T-duality and noncommutativity in type IIB superstring theory
|
|
- Βηθανία Καραβίας
- 6 χρόνια πριν
- Προβολές:
Transcript
1 T-duality and noncommutativity in type IIB superstring theory B. Nikolić and B. Sazdović Institute of Physics, 111 Belgrade, P.O.Box 57, SERBIA Abstract In this article we investigate noncommutativity of D9-brane worldvolume embedded in space-time of type IIB superstring theory. On the solution of boundary conditions, the initial coordinates become noncommutative. We show that noncommutativity relations are connected by N = 1 supersymmetry transformations and noncommutativity parameters are components of N = 1 supermultiplet. In addition, we show that background fields of the effective theory (initial theory on the solution of boundary conditions) and noncommutativity parameters represent the background fields of the T-dual theory. 1. Introduction Dp-branes with odd value of p are stable in type IIB superstring theory. As a particular choice, besides D9-brane, we can embed D5-brane in ten dimensional space-time of the type IIB theory in pure spinor formulation (up to the quadratic terms)[1, 2]. In the present paper we investigate the noncommutativity of D9-brane using canonical approach. The case of D5-brane has been considered in Ref.[3]. Also we investigate the supersymmetry of noncommutativity relations [4]. We choose Neumann boundary conditions for all bosonic coordinates x µ. The boundary condition for fermionic coordinates, (θ α θ α ) π = produces additional one for their canonically conjugated momenta, (π α π α ) π =. We treat boundary conditions as canonical constraints [5, 6, 7, 3]. Using their consistency conditions, we rewrite them in compact σ-dependent form. We find that they are of the second class and on these solutions, we obtain initial coordinates in terms of effective coordinates and momenta. Presence of the momenta is source of noncommutativity. Noncommutativity relations are consistent with N = 1 supersymmetry transformations. Work supported in part by the Serbian Ministry of Science and Technological Development, under contract No address: bnikolic@ipb.ac.rs, sazdovic@ipb.ac.rs 259
2 26 B. Nikolić, B. Sazdović We obtain that noncommutativity parameters contain only odd powers of background fields antisymmetric under world-sheet parity transformation Ω : σ σ and form one N = 1 supermultiplet. This result represents a supersymmetric generalization of the result obtained by Seiberg and Witten [8]. We also show that effective background fields and noncommutative parameters are the background fields of T-dual theory. 2. Type IIB superstring theory and canonical analysis We will investigate pure spinor formulation [2, 9, 7, 3] of type IIB theory, neglecting ghost terms and keeping quadratic ones S = κ d 2 ξ + x µ Π +µν x ν (1) Σ [ + d 2 ξ π α (θ α + Ψ α µx µ ) + + ( θ α + Ψ α µx µ ) π α + 1 ] 2κ π αf αβ π β, Σ where Π ±µν = B µν ± 1 2 G µν and ± = τ ± σ. All background fields are constant. The space-time coordinates are labeled by x µ (µ =, 1, 2,..., 9) and the fermionic ones by same chirality Majorana-Weyl spinors θ α and θ α. The variables π α and π α are canonically conjugated to the coordinates θ α and θ α, respectively. Canonical Hamiltonian is of the form H c = dσh c, H c = T T +, T ± = t ± τ ±, (2) where t ± = 1 4κ Gµν I ±µ I ±ν, I ±µ = π µ + 2κΠ ±µν x ν + π α Ψ α µ Ψ α µ π α, (3) τ + = (θ α + Ψ α µx µ )π α 1 4κ π αf αβ π β, τ = ( θ α + Ψ α µx µ ) π α + 1 4κ π αf αβ π β. Varying Hamiltonian H c, we obtain δh c = δh (R) c [γ () µ δx µ + π α δθ α + δ θ α π α ] π, (4) where δh c (R) is regular term without τ and σ derivatives of supercoordinates and supermomenta variations and γ () µ = Π +µ ν I ν + Π µ ν I +ν + π α Ψ α µ + Ψ α µ π α. (5) As a time translation generator Hamiltonian has to be differentiable with respect to coordinates and their canonically conjugated momenta which produces [ γ µ () δx µ + π α δθ α + δ θ α π ] π α =. (6)
3 T-duality and noncommutativity in type IIB superstring theory 261 Embedding D9-brane means that we impose Neumann boundary conditions for x µ coordinates, γ µ () π =. Fermionic boundary condition (θα θ α ) π = preserves half of the initial N = 2 supersymmetry and it produces additional boundary condition for fermionic momenta (π α π α ) π =. Using standard Poisson algebra, the consistency procedure for γ () µ produces an infinite set of constraints γ (n) µ {H c, γ (n 1) µ } (n = 1, 2, 3,... ), (7) which can be rewritten at σ = in the compact σ-dependent form Γ µ n= σ n n! γ(n) µ =Π +µ ν I ν (σ) + Π µ ν I +ν ( σ) + π α ( σ)ψ α µ + Ψ α µ π α (σ). Similarly, from conditions (θ α θ α ) = and (π α π α ) =, we get Γ α (σ) = Θ α (σ) Θ α (σ), Γ π α(σ) π α ( σ) π α (σ), (9) (8) where Θ α (σ) = θ α ( σ) Ψ α µ q µ (σ) 1 2κ F αβ + 1 2κ Gµν Ψ α µ dσ 1 P s (I +ν + I ν ), dσ 1 P s π β (1) Θ α (σ) = θ α (σ) + Ψ α µ q µ (σ) + 1 2κ F βα dσ 1 P s π β (11) + 1 2κ Gµν Ψα µ dσ 1 P s (I +ν + I ν ). We introduced new variables, symmetric and antisymmetric under worldsheet parity transformation Ω : σ σ. For bosonic variables we use the standard notation q µ (σ) = P s x µ (σ), q µ (σ) = P a x µ (σ), p µ (σ) = P s π µ (σ), p µ (σ) = P a π µ (σ), while for fermionic ones we use the projectors on σ symmetric and antisymmetric parts P s = 1 2 (1 + Ω), P a = 1 (1 Ω). (12) 2 From {H c, Γ A } = Γ A, Γ A = (Γ µ, Γ α, Γ π α), it follows that there are no more constraints in the theory. For practical reasons we will find the
4 262 B. Nikolić, B. Sazdović algebra of the constraints Γ A = (Γ µ, Γ α, Γ π α) instead of Γ A. It has the form { Γ A, Γ B } = M AB δ, (13) where the supermatrix M AB is given by the expression M AB = κgeff µν 2(Ψ eff ) γ µ 2(Ψ eff ) α 1 ν κ F αγ eff 2δ α δ. (14) 2δ γ β Here we obtain effective background fields G eff µν = G µν 4B µρ G ρλ B λν, (Ψ eff ) α µ = 1 2 Ψα +µ + B µρ G ρν Ψ α ν, F αβ eff = F αβ a Ψ α µg µν Ψ β ν, (15) where we introduced useful notation Ψ α ±µ = Ψ α µ ± Ψ α µ, F αβ s = 1 2 (F αβ + F βα ), F αβ a = 1 2 (F αβ F βα ). (16) This is supersymmetric generalization of Seiberg and Witten open string metric, G eff µν, because all effective fields contain bilinear combinations of Ω odd fields. The superdeterminant s det M AB is proportional to det G eff. Because we assume that effective metric G eff is nonsingular, we conclude that all constraints Γ A are of the second class. 3. Solution of the constraints and noncommutativity From Γ µ =, Γ α = and Γ π α =, we obtain x µ (σ) = q µ 2Θ µν dσ 1 p ν + 2Θ µα dσ 1 p α, π µ = p µ, (17) θ α (σ) = Φ α (σ) ξ α, π α = p α + p α, (18) θ α (σ) = Φ α (σ) 1 2 ξ α, π α = p α p α, (19) where Φ α (σ) = 1 2 ξα Θ µα dσ 1 p µ Θ αβ dσ 1 p β, ξα P a (θ α θ α ),
5 T-duality and noncommutativity in type IIB superstring theory 263 and 1 2 ξα P s θ α = P s θα, p α P s π α = P s π α, p α P a π α = P a π α, Θ µν = 1 κ (G 1 eff BG 1 ) µν, Θ µα = 2Θ µν (Ψ eff ) α ν 1 2κ Gµν ψ α ν, (2) Θ αβ = 1 2κ F s αβ + 4(Ψ eff ) α µθ µν (Ψ eff ) β ν 1 κ Ψα µ(g 1 BG 1 ) µν Ψ β ν + Gµν κ [ ] Ψ α µ(ψ eff ) β ν + Ψ β µ (Ψ eff ) α ν. (21) Using the solutions of the constraints (17)-(19) and the basic Poisson algebra, after removing the center of mass variables, we get the noncommutativity relations {x µ (σ), x ν ( σ)} = Θ µν (σ + σ), (22) {x µ (σ), θ α ( σ)} = 1 2 Θµα (σ + σ), {θ α (σ), θ β ( σ)} = 1 4 Θαβ (σ + σ). The function (σ + σ) is nonzero only at string endpoints 1 if x = (x) = if < x < 2π, 1 if x = 2π (23) (24) and we conclude that interior of the string is commutative, while string endpoints are noncommutative. 4. Supersymmetry of noncommutativity relations The action of initial theory (1) is invariant under global N = 2 supersymmetry with transformations of supercoordinates and background fields δx µ = ɛ α Γ µ αβ θβ + ɛ α Γ µ αβ θ β, δθ α = ɛ α, δ θ α = ɛ α, (25) δg µν = ɛ α +Γ [µ αβ Ψ β +ν] ɛα Γ [µ αβ Ψ β ν], δb µν = ɛ α +Γ [µ αβ Ψ β ν] ɛα Γ [µ αβ Ψ β +ν], δψ α +µ = 1 16 ɛβ Γ µ βγf γα s 1 16 ɛβ + Γ µ βγf γα a, δψ α µ = 1 16 ɛβ + Γ µ βγf γα s ɛβ Γ µ βγf γα a, (26)
6 264 B. Nikolić, B. Sazdović δa () =, δa (2) µν = ɛ α +Γ [µ αβ Ψ β +ν] ɛα Γ [µ αβ Ψ β ν] + A() δb µν, δa (4) µνρσ = 2ɛ α +Γ [µνρ αβ Ψ β σ] + 2ɛα Γ [µνρ αβ Ψ β +σ] + 6A(2) [µν δb ρσ]. Here we used notation ɛ α ± = ɛ α ± ɛ α = const., Γ µ1 µ 2...µ k Γ [µ1 Γ µ2... Γ µk ], (27) and [ ] in the subscripts of the fields mean antisymmetrization of space-time indices between brackets. The connection between potentials A (), A (2) µν and A (4) µνρσ and RR field strength F αβ is given in [7]. The truncation from N = 2 to N = 1 supersymmetry we can realize omitting transformations for G µν, Ψ +µ and F a [1]. The rest fields make N = 1 supermultiplet with transformation rules δb µν = ɛ α +Γ [µ αβ Ψ β ν], δψα µ = 1 16 ɛβ + Γ µ βγf γα s, δf αβ s =. (28) Now we can find the supersymmetric transformations of the coefficients, Θ µν, Θ µα and Θ αβ, multiplying the momenta in the solutions of boundary conditions. From δx µ (σ) = 1 2 ɛα +Γ µ αβ ξβ 2δΘ µν dσ 1 p ν 2Θ µν dσ 1 δp ν, (29) + 2δΘ µα dσ 1 p α + 2Θ µα dσ 1 δp α = ɛ α +Γ µ αβ θ(σ)β 1 2 ɛα +Γ µ ξ(σ) β αβ, δθ α (σ) = 1 2 ɛα + δθ µα dσ 1 p µ Θ µα dσ 1 δp µ δθ αβ dσ 1 p β Θ αβ dσ 1 δp β = 1 2 ɛα +, (3) we obtain global N = 1 SUSY transformations of the background fields δθ µν = ɛ α +Γ [µ αβ Θν]β, δθ µα = 1 2 ɛβ + Γµ βγ Θγα, δθ αβ =. (31) Consequently, these fields are components of N = 1 supermultiplet. Using N = 1 supersymmetry transformations of SUSY coordinates (25) and background fields (31), we can easily prove that noncommutativity relations are connected by supersymmetry transformations. The SUSY transformation of (22) ɛ α +Γ [µ αβ { x ν], θ β} = 1 2 ɛα +Γ [µ αβ Θν]β (σ + σ), (32)
7 T-duality and noncommutativity in type IIB superstring theory 265 produces the first relation in (23). Similarly, SUSY transformation of the first relation in (23) ɛ β + Γµ βγ {θγ, θ α } = 1 4 ɛβ + Γµ βγ Θγα (σ + σ), (33) produces the second relation in (23). 5. Type IIB theory and T-duality We suppose that action (1) has a global shift symmetry in all x µ directions. So, we have to introduce gauge fields v µ ± and make a change ± x µ D ± x µ ± x µ + v µ ±. (34) For the fields v µ ± we introduce additional term in the action S gauge (y, v ± ) = 1 2 κ d 2 ξy µ ( + v µ v µ + ), (35) Σ which produces vanishing of the field strength + v µ v µ + if we vary with respect to the Lagrange multipliers y µ. The full action has the form S (x, y, v ± ) = S(D ± x) + S gauge (y, v ± ). (36) Let us note that on the equations of motion for y µ we have v µ ± = ±x µ and the original dynamics survives unchanged. Now we can fix x µ to zero and obtain the action quadratic in the fields v µ ± which can be integrated out classically. On the equations of motion for v µ ± we obtain expressions for these gauge fields in terms of y µ and momenta ( ) v µ 2 + = 2 κ π αψ α ν + + y ν (G 1 eff Π G 1 ) νµ, (37) ( ) v µ 2 = 2(G 1 eff Π G 1 ) µν κ Ψ α ν π α + y ν. (38) Substituting them in the action S we obtain the dual action from which we read the dual background fields G µν = (G 1 eff )µν, B µν = κθ µν = (G 1 eff BG 1 ) µν, (39) [ [ Ψ µα = 2κΘ µν (G 1 eff )µν] Ψ α ν, Ψµα = 2κΘ µν + (G 1 eff )µν] Ψα ν, F αβ s = 2κΘ αβ, It is easy to see that F αβ a (4) = F αβ eff + 4(Ψ eff ) α µ(g 1 eff )µν (Ψ eff ) α ν. (41) Ψ µα + = 2κΘµα, Ψ µα = 2(G 1 eff )µν (Ψ eff ) α µ. (42)
8 266 B. Nikolić, B. Sazdović 6. Concluding remarks In this paper we considered noncommutativity properties and related supersymmetry transformations of D9 brane in type IIB superstring theory. We used the pure spinor formulation of the theory introduced in Refs.[2, 9]. We treated all boundary conditions at string endpoints as canonical constraints. Solving the second class constraints we obtain the initial coordinates x µ, θ α and θ α in terms of effective ones, q µ, ξ α and ξ α and momenta p µ and p α. The presence of momenta is a source of noncommutativity (22)-(23). The result of the present paper can be considered as a supersymmetric generalization of the result obtained for bosonic string [8]. Beside B µν, its superpartners Ψ α µ and Fs αβ are also a source of noncommutativity. In special case, when Ψ α = Ψ α µ, the noncommutativity relations (22)-(23) correspond to the relations of Ref.[9]. The N = 2 supermultiplet of T-dual theory is split in two N = 1 supermultiplets: the first, Ω even one, (G eff µν, (Ψ eff ) α µ, F αβ eff ), represents the background fields of the effective theory (initial theory on the solution of the boundary conditions) [7], while the second, Ω odd one, (Θ µν, Θ µα, Θ αβ ), contains the noncommutativity parameters. References [1] J. Polchinski, String theory - Volume II, Cambridge University Press, 1998; K. Becker, M. Becker and J. H. Schwarz, String Theory and M-Theory - A Modern Introduction, Cambridge University Press, 27. [2] N. Berkovits and P. Howe, Nucl. Phys. B635 (22) 75; P. A. Grassi, G. Policastro and P. van Nieuwenhuizen, JHEP 11 (22) 4; P. A. Grassi, G. Policastro and P. van Nieuwenhuizen, Adv. Theor. Math. Phys. 7 (23) 499; P. A. Grassi, G. Policastro and P. van Nieuwenhuizen, Phys. Lett. B553 (23) 96. [3] B. Nikolić and B. Sazdović, Nucl. Phys. B 836 (21) [4] B. Nikolić and B. Sazdović, JHEP 8 (21) 37. [5] F. Ardalan, H. Arfaei, M. M. Sheikh-Jabbari, Nucl. Phys. B576, 578 (2); C. S. Chu, P. M. Ho, Nucl. Phys. B568, 447 (2); T. Lee, Phys. Rev. D62 (2) [6] B. Sazdović, Eur. Phys. J C44 (25) 599; B. Nikolić and B. Sazdović, Phys. Rev. D74 (26) 4524; B. Nikolić and B. Sazdović, Phys. Rev. D75 (27) 8511; B. Nikolić and B. Sazdović, Adv. Theor. Math. Phys. 14 (21) 1. [7] B. Nikolić and B. Sazdović, Phys. Lett. B666 (28) 4. [8] N. Seiberg and E. Witten, JHEP 9 (1999) 32. [9] J. de Boer, P. A. Grassi and P. van Nieuwenhuizen, Phys. Lett. B574 (23) 98. [1] F. Riccioni, Phys. Lett. B56 (23) 223; N. Berkovits, ICTP Lectures on Covariant Quantization of the Superstring, hep-th/2959.
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 περισσότεραRelativistic particle dynamics and deformed symmetry
Relativistic particle dynamics and deformed Poincare symmetry Department for Theoretical Physics, Ivan Franko Lviv National University XXXIII Max Born Symposium, Wroclaw Outline Lorentz-covariant deformed
Διαβάστε περισσότεραMATH423 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 περισσότεραHigher Derivative Gravity Theories
Higher Derivative Gravity Theories Black Holes in AdS space-times James Mashiyane Supervisor: Prof Kevin Goldstein University of the Witwatersrand Second Mandelstam, 20 January 2018 James Mashiyane WITS)
Διαβάστε περισσότερα2 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 περισσότεραPhys460.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 περισσότερα4.6 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 περισσότεραAppendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee
Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset
Διαβάστε περισσότεραD 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 περισσότεραSecond 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 περισσότεραLecture 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 περισσότεραCongruence 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 περισσότεραSpace-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 περισσότεραPartial 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 περισσότεραSection 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 περισσότεραMatrices 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 περισσότεραderivation 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= {{D α, D α }, D α }. = [D α, 4iσ µ α α D α µ ] = 4iσ µ α α [Dα, D α ] µ.
PHY 396 T: SUSY Solutions for problem set #1. Problem 2(a): First of all, [D α, D 2 D α D α ] = {D α, D α }D α D α {D α, D α } = {D α, D α }D α + D α {D α, D α } (S.1) = {{D α, D α }, D α }. Second, {D
Διαβάστε περισσότεραEE512: 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 περισσότεραC.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 περισσότεραCHAPTER 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 περισσότεραExercises 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 περισσότεραHOMEWORK 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 περισσότεραΑπόκριση 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 περισσότεραConcrete 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 περισσότεραMath221: 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 περισσότερα3.4 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 περισσότεραExample 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( y) Partial Differential Equations
Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate
Διαβάστε περισσότεραEvery set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
Διαβάστε περισσότεραforms 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 περισσότεραJesse 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 περισσότεραHomework 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 περισσότεραSecond Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Διαβάστε περισσότεραHomework 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 περισσότεραTutorial problem set 6,
GENERAL RELATIVITY Tutorial problem set 6, 01.11.2013. SOLUTIONS PROBLEM 1 Killing vectors. a Show that the commutator of two Killing vectors is a Killing vector. Show that a linear combination with constant
Διαβάστε περισσότεραNotes on the Open Economy
Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.
Διαβάστε περισσότερα6.3 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 περισσότεραSCHOOL 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 περισσότεραSrednicki 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 περισσότεραStrain gauge and rosettes
Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified
Διαβάστε περισσότεραSolutions 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 περισσότεραDESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.
DESIGN OF MACHINERY SOLUTION MANUAL -7-1! PROBLEM -7 Statement: Design a double-dwell cam to move a follower from to 25 6, dwell for 12, fall 25 and dwell for the remader The total cycle must take 4 sec
Διαβάστε περισσότεραOn a four-dimensional hyperbolic manifold with finite volume
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Numbers 2(72) 3(73), 2013, Pages 80 89 ISSN 1024 7696 On a four-dimensional hyperbolic manifold with finite volume I.S.Gutsul Abstract. In
Διαβάστε περισσότεραApproximation 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 περισσότεραStatistical 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 περισσότεραSCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018
Journal of rogressive Research in Mathematics(JRM) ISSN: 2395-028 SCITECH Volume 3, Issue 2 RESEARCH ORGANISATION ublished online: March 29, 208 Journal of rogressive Research in Mathematics www.scitecresearch.com/journals
Διαβάστε περισσότεραSection 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 περισσότεραThe 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 περισσότερα1 String with massive end-points
1 String with massive end-points Πρόβλημα 5.11:Θεωρείστε μια χορδή μήκους, τάσης T, με δύο σημειακά σωματίδια στα άκρα της, το ένα μάζας m, και το άλλο μάζας m. α) Μελετώντας την κίνηση των άκρων βρείτε
Διαβάστε περισσότεραAreas 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 περισσότεραFinite 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 περισσότεραECE Spring Prof. David R. Jackson ECE Dept. Notes 2
ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =
Διαβάστε περισσότεραChapter 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 περισσότεραDerivation of Optical-Bloch Equations
Appendix C Derivation of Optical-Bloch Equations In this appendix the optical-bloch equations that give the populations and coherences for an idealized three-level Λ system, Fig. 3. on page 47, will be
Διαβάστε περισσότεραOrdinal 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 περισσότεραGeodesic Equations for the Wormhole Metric
Geodesic Equations for the Wormhole Metric Dr R Herman Physics & Physical Oceanography, UNCW February 14, 2018 The Wormhole Metric Morris and Thorne wormhole metric: [M S Morris, K S Thorne, Wormholes
Διαβάστε περισσότερα2. 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 περισσότεραCRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
Διαβάστε περισσότεραPARTIAL 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 περισσότεραExercise 1.1. Verify that if we apply GS to the coordinate basis Gauss form ds 2 = E(u, v)du 2 + 2F (u, v)dudv + G(u, v)dv 2
Math 209 Riemannian Geometry Jeongmin Shon Problem. Let M 2 R 3 be embedded surface. Then the induced metric on M 2 is obtained by taking the standard inner product on R 3 and restricting it to the tangent
Διαβάστε περισσότεραA Note on Intuitionistic Fuzzy. Equivalence Relation
International Mathematical Forum, 5, 2010, no. 67, 3301-3307 A Note on Intuitionistic Fuzzy Equivalence Relation D. K. Basnet Dept. of Mathematics, Assam University Silchar-788011, Assam, India dkbasnet@rediffmail.com
Διαβάστε περισσότεραSolution 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 περισσότεραNon-commutative Gauge Theories and Seiberg Witten Map to All Orders 1
Non-commutative Gauge Theories and Seiberg Witten Map to All Orders 1 Kayhan ÜLKER Feza Gürsey Institute * Istanbul, Turkey (savefezagursey.wordpress.com) The SEENET-MTP Workshop JW2011 1 K. Ulker, B Yapiskan
Διαβάστε περισσότεραAreas 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 περισσότεραMath 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 περισσότεραProblem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.
Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +
Διαβάστε περισσότεραForced Pendulum Numerical approach
Numerical approach UiO April 8, 2014 Physical problem and equation We have a pendulum of length l, with mass m. The pendulum is subject to gravitation as well as both a forcing and linear resistance force.
Διαβάστε περισσότεραST5224: 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 περισσότεραSPECIAL FUNCTIONS and POLYNOMIALS
SPECIAL FUNCTIONS and POLYNOMIALS Gerard t Hooft Stefan Nobbenhuis Institute for Theoretical Physics Utrecht University, Leuvenlaan 4 3584 CC Utrecht, the Netherlands and Spinoza Institute Postbox 8.195
Διαβάστε περισσότεραTridiagonal 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 περισσότεραSpinors and σ-matrices in 10 dimensions It is well known that in D-dimensional space-time Dirac spinor has 2 D 2
PiTP Study Guide to Spinors in D and 0D S.J.Gates Jr. John S. Toll Professor of Physics Director Center for String and Particle Theory University of Maryland Tel: 30-405-6025 Physics Department Fax: 30-34-9525
Διαβάστε περισσότεραHomework 4 Solutions Weyl or Chiral representation for γ-matrices. Phys624 Dirac Equation Homework 4
Homework 4 Solutions 4.1 - Weyl or Chiral representation for γ-matrices 4.1.1: Anti-commutation relations We can write out the γ µ matrices as where ( ) 0 σ γ µ µ = σ µ 0 σ µ = (1, σ), σ µ = (1 2, σ) The
Διαβάστε περισσότεραSection 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 περισσότεραω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω
0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +
Διαβάστε περισσότεραk 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 περισσότεραDirac Matrices and Lorentz Spinors
Dirac Matrices and Lorentz Spinors Background: In 3D, the spinor j = 1 representation of the Spin3) rotation group is constructed from the Pauli matrices σ x, σ y, and σ k, which obey both commutation
Διαβάστε περισσότεραReminders: 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 περισσότεραOverview. 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 περισσότεραVariational Wavefunction for the Helium Atom
Technische Universität Graz Institut für Festkörperphysik Student project Variational Wavefunction for the Helium Atom Molecular and Solid State Physics 53. submitted on: 3. November 9 by: Markus Krammer
Διαβάστε περισσότεραb. 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 περισσότεραSymmetric Stress-Energy Tensor
Chapter 3 Symmetric Stress-Energy ensor We noticed that Noether s conserved currents are arbitrary up to the addition of a divergence-less field. Exploiting this freedom the canonical stress-energy tensor
Διαβάστε περισσότεραQuadratic Expressions
Quadratic Expressions. The standard form of a quadratic equation is ax + bx + c = 0 where a, b, c R and a 0. The roots of ax + bx + c = 0 are b ± b a 4ac. 3. For the equation ax +bx+c = 0, sum of the roots
Διαβάστε περισσότεραΚΥΠΡΙΑΚΗ 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 περισσότεραParametrized Surfaces
Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some
Διαβάστε περισσότεραHigher spin gauge theories and their CFT duals
Higher spin gauge theories and their CFT duals E-mail: hikida@phys-h.keio.ac.jp 2 AdS Vasiliev AdS/CFT 4 Vasiliev 3 O(N) 3 Vasiliev 2 W N 1 AdS/CFT g µν Vasiliev AdS [1] AdS/CFT anti-de Sitter (AdS) (CFT)
Διαβάστε περισσότεραCHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS
CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS EXERCISE 01 Page 545 1. Use matrices to solve: 3x + 4y x + 5y + 7 3x + 4y x + 5y 7 Hence, 3 4 x 0 5 y 7 The inverse of 3 4 5 is: 1 5 4 1 5 4 15 8 3
Διαβάστε περισσότεραLocal Approximation with Kernels
Local Approximation with Kernels Thomas Hangelbroek University of Hawaii at Manoa 5th International Conference Approximation Theory, 26 work supported by: NSF DMS-43726 A cubic spline example Consider
Διαβάστε περισσότεραMean 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 περισσότεραEcon 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 περισσότεραExercises 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 περισσότεραSpherical Coordinates
Spherical Coordinates MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Fall 2011 Spherical Coordinates Another means of locating points in three-dimensional space is known as the spherical
Διαβάστε περισσότεραw 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 περισσότεραInverse 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 περισσότεραGeneral 2 2 PT -Symmetric Matrices and Jordan Blocks 1
General 2 2 PT -Symmetric Matrices and Jordan Blocks 1 Qing-hai Wang National University of Singapore Quantum Physics with Non-Hermitian Operators Max-Planck-Institut für Physik komplexer Systeme Dresden,
Διαβάστε περισσότεραLecture 15 - Root System Axiomatics
Lecture 15 - Root System Axiomatics Nov 1, 01 In this lecture we examine root systems from an axiomatic point of view. 1 Reflections If v R n, then it determines a hyperplane, denoted P v, through the
Διαβάστε περισσότεραNumerical 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 περισσότεραJackson 2.25 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell
Jackson 2.25 Hoework Proble Solution Dr. Christopher S. Baird University of Massachusetts Lowell PROBLEM: Two conducting planes at zero potential eet along the z axis, aking an angle β between the, as
Διαβάστε περισσότερα«Χρήσεις γης, αξίες γης και κυκλοφοριακές ρυθμίσεις στο Δήμο Χαλκιδέων. Η μεταξύ τους σχέση και εξέλιξη.»
ΕΘΝΙΚΟ ΜΕΤΣΟΒΙΟ ΠΟΛΥΤΕΧΝΕΙΟ ΣΧΟΛΗ ΑΓΡΟΝΟΜΩΝ ΚΑΙ ΤΟΠΟΓΡΑΦΩΝ ΜΗΧΑΝΙΚΩΝ ΤΟΜΕΑΣ ΓΕΩΓΡΑΦΙΑΣ ΚΑΙ ΠΕΡΙΦΕΡΕΙΑΚΟΥ ΣΧΕΔΙΑΣΜΟΥ ΔΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ: «Χρήσεις γης, αξίες γης και κυκλοφοριακές ρυθμίσεις στο Δήμο Χαλκιδέων.
Διαβάστε περισσότερα( ) 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