Some definite integrals connected with Gauss s sums
|
|
- Μυρίνα Μελετόπουλος
- 6 χρόνια πριν
- Προβολές:
Transcript
1 Some definite integrls connected with Guss s sums Messenger of Mthemtics XLIV If n is rel nd positive nd I(t where I(t is the imginry prt of t is less thn either n or we hve cos πtx coshπx e iπnx2 dx = 2 = n exp When n = the ove formul reduces to cos πtx coshπx sinπx2 dx = tn{ 8 π( t2 } cosπtxcos2πxy e iπnx2 dxdy cosh πy ( } { 4 iπ t2 cos πtx n coshπnx eiπnx2 dx. ( cos πtx coshπx cosπx2 dx. (2 if t = nd φ( = Ψ( = cosπnx 2 coshπx dx sinπnx 2 coshπx dx (3 then φ( = (2 Ψ ( +Ψ( Ψ( = (2 φ ( φ(. Similrly if 2 3 I(t is less thn either or n we hve (3 cos πtx +2cosh(2πx/ 3 eiπnx2 dx = ( } n exp { 4 iπ t2 cos πtx n +2cosh(2πnx/ 3 e iπnx2 dx. (4
2 76 Pper 2 If in (4 we suppose n = we otin nd if t = nd then cosπtxsinπx 2 +2cosh(2πx/ 3 dx = tn{ 8 π( t2 } φ( = Ψ( = cosπnx 2 +2cosh(2πx/ 3 dx sinπnx 2 +2cosh(2πx/ 3 dx φ( = (2 Ψ ( +Ψ( cosπtxcosπx 2 +2cosh(2πx/ 3 dx; (5 (2 ( Ψ( = φ φ(. In similr mnner we cn prove tht sin πtx tnhπx e iπnx2 dx = { } n exp 4 (+ iπ t2 sin πtx n tnhπnx eiπnx2 dx. (7 If we put n = in (7 we otin Now sin πtx tnhπx cosπx2 dx = tn{ 8 π(+t2 } sin tx lim t t tnhx eicx2 dx = lim t t = e icx e 2 x (6 (6 sin πtx tnhπx sinπx2 dx. (8 2sintx e 2x eicx2 dx+lim t sin tx e icx2 dx t dx+ i 2c. (9 Hence dividingothsidesof (7 yt ndmkingt weotin theresultcorresponding to (3 nd (6 viz.: if cos πnx φ( = e 2π x dx Ψ( = ( 2πn + sin πnx e 2π x dx
3 Some definite integrls connected with Guss s sums 77 then φ( = n (2 Ψ ( Ψ( Ψ( = n (2 φ ( +φ(. ( 2. I shll now shew tht the integrl ( my e expressed in finite terms for ll rtionl vlues of n. Consider the integrl J(t = If R( nd t re positive we hve J(t = 4 π r= r= costx dx cosh 2 πx 2 +x 2. ( r (2r + x 2 +(2r + 2 costx 2 +x 2 dx ( r = 2 {e (2r+t 2 (2r + 2 } (2r +e t = πe t 2cos +2 2π r= ( r e (2r+t 2 (2r + 2 ( nd it is esy to see tht this lst eqution remins true when t is complex provided R(t > nd I(t 2π. Thus the integrl J(t cn e expressed in finite terms for ll rtionl vlues of. Thus for exmple we hve costx dx cosh 2 πx +x 2 = coshtlog(2cosht tsinht (2 cos 2tx dx cosh πx+x 2 = 2cosht (e2t tn e t +e 2t tn e t nd so on. Now let Then if R( > F( = e n F(dn = cos 2tx coshπx e iπnx2 dx. (3 cos 2tx dx cosh πx+iπx2. (4
4 78 Pper 2 Now let Then f( = ( r exp{ (2r +t+ 4 (2r +2 iπn} r= + { ( } exp i n 4 π t2 πn r= ( r exp { (2r + t } n 4 (2r +2iπ.(5 n e n f(dn = = r= ( r e (2r+t ( π 4 (2r +2 iπ + 2 exp{ (2/π( it} (+icosh{(+i ( 2 π} cos 2tx dx cosh πx+iπx2 (6 in virtue of (; nd therefore Now it is known tht if φ( is continuous nd e n {F( f(}dn =. (7 e n φ(dn = for ll positive vlues of (or even only for n infinity of such vlues in rithmeticl progressio then φ( = for ll positive vlues of n. Hence F( = f(. (8 Equting the rel nd imginry prts in (3 nd (5 we hve cos 2tx coshπx cosπnx2 dx = { e t cos πn 4 e 3t cos 9πn 4 +e 5t cos 25πn } 4 + ( π {e t/n cos n 4 t2 πn + π ( π e 3t/n cos 4n 4 t2 πn + 9π } + (9 4n
5 Some definite integrls connected with Guss s sums 79 { cos 2tx coshπx sinπnx2 dx = e t sin πn 4 e 3t sin 9πn 4 +e 5t sin 25πn } 4 + ( π {e t/n sin n 4 t2 πn + π ( π e 3t/n sin 4n 4 t2 πn + 9π } +. (2 4n We cn verify the results (8 (9 nd (2 y mens of the eqution (. This eqution cn e expressed s functionl eqution in F( nd it is esy to see tht f( stisfies the sme eqution. The right-hnd side of these equtions cn e expressed in finite terms if n is ny rtionl numer. For let n = / where nd re ny two positive integers nd one of them is odd. Then the results (9 nd (2 reduce to ( cos 2tx πx 2 2cosht coshπx cos dx = [cosh{( t} cos(π/4 cosh{(3 t} cos(9π/4 +cosh{(5 t}cos(25π/4 to terms] ( [ {( + cosh } ( π t cos 4 t2 π + π 4 {( cosh 3 } ( π t cos 4 t2 π + 9π 4 + to terms ] (2 ( cos 2tx πx 2 2cosht coshπx sin dx = [cosh{( t} sin(π/4 cosh{(3 t} sin(9π/4 +cosh{(5 t}sin(25π/4 to terms] ( [ {( + cosh } ( π t sin 4 t2 π + π 4 {( cosh 3 } ( π t sin 4 t2 π + 9π ] + to terms. (22 4 Thus for exmple we hve when = nd = cosπx 2 coshπx cos2πtx dx = + 2sinπt 2 2 2coshπt (23
6 8 Pper 2 sinπx 2 coshπx It is esy to verify tht (23 nd (24 stisfy the reltion (2. The vlues of the integrls + 2cosπt 2 cos2πtx dx = 2. (24 2coshπt cosπnx 2 coshπx dx sinπnx 2 coshπx dx cn e otined esily from the preceding results y putting t = nd need no specil discussion. By successive differentitions of the results (9 nd (2 with respect to t nd n we cn evlute the integrls 2m sintx x cosh πx 2m costx x cosh πx cos sin πnx2 dx cos sin πnx2 dx for ll rtionl vlues of n nd ll positive integrl vlues of m. Thus for exmple we hve x 2cosπx2 coshπx dx = 8 2 4π (26 x 2 sinπx2 coshπx dx = (25 3. We cn get mny interesting results y pplying the theory of Cuchy s reciprocl functions to the preceding results. It is known tht if φ(xcosknx dx = Ψ( (27 then (i 2 α{ 2 φ(+φ(α+φ(2α+φ(3α+ } = 2Ψ(+Ψ(β+Ψ(2β+Ψ(3β+ (27 with the condition αβ = 2π/k; (ii α 2{φ(α φ(3α φ(5α+φ(7α+φ(9α } = Ψ(β Ψ(3β Ψ(5β+Ψ(7β+Ψ(9β (27 with the condition αβ = π/4k;
7 Some definite integrls connected with Guss s sums 8 (iii α 3{φ(α φ(5α φ(7α+φ(α +φ(3α } = Ψ(β Ψ(5β Ψ(7β+Ψ(β+Ψ(3β (27 with the condition αβ = π/6k where re the odd nturl numers without the multiples of 3. There re of course corresponding results for the function such s φ(xsinknx dx = Ψ( (28 α{φ(α φ(3α+φ(5α } = Ψ(β Ψ(3β+Ψ(5β with the condition αβ = π/2k. Thus from (23 nd (27 (i we otin the following results. If F(αβ = { } α 2 + cosr 2 πα 2 sinr 2 πβ 2 β cosh rπα coshrπβ (29 r= r= then F(αβ = F(βα = (2α{ 2 +e πα +e 4πα +e 9πα + } 2 provided tht αβ =. 4. If insted of strting with the integrl ( we strt with the corresponding sine integrl we cn shew tht when R( nd R(t re positive nd I(t π sintx dx sinh πx 2 +x 2 = 2 2 πe t 2sinπ + r= ( r e rt 2 r 2. (3 Hence the ove integrl cn e expressed in finite terms for ll rtionl vlues of. For exmple we hve From (3 we cn deduce tht sintx sinh 2 πx dx +x 2 = et tn e t e t tn e t. (3 sin 2tx sinhπx e iπnx2 dx = 2 e 2t+iπn +e 4t+4iπn e 6t+9iπn + {( } exp n 4 π + t2 i {e (t+ 4 iπ/n +e (3t+9 4 iπ/n + } (32 πn
8 82 Pper 2 R(t eing positive nd I(t 2π. The right-hnd side cn e expressed in finite terms for ll rtionl vlues of n. Thus for exmple we hve cosπx 2 sinhπx sinπx 2 sinhπx coshπt cosπt2 sin2πtx dx = (33 2sinhπt sin2πtx dx = sinπt2 2sinhπt (34 nd so on. Applying the formul (28 to (33 nd (34 we hve when αβ = 4 α ( rcos{(2r +2 πα 2 } sinh{(2r +πα} r= + β ( rcos{(2r +2 πβ 2 } sinh{(2r +πβ} r= = 2 α{ 2 +e 2πα +e 8πα +e 8πα + } 2 ; (35 α ( rsin{(2r +2 πα 2 } sinh{(2r +πα} r= = β ( rsin{(2r +2 πβ 2 } sinh{(2r +πβ}. By successive differentition of (32 with respect to t nd n we cn evlute the integrls 2m costx cos x sinh πx sin πnx2 dx 2m sintx x sinh πx r= cos sin πnx2 dx for ll rtionl vlues of n nd ll positive integrl vlues of m. Thus for exmple we hve x cosπx2 sinhπx dx = 8 x sinπx2 sinhπx dx = 4π x 3cosπx2 sinhπx dx = ( π 2 x 3sinπx2 sinhπx dx = 6π nd so on. The denomintors of the integrnds in (25 nd (36 re cosh πx nd sinh πx. Similr integrls hving the denomintors of their integrnds equl to r coshπ r xsinhπ r x (36 (37
9 Some definite integrls connected with Guss s sums 83 cn e evluted if r nd r re rtionl y splitting up the integrnd into prtil frctions. 5. The preceding formulæ my e generlised. Thus it my e shewn tht if R( nd R(t re positive I(t π nd < R(θ < then sinπθ = π 2 costx coshπx+cosπθ dx 2 +x 2 e t sinπθ cosπ+cosπθ + r= { } e (2r+ θt 2 (2r + θ 2 e (2r++θt 2 (2r ++θ 2. (38 From (38 it cn e deduced tht if n nd R(t re positive I(t π nd < θ < then costx sinπθ coshπx+cosπθ e iπnx2 dx = {e (2r+ θt+(2r+ θ2iπn e (2r++θt+(2r++θ2iπn } r= + } exp { (π 4 i t2 ( r sinrπθe (2rt+r2iπ/4n. (39 n πn The right-hnd side cn e expressed in finite terms if n nd θ re rtionl. In prticulr when θ = 3 we hve r= costx +2cosh(2πx/ 3 e iπnx2 dx = 2 {e 3 (t 3 iπ e 3 (2t 3 4iπ +e 3 (4t 3 6iπ } + } { (π 2 n exp 4 i t2 πn {e (t 3+iπ/3n e (2t 3+4iπ/3n +e (4t 3+6iπ/3n } (4 where re the nturl numers without the multiples of 3.
10 84 Pper 2 As n exmple when n = we hve cosπx 2 cosπtx +2cosh(2πx/ 3 dx = 2sin{(π 3πt2 /2} 8cosh(πt/ 3 4 sinπx 2 cosπtx +2cosh(2πx/ 3 dx = 3+2cos{(π 3πt 2 /2} 8cosh(πt/. 3 4 (4 6. The formul (32 ssumes net nd elegnt form when t is chnged to t + 2iπ. We hve then sintx tnhπx e iπnx2 dx (n > t > = { 2 +e t+iπn +e 2t+4iπn +e 3t+9iπn + } { ( } exp n 4 i π + t2 { πn 2 +e (t+iπ/n +e (2t+4iπ/n + }. (42 In prticulr when n = we hve cosπx 2 tnhπx sin2πtx dx = 2 tnhπt{ cos( 4 π +πt2 } sinπx 2 tnhπx sin2πtx dx = 2 tnhπtsin( 4 π +πt2. (43 We shll now consider n importnt specil cse of (42. It cn esily e seen from (9 tht the left-hnd side of (42 when divided y t tends to cos πnx e 2π x dx i 2πn + sin πnx e 2π x dx s t. But the limit of the right-hnd side of (42 divided y t cn e found when n is rtionl. Let then n = / where nd re ny two positive integers nd let (44 φ( = cos πnx e 2π x dx Ψ( = 2πn + sin πnx e 2π x dx.
11 Some definite integrls connected with Guss s sums 85 The reltion etween φ( nd Ψ( hs een stted lredy in (. From (42 nd (44 it cn esily e deduced tht if nd re oth odd then ( r= φ = 4 ( 2rcos r= ( r= Ψ = 4 ( 2rsin r= ( r 2 π ( r 2 π ( ( r= ( 2rsin r= r= ( 2rcos r= ( 4 π + r2 π ( 4 π + r2 π (45 It cn esily e seen tht these stisfy the reltion (. Similrly when one of nd is odd nd the other even it cn e shewn tht φ ( Ψ ( σ = 4π 2 ( + 2 σ = 4π + 2 ( 2 r= r= r( r r= r= r( r r= r= r( r r= r= r( r ( cos r 2 π ( sin 4 π + r2 π ( sin r 2 π cos ( 4 π + r2 π (46 where σ = ( cos 4 π + r2 π σ = sin ( 4 π + r2 π = ( sin r 2 π = cos ( r 2 π. (47 Thus for exmple we hve φ( = 2 φ( = φ(2 = φ(6 = φ ( 2 = 4π φ( φ(4 = 3 2 = (48 nd so on. By differentiting (42 with respect to n we cn evlute the integrls x m e 2π x cos sin πnx dx (49
12 86 Pper 2 for ll rtionl vlues of n nd positive integrl vlues of m. Thus for exmple we hve nd so on. xcos 2 πx e 2π x dx = 3 4π 8π 2 xcos2πx e 2π x dx = 64 ( 2 3 π + 5 π 2 x 2 cos2πx e 2π x dx = 256 ( 5π + 5π 2 (5
Oscillatory integrals
Oscilltory integrls Jordn Bell jordn.bell@gmil.com Deprtment of Mthemtics, University of Toronto August, 0 Oscilltory integrls Suppose tht Φ C R d ), ψ DR d ), nd tht Φ is rel-vlued. I : 0, ) C by Iλ)
Διαβάστε περισσότεραSolutions 3. February 2, Apply composite Simpson s rule with m = 1, 2, 4 panels to approximate the integrals:
s Februry 2, 216 1 Exercise 5.2. Apply composite Simpson s rule with m = 1, 2, 4 pnels to pproximte the integrls: () x 2 dx = 1 π/2, (b) cos(x) dx = 1, (c) e x dx = e 1, nd report the errors. () f(x) =
Διαβάστε περισσότεραSolutions_3. 1 Exercise Exercise January 26, 2017
s_3 Jnury 26, 217 1 Exercise 5.2.3 Apply composite Simpson s rule with m = 1, 2, 4 pnels to pproximte the integrls: () x 2 dx = 1 π/2 3, (b) cos(x) dx = 1, (c) e x dx = e 1, nd report the errors. () f(x)
Διαβάστε περισσότεραAMS 212B Perturbation Methods Lecture 14 Copyright by Hongyun Wang, UCSC. Example: Eigenvalue problem with a turning point inside the interval
AMS B Perturbtion Methods Lecture 4 Copyright by Hongyun Wng, UCSC Emple: Eigenvlue problem with turning point inside the intervl y + λ y y = =, y( ) = The ODE for y() hs the form y () + λ f() y() = with
Διαβάστε περισσότεραΤΜΗΜΑ ΗΛΕΚΤΡΟΛΟΓΩΝ ΜΗΧΑΝΙΚΩΝ ΚΑΙ ΜΗΧΑΝΙΚΩΝ ΥΠΟΛΟΓΙΣΤΩΝ
ΗΜΥ ΔΙΑΚΡΙΤΗ ΑΝΑΛΥΣΗ ΚΑΙ ΔΟΜΕΣ ΤΜΗΜΑ ΗΛΕΚΤΡΟΛΟΓΩΝ ΜΗΧΑΝΙΚΩΝ ΚΑΙ ΜΗΧΑΝΙΚΩΝ ΥΠΟΛΟΓΙΣΤΩΝ ΗΜΥ Διακριτή Ανάλυση και Δομές Χειμερινό Εξάμηνο 6 Σειρά Ασκήσεων Ακέραιοι και Διαίρεση, Πρώτοι Αριθμοί, GCD/LC, Συστήματα
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 περισσότεραFourier 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 περισσότεραPractice 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 περισσότεραINTEGRAL INEQUALITY REGARDING r-convex AND
J Koren Mth Soc 47, No, pp 373 383 DOI 434/JKMS47373 INTEGRAL INEQUALITY REGARDING r-convex AND r-concave FUNCTIONS WdAllh T Sulimn Astrct New integrl inequlities concerning r-conve nd r-concve functions
Διαβάστε περισσότεραΣχολή Εφαρμοσμένων Μαθηματικών και Φυσικών Επιστημών. Εθνικό Μετσόβιο Πολυτεχνείο. Thales Workshop, 1-3 July 2015.
Σχολή Εφαρμοσμένων Μαθηματικών και Φυσικών Επιστημών Εθνικό Μετσόβιο Πολυτεχνείο Thles Worksho, 1-3 July 015 The isomorhism function from S3(L(,1)) to the free module Boštjn Gbrovšek Άδεια Χρήσης Το παρόν
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 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 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 περισσότεραReview-2 and Practice problems. sin 2 (x) cos 2 (x)(sin(x)dx) (1 cos 2 (x)) cos 2 (x)(sin(x)dx) let u = cos(x), du = sin(x)dx. = (1 u 2 )u 2 ( du)
. Trigonometric Integrls. ( sin m (x cos n (x Cse-: m is odd let u cos(x Exmple: sin 3 (x cos (x Review- nd Prctice problems sin 3 (x cos (x Cse-: n is odd let u sin(x Exmple: cos 5 (x cos 5 (x sin (x
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 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 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 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 περισσότεραIf ABC is any oblique triangle with sides a, b, and c, the following equations are valid. 2bc. (a) a 2 b 2 c 2 2bc cos A or cos A b2 c 2 a 2.
etion 6. Lw of osines 59 etion 6. Lw of osines If is ny oblique tringle with sides, b, nd, the following equtions re vlid. () b b os or os b b (b) b os or os b () b b os or os b b You should be ble to
Διαβάστε περισσότεραUniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
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 περισσότεραTo find the relationships between the coefficients in the original equation and the roots, we have to use a different technique.
Further Conepts for Avne Mthemtis - FP1 Unit Ientities n Roots of Equtions Cui, Qurti n Quinti Equtions Cui Equtions The three roots of the ui eqution x + x + x + 0 re lle α, β n γ (lph, et n gmm). The
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 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 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 περισσότεραSOLUTIONS TO PROBLEMS IN LIE ALGEBRAS IN PARTICLE PHYSICS BY HOWARD GEORGI STEPHEN HANCOCK
SOLUTIONS TO PROBLEMS IN LIE ALGEBRAS IN PARTICLE PHYSICS BY HOWARD GEORGI STEPHEN HANCOCK STEPHEN HANCOCK Chpter 6 Solutions 6.A. Clerly NE α+β hs root vector α+β since H i NE α+β = NH i E α+β = N(α+β)
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 περισσότεραOscillation of Nonlinear Delay Partial Difference Equations. LIU Guanghui [a],*
Studies in Mthemtil Sienes Vol. 5, No.,, pp. [9 97] DOI:.3968/j.sms.938455.58 ISSN 93-8444 [Print] ISSN 93-845 [Online] www.snd.net www.snd.org Osilltion of Nonliner Dely Prtil Differene Equtions LIU Gunghui
Διαβάστε περισσότεραSOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM
SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM Solutions to Question 1 a) The cumulative distribution function of T conditional on N n is Pr T t N n) Pr max X 1,..., X N ) t N n) Pr max
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 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 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 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 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 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 περισσότεραLecture 5: Numerical Integration
Lecture notes on Vritionl nd Approximte Metods in Applied Mtemtics - A Peirce UBC 1 Lecture 5: Numericl Integrtion Compiled 15 September 1 In tis lecture we introduce tecniques for numericl integrtion,
Διαβάστε περισσότεραElectromagnetic Waves I
Electromgnetic Wves I Jnury, 03. Derivtion of wve eqution of string. Derivtion of EM wve Eqution in time domin 3. Derivtion of the EM wve Eqution in phsor domin 4. The complex propgtion constnt 5. The
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 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 περισσότεραECE 308 SIGNALS AND SYSTEMS FALL 2017 Answers to selected problems on prior years examinations
ECE 308 SIGNALS AND SYSTEMS FALL 07 Answers to selected problems on prior years examinations Answers to problems on Midterm Examination #, Spring 009. x(t) = r(t + ) r(t ) u(t ) r(t ) + r(t 3) + u(t +
Διαβάστε περισσότεραSection 7.7 Product-to-Sum and Sum-to-Product Formulas
Section 7.7 Product-to-Sum and Sum-to-Product Fmulas Objective 1: Express Products as Sums To derive the Product-to-Sum Fmulas will begin by writing down the difference and sum fmulas of the cosine function:
Διαβάστε περισσότεραSpherical quadrangles with three equal sides and rational angles
Also vilble t http://mc-journl.eu ISSN 1855-3966 (printed edn.), ISSN 1855-3974 (electronic edn.) ARS MATHEMATICA CONTEMPORANEA 1 (017) 415 44 Sphericl qudrngles with three equl sides nd rtionl ngles Abstrct
Διαβάστε περισσότεραF19MC2 Solutions 9 Complex Analysis
F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at
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 περισσότεραCHAPTER (2) Electric Charges, Electric Charge Densities and Electric Field Intensity
CHAPTE () Electric Chrges, Electric Chrge Densities nd Electric Field Intensity Chrge Configurtion ) Point Chrge: The concept of the point chrge is used when the dimensions of n electric chrge distriution
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 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 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 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 περισσότεραCHAPTER 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 περισσότεραResearch Article The Study of Triple Integral Equations with Generalized Legendre Functions
Hindwi Pulishing Corportion Astrct nd Applied Anlysis Volume 28, Article ID 395257, 2 pges doi:.55/28/395257 Reserch Article The Study of Triple Integrl Equtions with Generlized Legendre Functions B. M.
Διαβάστε περισσότεραLAPLACE TYPE PROBLEMS FOR A DELONE LATTICE AND NON-UNIFORM DISTRIBUTIONS
Dedicted to Professor Octv Onicescu, founder of the Buchrest School of Probbility LAPLACE TYPE PROBLEMS FOR A DELONE LATTICE AND NON-UNIFORM DISTRIBUTIONS G CARISTI nd M STOKA Communicted by Mrius Iosifescu
Διαβάστε περισσότεραORDINAL ARITHMETIC JULIAN J. SCHLÖDER
ORDINAL ARITHMETIC JULIAN J. SCHLÖDER Abstract. We define ordinal arithmetic and show laws of Left- Monotonicity, Associativity, Distributivity, some minor related properties and the Cantor Normal Form.
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 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 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 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 περισσότεραON CONVERGENCE THEOREMS FOR FUZZY HENSTOCK INTEGRALS
Irnin Journl of Fuzzy Systems Vol. 14, No. 6, 2017 pp. 87-102 87 ON CONVERGENCE THEOREMS FOR FUZZY HENSTOCK INTEGRALS B. M. UZZAL AFSAN Abstrct. The min purpose of this pper is to estblish different types
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 περισσότεραTrigonometric Formula Sheet
Trigonometric Formula Sheet Definition of the Trig Functions Right Triangle Definition Assume that: 0 < θ < or 0 < θ < 90 Unit Circle Definition Assume θ can be any angle. y x, y hypotenuse opposite θ
Διαβάστε περισσότεραVidyamandir Classes. Solutions to Revision Test Series - 2/ ACEG / IITJEE (Mathematics) = 2 centre = r. a
Per -.(D).() Vdymndr lsses Solutons to evson est Seres - / EG / JEE - (Mthemtcs) Let nd re dmetrcl ends of crcle Let nd D re dmetrcl ends of crcle Hence mnmum dstnce s. y + 4 + 4 6 Let verte (h, k) then
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 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 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 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 περισσότεραPg 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 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 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 περισσότεραMathCity.org Merging man and maths
MathCity.org Merging man and maths Exercise 10. (s) Page Textbook of Algebra and Trigonometry for Class XI Available online @, Version:.0 Question # 1 Find the values of sin, and tan when: 1 π (i) (ii)
Διαβάστε περισσότεραANSWERSHEET (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 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 περισσότεραMA 342N Assignment 1 Due 24 February 2016
M 342N ssignment Due 24 February 206 Id: 342N-s206-.m4,v. 206/02/5 2:25:36 john Exp john. Suppose that q, in addition to satisfying the assumptions from lecture, is an even function. Prove that η(λ = 0,
Διαβάστε περισσότεραSimilarly, we may define hyperbolic functions cosh α and sinh α from the unit hyperbola
Universit of Hperbolic Functions The trigonometric functions cos α an cos α are efine using the unit circle + b measuring the istance α in the counter-clockwise irection along the circumference of the
Διαβάστε περισσότεραEvaluation of some non-elementary integrals of sine, cosine and exponential integrals type
Noname manuscript No. will be inserted by the editor Evaluation of some non-elementary integrals of sine, cosine and exponential integrals type Victor Nijimbere Received: date / Accepted: date Abstract
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 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 περισσότεραf (x) g (x) f (x) g (x) + f (x) g (x) f (x) g (x) Solved Examples Example 2: Prove that the determinant sinθ x 1
Mthemtis 7. f (x) g (x) (g) If (x) f (x) g (x) then f (x) g f (x) (x) g (x) (x) + or f (x) g (x) f (x) g (x) f (x) g (x) f (x) g (x) + f (x) g (x) f (x) g (x) (h) If f(x) g(x) h(x) (x) α β γ then f(x)dx
Διαβάστε περισσότεραOther 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 περισσότεραMath 446 Homework 3 Solutions. (1). (i): Reverse triangle inequality for metrics: Let (X, d) be a metric space and let x, y, z X.
Math 446 Homework 3 Solutions. (1). (i): Reverse triangle inequalit for metrics: Let (X, d) be a metric space and let x,, z X. Prove that d(x, z) d(, z) d(x, ). (ii): Reverse triangle inequalit for norms:
Διαβάστε περισσότεραA General Note on δ-quasi Monotone and Increasing Sequence
International Mathematical Forum, 4, 2009, no. 3, 143-149 A General Note on δ-quasi Monotone and Increasing Sequence Santosh Kr. Saxena H. N. 419, Jawaharpuri, Badaun, U.P., India Presently working in
Διαβάστε περισσότεραLecture 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 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 περισσότεραCoefficient Inequalities for a New Subclass of K-uniformly Convex Functions
International Journal of Computational Science and Mathematics. ISSN 0974-89 Volume, Number (00), pp. 67--75 International Research Publication House http://www.irphouse.com Coefficient Inequalities for
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 περισσότεραDifferentiation exercise show differential equation
Differentiation exercise show differential equation 1. If y x sin 2x, prove that x d2 y 2 2 + 2y x + 4xy 0 y x sin 2x sin 2x + 2x cos 2x 2 2cos 2x + (2 cos 2x 4x sin 2x) x d2 y 2 2 + 2y x + 4xy (2x cos
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 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 περισσότερα9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr
9.9 #. Area inside the oval limaçon r = + cos. To graph, start with = so r =. Compute d = sin. Interesting points are where d vanishes, or at =,,, etc. For these values of we compute r:,,, and the values
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 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 περισσότεραNowhere-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 περισσότεραChapter 7b, Torsion. τ = 0. τ T. T τ D'' A'' C'' B'' 180 -rotation around axis C'' B'' D'' A'' A'' D'' 180 -rotation upside-down C'' B''
Chpter 7b, orsion τ τ τ ' D' B' C' '' B'' B'' D'' C'' 18 -rottion round xis C'' B'' '' D'' C'' '' 18 -rottion upside-down D'' stright lines in the cross section (cross sectionl projection) remin stright
Διαβάστε περισσότεραDifferential equations
Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential
Διαβάστε περισσότεραReview Exercises for Chapter 7
8 Chapter 7 Integration Techniques, L Hôpital s Rule, and Improper Integrals 8. For n, I d b For n >, I n n u n, du n n d, dv (a) d b 6 b 6 (b) (c) n d 5 d b n n b n n n d, v d 6 5 5 6 d 5 5 b d 6. b 6
Διαβάστε περισσότεραNotes on Tobin s. Liquidity Preference as Behavior toward Risk
otes on Tobin s Liquidity Preference s Behvior towrd Risk By Richrd McMinn Revised June 987 Revised subsequently Tobin (Tobin 958 considers portfolio model in which there is one sfe nd one risky sset.
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 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 περισσότεραCorrections to Partial Differential Equations and Boundary-Value Problems with Applications by M. Pinsky, August 2001
Corrections to Prtil Differentil Equtions nd Boundry-Vlue Problems with Applictions by M. Pinsky, August pge 4, exercise : u(x, y) = e kx e k y pge 5, line : Newton s lw of... pge 5, line : u(x i ; t)
Διαβάστε περισσότεραMATHEMATICS. 1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81
1. If A and B are square matrices of order 3 such that A = -1, B =3, then 3AB = 1) -9 2) -27 3) -81 4) 81 We know that KA = A If A is n th Order 3AB =3 3 A. B = 27 1 3 = 81 3 2. If A= 2 1 0 0 2 1 then
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 περισσότερα