθ bb φφ 00 θθ bb WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz ff oooooo yy

15 Show universality from model Path 1) Define ff oooooo Path 2) Show zz as new vector vv, which containing informations of xx, yy and xx At last, Universality with Vector vv

16 Show universality from model Define ff oooooo as a neural network that approximates the following multiplexer function and its derivatives ff oooooo zz zz zz zz ; θθ oooooo = 11 zz=0 gg pppppp ; θθ gg + 11 zz 0 h pppppppp zz; θθ h, 4 zz zz Where gg pppppp is a linear function with parameters θθ gg such that zz L = ee yy (2) Where h pppppppp is a neural network with one or more hidden layers. Then, after pose-update, ff oooooo zz zz zz ; θθ oooooo = h pppppppp zz ; θθ h, 5 xx θθ ffff, θθ bb φφ 00 θθ bb WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz gg pppppp h pppppppp yy

17 Show universality from model Change the form of zz with kernel form zz = αασ NN ii=1 AA ii ee yy φφ xx; θθ ffff, θθ bb BBii BB ii φφ xx ; θθ ffff, θθ bb = NN αασii=1 AA ii ee yy kk ii xx, xx zz = αασ NN ii=1 AA ii ee yy kk ii xx, xx has the all information of xx, yy and xx. Assume ee yy is a linear function of yy which can extract the original information yy. xx θθ ffff, θθ bb φφ 00 θθ bb WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz gg pppppp h pppppppp yy

18 Show universality from model Change the form of zz with kernel form zz = αασ NN ii=1 AA ii ee yy φφ xx; θθ ffff, θθ bb BBii BB ii φφ xx ; θθ ffff, θθ bb = NN αασii=1 AA ii ee yy kk ii xx, xx zz = αασ NN ii=1 AA ii ee yy kk ii xx, xx has the all information of xx, yy and xx. Assume ee yy is a linear function of yy which can extract the original information yy. Idea 1) Decompose index ii = 1,, NN to a product of jj = 0,, JJ 1 aaaaaa ll = 0,, LL 1, and then assign those to xx aaaaaa xx Idea 2) Discretize xx and xx to jj and ll by kernel kk(, ) Idea 3) Make new vector vv, which contain all information of xx, xx aaaaaa yy from AA ii, ee yy aaaaaa kk ii

19 Show universality from model Idea 1) Decompose index ii = 1,, NN to a product of jj = 0,, JJ 1 aaaaaa ll = 0,, LL 1, and then assign those to xx aaaaaa xx zz = αασ NN ii=1 AA ii ee yy kk ii xx, xx = αασ JJ 1 jj=0 Σ ll=0 LL 1 AA jjjj Idea 2) Discretize xx and xx to jj and ll by kernel kk(, ) kk jjjj xx, xx = 1 0 iiii dddddddddd xx = ee jj aaaaaa dddddddddd xx ooooooooooooooooo ee yy kk jjjj xx, xx = ee ll (6) xx θθ ffff, θθ bb φφ 00 θθ bb WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz gg pppppp h pppppppp yy

20 Show universality from model Idea 3) Make new vector vv, which contain all information of xx, xx aaaaaa yy from AA ii, ee yy aaaaaa kk ii Choose ee yy to be a linear function that outputs J LL stacked copies of yy εε εε Define AA jjjj to be a select yy at the position of (jj, ll) = jj + JJ LL, AA jjjj = 1 + εε, 1 + εε at position (jj, ll) εε εε As a result, zz = αασ NN ii=1 AA ii ee yy kk ii xx, xx 0 0 = vv xx, xx, yy yy 0 0 xx = αασ JJ 1 jj=0 Σ ll=0 θθ ffff, θθ bb LL 1 AA jjjj φφ 00 θθ bb ee yy kk jjjj xx, xx WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz gg pppppp h pppppppp yy

21 Show universality from model As a result, zz = αασ NN ii=1 AA ii ee yy kk ii xx, xx ff xx ; θθ = αασ JJ 1 jj=0 Σ ll=0 h pppppppp αααα xx, xx, yy ; θθ h LL 1 AA jjjj ee yy kk jjjj xx, xx = αααα xx, xx, yy, where vv xx, xx, yy It is a universal function approximator with respect to its inputs xx, xx, yy 0 0 yy 0 0 xx θθ ffff, θθ bb φφ 00 θθ bb WW NN WW NN ww NN WW ii WW ii ww ii WW 1 WW 1 ww 1 zz zz zz gg pppppp h pppppppp yy

22 Experiments Q1) Is there empirical benefit to using one meta-learning approach versus another, and in which case? A1) Empirically show the inductive bias of gradient-based vs recurrent meta-learners Explore the differences between gradient-based vs recurrent A learner trained with MAML, improve or start to overfit after additional gradient steps. Better few-shot learning performance on tasks outside of the training distribution?

23 Experiments

24 Experiments

25 Experiments Q2) Theory suggest that deeper networks lead to increased expressive power for representing different learning procedures. Is it right? A1) Investigate the role of model depth in gradient-based metalearning

26 Experiments

27 Conclusion Meta-learners that use standard gradient descent with a sufficiently deep representation can approximate any learning procedure, and are equally expressive as recurrent learners. In experiments, MAML is more successful when faced with out-of-domain tasks compared to recurrent model We formalize what it means for a meta-learner to be able to approximate any learning algorithm in terms of its ability to represent functions of the dataset and test inputs.

28 Appendix A B C we assume inputs and all pre-synaptic activations are non-negative, then deep ReLU act like deep linear networks. (1) zz NN = αασ ii=1 ii 1 jj=1 WW jj ii 1 jj=1 WW jj ee yy φφ xx; θθ ffff, θθ bb jj=ii+1 = αασ NN ii=1 AA ii ee yy φφ xx; θθ ffff, θθ bb BBii BB ii φφ xx ; θθ ffff, θθ bb (3) zz L yy, ff xx; θθ ff oooooo zz zz zz kk jjjj xx, xx = ee yy ee yy 2 ; θθ oooooo = 11 zz=0 gg pppppp zz zz zz iiii dddddddddd xx = ee jj aaaaaa dddddddddd xx NN ii 1 WW jj jj=1 WW jj h zz; θθ, 4, ff ; θθ gg + 11 zz 0 zz zz pppppppp h oooooo zz ooooooooooooooooo = ee ll (6) φφ xx ; θθ ffff, θθ bb ; θθ oooooo = h pppppppp zz ; θθ h, 5

29 Appendix A zz NN = αασ ii=1 ii 1 jj=1 WW jj ii 1 jj=1 WW jj ee yy φφ xx; θθ ffff, θθ bb = αασ NN ii=1 AA ii ee yy φφ xx; θθ ffff, θθ bb BBii BB ii φφ xx ; θθ ffff, θθ bb Choose all WW ii and WW ii to be a square and full rank. Set WW ii = MM ii MM 1 ii+1 MM 0 = II) Set AA 1 = II, AA ii = MM ii 1 MM ii 1 1 NN and WW ii = MM ii 1 MM ii then jj=ii+1 and BB ii = MM ii+1, BB NN = II NN jj=ii+1 WW jj ii 1 jj=1 WW jj φφ xx ; θθ ffff, θθ bb ii 1 WW jj = MM ii+1, jj=1 WW jj = MM ii 1 ( MM NN+1 = II,

30 Appendix A All inputs are non-negative: Input φφ consist of three term, (discretization, constant 0, 0 before update and not used afterward) All inputs are non-negative before and after update. All pre-synaptic activations are non-negative: It is sufficient to show that products of WW ii, ii=jj WW ii (1 jj NN) are positive semi-definite. So, show that NN ii=jj WW ii, NN ii=jj WW ii, NN ii=jj ww ii (1 jj NN) are positive semi-definite. We define NN ii=jj WW ii = MM jj+1 = BB ii, and BB ii is set to be a positive definite. 1 We define WW ii = MM ii 1 MM ii where AA ii = MM ii 1 MM ii 1, so each MM ii is also symmetric positive definite and WW ii is positive definite. Purpose of ww ii is to provide nonzero gradient to the input θθ bb, thus positive value for each ww ii will suffice. NN

31 Appendix B zz L yy, ff xx; θθ 00 ee yy ee yy 2 zz L yy, ff xx; θθ = zz ff xx; θθ yy L yy, yy = ff xx; θθ = ff oooooo zz; θθ oooooo = gg pppppp zz; θθ gg Because we assume gg pppppp as a linear function of θθ gg, let gg pppppp zz; θθ gg = WW gg WW gg ww gg zz = WW gg zz + WW gg zz gg + ww gg zz To make top element of ee(xx, yy) to be 00, let WW gg = 0, which make yy = 0. Then, ee yy = WW gg yy L yy, 0 For any linear loss function for yy, ee yy = AAAA, to extract all information of yy, AA has to be invertible. Sufficient loss function: standard mean-squared error or softmax cross entropy. 00 ee yy ee yy

32 Appendix C kk jjjj xx, xx Choose φφ and BB jjjj : = φφ xx; θθ ffff, θθ bb BBjjjj BB jjjj φφ xx ; θθ 1 ffff, θθ bb = 0 φφ ; θθ ffff, θθ bb ddiiiiiiii 0 0 ddiiiiiiii iiff θθ bb = 0 ooooooooooooooooo iiii dddddddddd xx = ee jj aaaaaa dddddddddd xx ooooooooooooooooo BB jjjj = EE jjjj EE jjjj EE llll 0 + εεεε = ee ll Then, where EE iiii denote the matrix a 1 at ii, kk φφ xx; θθ ffff, θθ bb BBjjjj ee jj iiff dddddddddd xx = ee jj ooooooooooooooooo and 0 otherwise BB jjjj φφ xx ; θθ ee ffff, θθ bb ll 0 iiff dddddddddd xx = ee ll 0 0 ooooooooooooooooo

33 Appendix C kk jjjj xx, xx = φφ xx; θθ ffff, θθ bb BBjjjj BB jjjj φφ xx ; θθ 1 ffff, θθ bb = 0 φφ ; θθ ffff, θθ bb φφ xx; θθ ffff, θθ bb BBjjjj ee jj So, ddiiiiiiii 0 0 ddiiiiiiii kk jjjj xx, xx ee jj 0 ee ll 0 0 iiff θθ bb = 0 ooooooooooooooooo iiff dddddddddd xx = ee jj ooooooooooooooooo iiii dddddddddd xx = ee jj aaaaaa dddddddddd xx ooooooooooooooooo BB jjjj = EE jjjj EE jjjj EE llll 0 + εεεε = ee ll BB jjjj φφ xx ; θθ ee ffff, θθ bb ll 0 iiff dddddddddd xx = ee ll 0 0 ooooooooooooooooo iiff dddddddddd xx = ee jj aaaaaa dddddddddd xx ooooooooooooooooo = ee ll

34 Thank you!

2 Composition. Invertible Mappings

2 Composition. Invertible Mappings Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,

Διαβάστε περισσότερα

C.S. 430 Assignment 6, Sample Solutions

C.S. 430 Assignment 6, Sample Solutions C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order

Διαβάστε περισσότερα

derivation of the Laplacian from rectangular to spherical coordinates

derivation of the Laplacian from rectangular to spherical coordinates derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used

Διαβάστε περισσότερα

Other Test Constructions: Likelihood Ratio & Bayes Tests

Other Test Constructions: Likelihood Ratio & Bayes Tests Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :

Διαβάστε περισσότερα

ST5224: Advanced Statistical Theory II

ST5224: Advanced Statistical Theory II ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known

Διαβάστε περισσότερα

EE512: Error Control Coding

EE512: Error Control Coding EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3

Διαβάστε περισσότερα

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3

Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all

Διαβάστε περισσότερα

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

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β 3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle

Διαβάστε περισσότερα

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)

Διαβάστε περισσότερα

Matrices and Determinants

Matrices and Determinants Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z

Διαβάστε περισσότερα

Fractional Colorings and Zykov Products of graphs

Fractional Colorings and Zykov Products of graphs Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is

Διαβάστε περισσότερα

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

Partial Differential Equations in Biology The boundary element method. March 26, 2013 The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet

Διαβάστε περισσότερα

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

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Αν κάπου κάνετε κάποιες υποθέσεις να αναφερθούν στη σχετική ερώτηση. Όλα τα αρχεία που αναφέρονται στα προβλήματα βρίσκονται στον ίδιο φάκελο με το εκτελέσιμο

Διαβάστε περισσότερα

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

w o = R 1 p. (1) R = p =. = 1 Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:

Διαβάστε περισσότερα

6.3 Forecasting ARMA processes

6.3 Forecasting ARMA processes 122 CHAPTER 6. ARMA MODELS 6.3 Forecasting ARMA processes The purpose of forecasting is to predict future values of a TS based on the data collected to the present. In this section we will discuss a linear

Διαβάστε περισσότερα

Problem Set 3: Solutions

Problem Set 3: Solutions CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C

Διαβάστε περισσότερα

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

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch: HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying

Διαβάστε περισσότερα

Finite Field Problems: Solutions

Finite Field Problems: Solutions Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The

Διαβάστε περισσότερα

Section 8.3 Trigonometric Equations

Section 8.3 Trigonometric Equations 99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.

Διαβάστε περισσότερα

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =

Διαβάστε περισσότερα

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

Solution Series 9. i=1 x i and i=1 x i. Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x

Διαβάστε περισσότερα

Homework 8 Model Solution Section

Homework 8 Model Solution Section MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx

Διαβάστε περισσότερα

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

Approximation of distance between locations on earth given by latitude and longitude Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth

Διαβάστε περισσότερα

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

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required) Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts

Διαβάστε περισσότερα

Lecture 2. Soundness and completeness of propositional logic

Lecture 2. Soundness and completeness of propositional logic Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness

Διαβάστε περισσότερα

Section 7.6 Double and Half Angle Formulas

Section 7.6 Double and Half Angle Formulas 09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)

Διαβάστε περισσότερα

Congruence Classes of Invertible Matrices of Order 3 over F 2

Congruence Classes of Invertible Matrices of Order 3 over F 2 International Journal of Algebra, Vol. 8, 24, no. 5, 239-246 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ija.24.422 Congruence Classes of Invertible Matrices of Order 3 over F 2 Ligong An and

Διαβάστε περισσότερα

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in

Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that

Διαβάστε περισσότερα

Takeaki Yamazaki (Toyo Univ.) 山崎丈明 ( 東洋大学 ) Oct. 24, RIMS

Takeaki Yamazaki (Toyo Univ.) 山崎丈明 ( 東洋大学 ) Oct. 24, RIMS Takeaki Yamazaki (Toyo Univ.) 山崎丈明 ( 東洋大学 ) Oct. 24, 2017 @ RIMS Contents Introduction Generalized Karcher equation Ando-Hiai inequalities Problem Introduction PP: The set of all positive definite operators

Διαβάστε περισσότερα

Math221: HW# 1 solutions

Math221: HW# 1 solutions Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin

Διαβάστε περισσότερα

Statistical Inference I Locally most powerful tests

Statistical Inference I Locally most powerful tests Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided

Διαβάστε περισσότερα

Example Sheet 3 Solutions

Example Sheet 3 Solutions Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note

Διαβάστε περισσότερα

The Simply Typed Lambda Calculus

The Simply Typed Lambda Calculus Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and

Διαβάστε περισσότερα

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

Bayesian statistics. DS GA 1002 Probability and Statistics for Data Science. Bayesian statistics DS GA 1002 Probability and Statistics for Data Science http://www.cims.nyu.edu/~cfgranda/pages/dsga1002_fall17 Carlos Fernandez-Granda Frequentist vs Bayesian statistics In frequentist

Διαβάστε περισσότερα

Numerical Analysis FMN011

Numerical Analysis FMN011 Numerical Analysis FMN011 Carmen Arévalo Lund University carmen@maths.lth.se Lecture 12 Periodic data A function g has period P if g(x + P ) = g(x) Model: Trigonometric polynomial of order M T M (x) =

Διαβάστε περισσότερα

4.6 Autoregressive Moving Average Model ARMA(1,1)

4.6 Autoregressive Moving Average Model ARMA(1,1) 84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this

Διαβάστε περισσότερα

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013

Jesse Maassen and Mark Lundstrom Purdue University November 25, 2013 Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering

Διαβάστε περισσότερα

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

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ. Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action

Διαβάστε περισσότερα

Tridiagonal matrices. Gérard MEURANT. October, 2008

Tridiagonal matrices. Gérard MEURANT. October, 2008 Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,

Διαβάστε περισσότερα

Srednicki Chapter 55

Srednicki Chapter 55 Srednicki Chapter 55 QFT Problems & Solutions A. George August 3, 03 Srednicki 55.. Use equations 55.3-55.0 and A i, A j ] = Π i, Π j ] = 0 (at equal times) to verify equations 55.-55.3. This is our third

Διαβάστε περισσότερα

Solutions to Exercise Sheet 5

Solutions to Exercise Sheet 5 Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X

Διαβάστε περισσότερα

Instruction Execution Times

Instruction Execution Times 1 C Execution Times InThisAppendix... Introduction DL330 Execution Times DL330P Execution Times DL340 Execution Times C-2 Execution Times Introduction Data Registers This appendix contains several tables

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

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

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1. Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given

Διαβάστε περισσότερα

What happens when two or more waves overlap in a certain region of space at the same time?

What happens when two or more waves overlap in a certain region of space at the same time? Wave Superposition What happens when two or more waves overlap in a certain region of space at the same time? To find the resulting wave according to the principle of superposition we should sum the fields

Διαβάστε περισσότερα

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο

Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων. Εξάμηνο 7 ο Εργαστήριο Ανάπτυξης Εφαρμογών Βάσεων Δεδομένων Εξάμηνο 7 ο Procedures and Functions Stored procedures and functions are named blocks of code that enable you to group and organize a series of SQL and PL/SQL

Διαβάστε περισσότερα

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006 Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα είναι μικρότεροι το 1000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Διάρκεια: 3,5 ώρες Καλή

Διαβάστε περισσότερα

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

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8  questions or comments to Dan Fetter 1 Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test

Διαβάστε περισσότερα

ΠΤΥΧΙΑΚΗ ΕΡΓΑΣΙΑ ΒΑΛΕΝΤΙΝΑ ΠΑΠΑΔΟΠΟΥΛΟΥ Α.Μ.: 09/061. Υπεύθυνος Καθηγητής: Σάββας Μακρίδης

ΠΤΥΧΙΑΚΗ ΕΡΓΑΣΙΑ ΒΑΛΕΝΤΙΝΑ ΠΑΠΑΔΟΠΟΥΛΟΥ Α.Μ.: 09/061. Υπεύθυνος Καθηγητής: Σάββας Μακρίδης Α.Τ.Ε.Ι. ΙΟΝΙΩΝ ΝΗΣΩΝ ΠΑΡΑΡΤΗΜΑ ΑΡΓΟΣΤΟΛΙΟΥ ΤΜΗΜΑ ΔΗΜΟΣΙΩΝ ΣΧΕΣΕΩΝ ΚΑΙ ΕΠΙΚΟΙΝΩΝΙΑΣ ΠΤΥΧΙΑΚΗ ΕΡΓΑΣΙΑ «Η διαμόρφωση επικοινωνιακής στρατηγικής (και των τακτικών ενεργειών) για την ενδυνάμωση της εταιρικής

Διαβάστε περισσότερα

Overview. Transition Semantics. Configurations and the transition relation. Executions and computation

Overview. Transition Semantics. Configurations and the transition relation. Executions and computation Overview Transition Semantics Configurations and the transition relation Executions and computation Inference rules for small-step structural operational semantics for the simple imperative language Transition

Διαβάστε περισσότερα

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

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R + Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b

Διαβάστε περισσότερα

6.1. Dirac Equation. Hamiltonian. Dirac Eq.

6.1. Dirac Equation. Hamiltonian. Dirac Eq. 6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2

Διαβάστε περισσότερα

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal

Διαβάστε περισσότερα

EE101: Resonance in RLC circuits

EE101: Resonance in RLC circuits EE11: Resonance in RLC circuits M. B. Patil mbatil@ee.iitb.ac.in www.ee.iitb.ac.in/~sequel Deartment of Electrical Engineering Indian Institute of Technology Bombay I V R V L V C I = I m = R + jωl + 1/jωC

Διαβάστε περισσότερα

Homework 3 Solutions

Homework 3 Solutions Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For

Διαβάστε περισσότερα

Math 6 SL Probability Distributions Practice Test Mark Scheme

Math 6 SL Probability Distributions Practice Test Mark Scheme Math 6 SL Probability Distributions Practice Test Mark Scheme. (a) Note: Award A for vertical line to right of mean, A for shading to right of their vertical line. AA N (b) evidence of recognizing symmetry

Διαβάστε περισσότερα

Space-Time Symmetries

Space-Time Symmetries Chapter Space-Time Symmetries In classical fiel theory any continuous symmetry of the action generates a conserve current by Noether's proceure. If the Lagrangian is not invariant but only shifts by a

Διαβάστε περισσότερα

[1] P Q. Fig. 3.1

[1] P Q. Fig. 3.1 1 (a) Define resistance....... [1] (b) The smallest conductor within a computer processing chip can be represented as a rectangular block that is one atom high, four atoms wide and twenty atoms long. One

Διαβάστε περισσότερα

Reminders: linear functions

Reminders: linear functions Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U

Διαβάστε περισσότερα

Example of the Baum-Welch Algorithm

Example of the Baum-Welch Algorithm Example of the Baum-Welch Algorithm Larry Moss Q520, Spring 2008 1 Our corpus c We start with a very simple corpus. We take the set Y of unanalyzed words to be {ABBA, BAB}, and c to be given by c(abba)

Διαβάστε περισσότερα

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

Chapter 6: Systems of Linear Differential. be continuous functions on the interval Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations

Διαβάστε περισσότερα

( ) 2 and compare to M.

( ) 2 and compare to M. Problems and Solutions for Section 4.2 4.9 through 4.33) 4.9 Calculate the square root of the matrix 3!0 M!0 8 Hint: Let M / 2 a!b ; calculate M / 2!b c ) 2 and compare to M. Solution: Given: 3!0 M!0 8

Διαβάστε περισσότερα

Concrete Mathematics Exercises from 30 September 2016

Concrete Mathematics Exercises from 30 September 2016 Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)

Διαβάστε περισσότερα

Access Control Encryption Enforcing Information Flow with Cryptography

Access Control Encryption Enforcing Information Flow with Cryptography Access Control Encryption Enforcing Information Flow with Cryptography Ivan Damgård, Helene Haagh, and Claudio Orlandi http://eprint.iacr.org/2016/106 Outline Access Control Encryption Motivation Definition

Διαβάστε περισσότερα

These derivations are not part of the official forthcoming version of Vasilaky and Leonard

These derivations are not part of the official forthcoming version of Vasilaky and Leonard Target Input Model with Learning, Derivations Kathryn N Vasilaky These derivations are not part of the official forthcoming version of Vasilaky and Leonard 06 in Economic Development and Cultural Change.

Διαβάστε περισσότερα

Areas and Lengths in Polar Coordinates

Areas and Lengths in Polar Coordinates Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the

Διαβάστε περισσότερα

1. For each of the following power series, find the interval of convergence and the radius of convergence:

1. For each of the following power series, find the interval of convergence and the radius of convergence: Math 6 Practice Problems Solutios Power Series ad Taylor Series 1. For each of the followig power series, fid the iterval of covergece ad the radius of covergece: (a ( 1 x Notice that = ( 1 +1 ( x +1.

Διαβάστε περισσότερα

Section 9.2 Polar Equations and Graphs

Section 9.2 Polar Equations and Graphs 180 Section 9. Polar Equations and Graphs In this section, we will be graphing polar equations on a polar grid. In the first few examples, we will write the polar equation in rectangular form to help identify

Διαβάστε περισσότερα

Exercises to Statistics of Material Fatigue No. 5

Exercises to Statistics of Material Fatigue No. 5 Prof. Dr. Christine Müller Dipl.-Math. Christoph Kustosz Eercises to Statistics of Material Fatigue No. 5 E. 9 (5 a Show, that a Fisher information matri for a two dimensional parameter θ (θ,θ 2 R 2, can

Διαβάστε περισσότερα

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

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1 Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the

Διαβάστε περισσότερα

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD CHAPTER FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD EXERCISE 36 Page 66. Determine the Fourier series for the periodic function: f(x), when x +, when x which is periodic outside this rge of period.

Διαβάστε περισσότερα

New bounds for spherical two-distance sets and equiangular lines

New bounds for spherical two-distance sets and equiangular lines New bounds for spherical two-distance sets and equiangular lines Michigan State University Oct 8-31, 016 Anhui University Definition If X = {x 1, x,, x N } S n 1 (unit sphere in R n ) and x i, x j = a

Διαβάστε περισσότερα

The challenges of non-stable predicates

The challenges of non-stable predicates The challenges of non-stable predicates Consider a non-stable predicate Φ encoding, say, a safety property. We want to determine whether Φ holds for our program. The challenges of non-stable predicates

Διαβάστε περισσότερα

Second Order Partial Differential Equations

Second Order Partial Differential Equations Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y

Διαβάστε περισσότερα

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

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is Pg. 9. The perimeter is P = The area of a triangle is A = bh where b is the base, h is the height 0 h= btan 60 = b = b In our case b =, then the area is A = = 0. By Pythagorean theorem a + a = d a a =

Διαβάστε περισσότερα

Mean bond enthalpy Standard enthalpy of formation Bond N H N N N N H O O O

Mean bond enthalpy Standard enthalpy of formation Bond N H N N N N H O O O Q1. (a) Explain the meaning of the terms mean bond enthalpy and standard enthalpy of formation. Mean bond enthalpy... Standard enthalpy of formation... (5) (b) Some mean bond enthalpies are given below.

Διαβάστε περισσότερα

EE434 ASIC & Digital Systems Arithmetic Circuits

EE434 ASIC & Digital Systems Arithmetic Circuits EE434 ASIC & Digital Systems Arithmetic Circuits Spring 25 Dae Hyun Kim daehyun@eecs.wsu.edu Arithmetic Circuits What we will learn Adders Basic High-speed 2 Adder -bit adder SSSSSS = AA BB CCCC CCCC =

Διαβάστε περισσότερα

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

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)

Διαβάστε περισσότερα

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

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =? Teko Classes IITJEE/AIEEE Maths by SUHAAG SIR, Bhopal, Ph (0755) 3 00 000 www.tekoclasses.com ANSWERSHEET (TOPIC DIFFERENTIAL CALCULUS) COLLECTION # Question Type A.Single Correct Type Q. (A) Sol least

Διαβάστε περισσότερα

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

MATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3) 1. MATH43 String Theory Solutions 4 x = 0 τ = fs). 1) = = f s) ) x = x [f s)] + f s) 3) equation of motion is x = 0 if an only if f s) = 0 i.e. fs) = As + B with A, B constants. i.e. allowe reparametrisations

Διαβάστε περισσότερα

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

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We

Διαβάστε περισσότερα

Electronic Analysis of CMOS Logic Gates

Electronic Analysis of CMOS Logic Gates Electronic Analysis of CMOS Logic Gates Dae Hyun Kim EECS Washington State University References John P. Uyemura, Introduction to VLSI Circuits and Systems, 2002. Chapter 7 Goal Understand how to perform

Διαβάστε περισσότερα

Computing Gradient. Hung-yi Lee 李宏毅

Computing Gradient. Hung-yi Lee 李宏毅 Computing Gradient Hung-yi Lee 李宏毅 Introduction Backpropagation: an efficient way to compute the gradient Prerequisite Backpropagation for feedforward net: http://speech.ee.ntu.edu.tw/~tkagk/courses/mlds_05_/lecture/

Διαβάστε περισσότερα

PARTIAL NOTES for 6.1 Trigonometric Identities

PARTIAL NOTES for 6.1 Trigonometric Identities PARTIAL NOTES for 6.1 Trigonometric Identities tanθ = sinθ cosθ cotθ = cosθ sinθ BASIC IDENTITIES cscθ = 1 sinθ secθ = 1 cosθ cotθ = 1 tanθ PYTHAGOREAN IDENTITIES sin θ + cos θ =1 tan θ +1= sec θ 1 + cot

Διαβάστε περισσότερα

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------

Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- ----------------- Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin

Διαβάστε περισσότερα

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

If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2 Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the

Διαβάστε περισσότερα

Living and Nonliving Created by: Maria Okraska

Living and Nonliving Created by: Maria Okraska Living and Nonliving Created by: Maria Okraska http://enchantingclassroom.blogspot.com Living Living things grow, change, and reproduce. They need air, water, food, and a place to live in order to survive.

Διαβάστε περισσότερα

Assalamu `alaikum wr. wb.

Assalamu `alaikum wr. wb. LUMP SUM Assalamu `alaikum wr. wb. LUMP SUM Wassalamu alaikum wr. wb. Assalamu `alaikum wr. wb. LUMP SUM Wassalamu alaikum wr. wb. LUMP SUM Lump sum lump sum lump sum. lump sum fixed price lump sum lump

Διαβάστε περισσότερα

Lecture 10 - Representation Theory III: Theory of Weights

Lecture 10 - Representation Theory III: Theory of Weights Lecture 10 - Representation Theory III: Theory of Weights February 18, 2012 1 Terminology One assumes a base = {α i } i has been chosen. Then a weight Λ with non-negative integral Dynkin coefficients Λ

Διαβάστε περισσότερα

TMA4115 Matematikk 3

TMA4115 Matematikk 3 TMA4115 Matematikk 3 Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet Trondheim Spring 2010 Lecture 12: Mathematics Marvellous Matrices Andrew Stacey Norges Teknisk-Naturvitenskapelige Universitet

Διαβάστε περισσότερα

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

If we restrict the domain of y = sin x to [ π 2, π 2 Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the

Διαβάστε περισσότερα

Lecture 13 - Root Space Decomposition II

Lecture 13 - Root Space Decomposition II Lecture 13 - Root Space Decomposition II October 18, 2012 1 Review First let us recall the situation. Let g be a simple algebra, with maximal toral subalgebra h (which we are calling a CSA, or Cartan Subalgebra).

Διαβάστε περισσότερα

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits. EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.

Διαβάστε περισσότερα

D Alembert s Solution to the Wave Equation

D Alembert s Solution to the Wave Equation D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique

Διαβάστε περισσότερα

Συστήματα Διαχείρισης Βάσεων Δεδομένων

Συστήματα Διαχείρισης Βάσεων Δεδομένων ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Συστήματα Διαχείρισης Βάσεων Δεδομένων Φροντιστήριο 9: Transactions - part 1 Δημήτρης Πλεξουσάκης Τμήμα Επιστήμης Υπολογιστών Tutorial on Undo, Redo and Undo/Redo

Διαβάστε περισσότερα

Μηχανική Μάθηση Hypothesis Testing

Μηχανική Μάθηση Hypothesis Testing ΕΛΛΗΝΙΚΗ ΔΗΜΟΚΡΑΤΙΑ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΡΗΤΗΣ Μηχανική Μάθηση Hypothesis Testing Γιώργος Μπορμπουδάκης Τμήμα Επιστήμης Υπολογιστών Procedure 1. Form the null (H 0 ) and alternative (H 1 ) hypothesis 2. Consider

Διαβάστε περισσότερα

Capacitors - Capacitance, Charge and Potential Difference

Capacitors - Capacitance, Charge and Potential Difference Capacitors - Capacitance, Charge and Potential Difference Capacitors store electric charge. This ability to store electric charge is known as capacitance. A simple capacitor consists of 2 parallel metal

Διαβάστε περισσότερα

Εγκατάσταση λογισμικού και αναβάθμιση συσκευής Device software installation and software upgrade

Εγκατάσταση λογισμικού και αναβάθμιση συσκευής Device software installation and software upgrade Για να ελέγξετε το λογισμικό που έχει τώρα η συσκευή κάντε κλικ Menu > Options > Device > About Device Versions. Στο πιο κάτω παράδειγμα η συσκευή έχει έκδοση λογισμικού 6.0.0.546 με πλατφόρμα 6.6.0.207.

Διαβάστε περισσότερα

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

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds! MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.

Διαβάστε περισσότερα