New Applications of an Improved (G /G)-expansion Method to Construct the Exact Solutions of Nonlinear PDEs
|
|
- Μνήμη Μέλιοι
- 7 χρόνια πριν
- Προβολές:
Transcript
1 Freund Publishing House Ltd. International Journal of Nonlinear Sciences & Numerical Simulation (4): New Applications of an Improved (G /G)-epansion Method to Construct the Eact Solutions of Nonlinear PEs Elsayed M. E. Zayed Khaled A. Gepreel Mathematics epartment Faculty of Science Taif University El-Taif El- Hawiyah Kingdom of Saudi Arabia Mathematics epartment Faculty of Science Zagazig University Zagazig Egypt Abstract In the present article we construct traveling wave solutions involving parameters of some nonlinear PEs in mathematical physics namely Konopelchenko-ubrovsky equations Kersten- Krasil Shchik equations Whitham- Broer Kaup equations the fifth order KdV equation using an improved ( G / G ) epansion method where G satisfies a second order linear ordinary differential equation. When these parameters are taken special values the solitary waves are derived from the traveling waves. The eact wave solutions are epressed by hyperbolic trigonometric rational functions. Comparison between this method the ep-function method is presented. Keywords: an improved ( G / G ) - epansion method traveling wave solutions solitary wave solutions nonlinear PEs ep-function method. Introduction In recent years the eact solutions of nonlinear PEs have been investigated by many authors (see for eample [-0] ) who are interested in nonlinear physical phenomena. Many powerful methods have been presented such as the tanh-method [7] the inverse scattering transform [] the Backlund transform [90] the generalized Riccati equation [-6] the Sine-Cosine method[] the F-epansion method [0] the Epfunction method [57] the ( G / G) epansion method [89] so on. In the present article we shall use a new method which is called an improved ( G / G) -epansion method to obtain the traveling wave solutions of Corresponding Author: emezayed@hotmail.com kagepreel@yahoo.com nonlinear PEs. The main idea of this method is that the traveling wave solutions of nonlinear evolution equations can be epressed by a polynomial in ( G / G) where G = G(ξ) satisfies the second order linear ordinary differential equation G ( ξ ) λg ( ξ) μg( ξ ) = 0 ξ = V t while λ μ V are constants. The degree of this polynomial can be determined by considering the homogeneous balance between the highest order derivatives the nonlinear terms appearing in the given nonlinear equations. The coefficients of this polynomial can be obtained by solving a set of algebraic equations resulted from the process of using the proposed method. Recently Bin et al [] Zayed et al [8] have obtained eact solutions of some nonlinear PEs using this method. In this article the improved ( G / G) epansion method will be used to determine the eact wave solutions of Konopelchenko-ubrovsky equations Kersten-
2 74 E.M.E. Zayed & K.A. Gepreel: New applications of improved (G /G)-epansion method to construct eact solutions of nonlinear PEs Krasil Shchik equations Whitham-Broer Kaup equations the fifth order KdV equation in terms of hyperbolic trigonometric rational functions. escription of an improved ( G/G) - epansion method Suppose that we have a nonlinear PE in the following form: F ( u u u u u u u...) = 0. (.) t y tt where uyt ( ) is an unknown unction F is a polynomial in u = u( y t) its partial derivatives in which the highest order derivatives nonlinear terms are involved. Let us now give the main steps for solving Eq. (.) using an improved ( G / G)-epansion method [8] as follows: Step. The traveling wave variable: uyt ( ) = uξ ( ) ξ = y- Vt (.) where V is a constant permits us reducing Eq. (.) to the following OE : Puu ( u u...) = 0. (.) where P is a polynomial in u( ξ ) its total derivatives. Step. Suppose that the solution of (.) can be epressed by a polynomial in ( G / G) as follows: u m i G = i m G (.4) where G = G( ξ ) satisfies the second order linear differential equation where G = G( ξ ) satisfies the second order linear differential equation G ( ξ ) λg ( ξ) μg( ξ) = 0 (.5) where i (i = 0 ± ±... ± m) λ μ are constants to be determined later m 0 or -m 0. The positive integer m can be y determined by considering the homogeneous balance between the highest order derivatives the nonlinear terms appearing in (.). Step. Substituting (.4) into (.) using (.5) collecting all terms with the same order of ( G / G) together then equating each coefficient of the resulted polynomial to zero yield a set of algebraic equations for i λ V μ. Step 4. Since the general solutions of (.5) have been well known for us then substituting i λ V μ the general solutions of (.5) into (.4) we have traveling wave solutions of the nonlinear differential equation (.). Applications In this section we apply the improved ( G / G)- epansion method to construct the traveling wave solutions for some nonlinear partial differential equations in mathematical physics as follows:. Eample. Konopelchenko-ubrovsky equations We start with the following Konopelchenko-ubrovsky equations [80] : ut u 6βuu u u wy u w= 0 w u y= 0 (.) where β are constants. For w y = 0 Eqs. (.) is called the Gardner equation. For = 0 Eqs.(.) is the well- known Kadomtsev- Petviashvili equation for β = 0 it is called modified Kadomtsev- Petviashvili equation. Let us now solve Eqs. (.) by the proposed method. To this end we see that the traveling wave variables uyt ( ) = u( ξ) vyt ( ) = v( ξ) ξ= y Vt (.) permit us to convert Eqs (.) into the following system:
3 ISSN: International Journal of Nonlinear Sciences & Numerical Simulation (4): Vu u βuu u u w u w = w u = (.) Suppose that the solutions of the system (.) can be epressed by two polynomials in terms of ( G / G) as follows: m i G G u= i w= βi G G i= m i= n n (.4) while G = G( ξ ) satisfies the second order linear OE (.5) while i β i are arbitrary constants. Considering the homogeneous balance between the highest order derivative u the nonlinear terms uu uw in (.) we get m= n=. Consequently we have G G 0 u = G G And G G 0 w = β G β G β It is easy to see that G G u = λ μ G G G G λ μ G G λ ( μ λ ) G G ( μ λ ) λμ G μ μλ λ G i (.5) (.6) (.7) G G G u = G G G G G (.8) 4 G G G u = 6 λ (8μ 7 λ ) G G G G G (8 μλ λ ) λ(8 μ λ ) G G G G (8 7 ) μ λ μ λμ G G 4 G 6 μ μλ μ λ μ. G (.9) On substituting (.5)-(.9) into (.) collecting all terms with the same powers of ( G / G) setting them to zero we get a system of algebraic equations which can be solved by the Maple or Mathematica to get the following results: Case 0 = ± [ ± β m λ ] = ± V = [ ( λ 8μ m 6λ ) β 6 β 0 ] μ μ β = ± = ± β = ±. (.0) Case μ 0 = ± [ ± β m λ] = ± V = [ ( λ 4μ m 6λ) β 6 β 0 ] μ β = ± = β = 0 (.) Case 0 = ± [ ± β m λ] = ± V = [ ( λ 4μ m 6λ) β 6 β0 ] β = ± = β = 0 (.) where 0.
4 76 E.M.E. Zayed & K.A. Gepreel: New applications of improved (G /G)-epansion method to construct eact solutions of nonlinear PEs Note that there are other cases which are omitted here. Since the solutions obtained here are so many we just list some eact solutions corresponding to case to illustrate the effectiveness of the improved ( G / G) epansion method. Substituting (.0) into (.5) (.6) yields G μ G u =± ± ± [ ± β m λ ] G G (.) G μ G w=± ± β0 G G where (.4) t ξ = [ ( λ 8μ m6λ) β 6 β0]. (.5) On solving Eq.(.5) substituting the value of the ratio ( G / G) into (.) (.4) we have the following eact solutions: Family. If λ 4μ> 0 then we have ξ ξ h λ w = β 0 m ± ξ ξ B cosh ξ ξ cosh sinh A A μ ± λ ξ ξ sinh cosh A B where = λ μ. Family. 4 If λ 4μ < 0 then we have u =± [ ± β m ] ξ ξ Asin ± ξ ξ Bsin (.7) Asin ξ ξ μ λ ± ξ Bsin ξ (.8) u =± [ ± β m ] h ± h h μ λ ± h (.6) ξ ξ Asin λ w = β0 m ± ξ ξ Bsin ξ ξ Asin μ λ ± ξ ξ Bsin (.9)
5 ISSN: International Journal of Nonlinear Sciences & Numerical Simulation (4): where = μ λ. Family. 4 If λ 4μ= 0 then we have B u =± [ ± β m ] ± ( Bξ A) μ B λ ± Bξ A (.0) λ B μ B λ w= β0 m ± ±. ( Bξ A) Bξ A (.) In particular if B= 0 A 0 λ > 0 μ = 0 then we deduce from (.6) (.7) that: λ λξ u =± [ ± β m ] ± coth (.) λ λ λξ w = β 0 m ± coth (.) while if B 0 B > A λ > 0 μ = 0 then we have: λ λξ u = ± [ ± β m ] ± tanh( ξ ) 0 (.4) λ λ λξ w = β 0 m ± tanh( ξ 0 ). (.5) Note that (.)- (.5) represent the solitary wave solutions of the Konopelchenko- ubrovsky equations (.) where t ξ = [ ( λ m6λ) β 6 β0] tanh A ξ 0 = ( ). (.6) B. Eample. Kersten- Krasil Shchik equations In this section we study the following Kersten- Krasil Shchik equations [6]: u u t w w t 6uu ww w w w w uw wu u w = 0. 6uww = 0 (.7) The traveling wave variables (.) permit us to convert Eqs. (.7) into: Vu u 6uu ww ww w u 6uww = 0 Vw w w w uw wu = 0. (.8) Considering the homogeneous balance between the highest order derivative u the nonlinear terms u u w w in (.8) we get n = m =. Thus the solutions of Eqs. (.8) have the following forms: G G G G 0 u = G G G G (.9) G G 0. w = β G β G β (.0) On substituting (.9) (.0) into (.8) collecting all terms with the same powers of ( G / G) setting them to zero we get a system of algebraic equations which can be solved with the Maple or Mathematica to get the following results: Case = = λ = 0 0 = λ = μ V = λ 8μ β = i β = iμ β 0 = iλ (.)
6 78 E.M.E. Zayed & K.A. Gepreel: New applications of improved (G /G)-epansion method to construct eact solutions of nonlinear PEs Case = = λ 0 = μ = μλ = μ β = i β = iμ β0 = 0 V = λ 8 μ (.) Case = 0 = 0 β = 0 = μ 0 0 = μλ β = iμ β = iλ V = λ 4μ. = μ (.) Note that there are other cases which are omitted here. Since the solutions obtained here are so many we just list some eact solutions corresponding to case. Substituting (.) into (.9) (.0) yield G G u λ λμ G μ G = ± G G G G (.4) G G w = i iμ iλ G G (.5) where ξ = ( λ 8 μ) t i =. Consequently we have the following eact wave solutions: Family. If λ 4μ > 0 then we have cosh sinh A B λ u = h cosh sinh A B λ λμ h cosh sinh A B λ μ h (.6) h Bsinh w=± i h h Bsinh i λ ± μ. h (.7) Family. If λ 4μ > 0 then we have ξ ξ sin cos A B λ u = ξ ξ Bsin ξ ξ Asin λ λμ ξ ξ Bsin ξ ξ Asin λ μ ξ ξ Bsin (.8)
7 ISSN: International Journal of Nonlinear Sciences & Numerical Simulation (4): ξ ξ Asin w=± i ξ ξ Bsin ξ ξ Asin i λ ± μ. ξ ξ Bsin (.9) Family. If λ 4μ = 0 then we have B B λ u = λμ ( Bξ A) Bξ A B λ λ μ Bξ A (.40) ib B λ w = ± iμ. Bξ A Bξ A (.4) In particular if B= 0 A 0 λ > 0 μ = 0 then we get from (.6) (.7) that: λ λξ λξ u = csc h ( ) v= iλ coth( ) (.4). Eample. Whitham- Broer Kaup equations In this section we study the following Whitham- Broer Kaup equations [56]: ut uu v βv = 0 (.44) v ( uv) βv u = 0 t where β are constants. The system (.44) is a complete integrable model which describes the dispersive long wave is shallow water. In this system β are real constants that represent different dispersive powers. We deduce from the homogeneous balance between the highest order derivatives the nonlinear terms in Eqs.(.44) that n = m =. Thus the solutions of Eqs. (.44) have the following forms: G G G G 0 u = G G G G (.45) G G G G 0. v= β G β β G G β G β (.46) On substituting (.45) (.46) into (.44) using the Maple or Mathematica we have the following cases: while if B 0 B > A λ > 0 μ = 0 then we get from (.6) (.7) that: λ λξ u = λξ v = iλ tanh( ξ0 ). sec h ( ξ0 ) (.4) Note that (.4) (.4) represent the solitary wave solutions of the Kersten- Krasil Shchik equations (.7) where ξ = λ t ξ 0 = tanh ( A/ B). Case. μ μ(λ ) = = λ 4μ 0( λ 4 μ) β 6μ 6 μ(5 λ ) = β = 800( λ 4 μ) 4000 ( λ 4 μ) β = = ( λ 4 μ) 600( λ 4 μ) β (0 λ 9λ 80λμ 47 μ) 800( λ 4 μ) 0 = 0λ 0λ 0 λ 80μ0 00μ V = 0( λ 4 μ) C = ( λ 4 μ)
8 80 E.M.E. Zayed & K.A. Gepreel: New applications of improved (G /G)-epansion method to construct eact solutions of nonlinear PEs C [ = 0 μ λ 8000 ( λ 4 μ) 5 0λ 0 μ 4 λ λ μ 4 μ0 λ λμ μ0λ 6 0 λ μ 4 0λ λ 0λ μ 0μ μ0 λ ] = = β = β = 0. (.47) Case. (0 λ ) = = λ 4μ 0( λ 4 μ) 6 β = = 800( λ 4 μ) 600( λ 4 μ) (40 λ λ 60 μ ) β = 800 ( λ 4 μ) 56 C = β = 000 ( λ 4 μ) ( λ 4 μ) (0λ 9λ 80λμ 47 μ) β0 = 800( λ 4 μ) 4 V = [400 λ ( λ 4 μ) 0λ 000λ μ 880λμ 6400μ 0 0μ 99 λ ] C = [ μ 8000 ( λ 4 μ) μλ 44000λ 970 λ 540 μ μλ 9000 μ 0λ μ0λ μ λ λ 4 980λ 0 089λ 0λμ 0 60λμ 6400 μ 0 ] = = β = β = 0 (.48) ± where = λ 4μ 0. 0 (4 μ λ ) We just now list the eact solutions corresponding to the case. On substituting (.47) into (.45) (.46) we get μ(0 λ ) G μ G 0 u = 0( λ 4 μ) G λ 4μ G (0 λ 9λ 80λμ v = 800( λ 4μ) 6μ (5 λ ) 4000 ( λ 4μ) where G G (.49) 47μ) 6μ 800( λ 4μ) G G (.50) t(0λ 0 0λ λ 80μ0 00μ ) ξ =. 0( λ 4μ) Consequently we deduce the following eact wave solutions: Family. If λ 4μ >0 then we have h Bsinh μ(0 λ ) λ u= 0( λ 4 μ) h h Bsinh μ λ 0 λ 4μ h (0λ 9λ 80λμ 47 μ) v= 800( λ 4 μ) h Bsinh 6 μ(5 λ ) λ 4000 ( λ 4 μ) h h Bsinh 6μ λ 800( λ 4 μ) h (.5)
9 ISSN: International Journal of Nonlinear Sciences & Numerical Simulation (4): Family. If λ 4μ <0 then we have ξ ξ Asin μ(0λ ) u λ = 0( λ 4 μ) ξ ξ Bsin ξ ξ Asin μ λ 0 λ 4μ ξ ξ Bsin (.5) (0λ 9λ 80λμ 47 μ) v= 800( λ 4 μ) ξ ξ Asin 6 μ(5 λ ) λ 4000 ( λ 4 μ) ξ ξ Bsin ξ ξ Asin 6μ λ. 800( λ 4 μ) ξ ξ Bsin (.54).4. Eample 4. The fifth order KdV equation In this section we study the following nonlinear fifth order KdV equation [44]: u u u βu u γuu u = 0 (.55) t where β γ are constants. The homogeneous balance of Eq. (.55) gives m =. Consequently the solution of Eq.(.55) has the form (.45). After some reduction we have the following cases: Case 60μ γμ β = 6μ 6 4 V = [44μ 9μ λ = 4 = = 0 where μ 0. Case γμ 0 = μ ] = μ (.56) (56 γ) ( λ 8 μ) 0 β = = = λ 4 4 V = μ μ γμλ γλ 6μλ 6 ( γ 48) γμ ] = = = 0 (.57) where 0. We just now list the eact solutions corresponding to Case. The eact solutions of Eq.(.55) have the following forms: Family If μ < 0 then we have h u = μ μ h μ Family μ ξ Bsinh μ ξ B cosh If μ > 0 then we have μ ξ Bsinh μ ξ B cosh μ ξ μ ξ Asin μ ξ B cos u = μ μ μ ξ B sin sin cos A μ ξ B μ ξ. μ cos sin A μ ξ B μ ξ μ ξ μ ξ. μ ξ μ ξ (.58) (.59)
10 8 E.M.E. Zayed & K.A. Gepreel: New applications of improved (G /G)-epansion method to construct eact solutions of nonlinear PEs get In particular if B = 0 A 0 μ < 0 then we coth tanh u = μ ξ μ ξ μ (.60) while if B 0 B > A μ < 0 then we get u = coth ( μξ ξ0 ) tanh ( μξ ξ0 ) μ (.6) where ξ0 = tanh ( A/ B). Note that (.60) (.6) represent the solitary wave solutions of (.55). 4. Ep-function Method Let us now compare between the ( G / G)- epansion method the other methods such as the Ep- function method introduced by He et al [5] to search for the eact solutions of nonlinear PEs. To this end we apply the Epfunction to the Konopelchenko-ubrovsky equations (.). Now we make the ansatz: a d ep (d ξ )... a-cep (-c ξ ) u= a q ep (q ξ)... a-pep (-p ξ) b k ep (k ξ )... b-mep (-m ξ ) w=. b ep (L ξ )... a ep (-I ξ ) L -I (.6) For the solutions of Eq. (.) we balance the highest order linear derivative u the nonlinear terms u u wu in Eqs (.). After some calculations we have d = q= L= k c= p= m= I. If we choose p = q =. In this case the solutions of Eqs.(.) can be epressed as follows: a ep ( ξ)a 0 aep (- ξ) u= b ep ( ξ)b 0 bep (- ξ) A ep ( ξ )A 0 Aep (- ξ ) w=. B ep ( ξ )B B ep (- ξ ) 0 (.6) Substituting (.6) into (.) collecting the coefficients of ep ( lξ ) l = 0 ±... we get a system of algebraic equations. Solving this system with the aid of the Maple we have the following results: Case i a = β = ( i ) b = b0 ( i 4) b0 ( i ) a = b = ; b0 ( i ) b0( A i ) B = A0 = b0 (i A i A) A = V = 6i A B0 = b0 a0 = 0 (.64) where A b 0 are arbitrary constants i =. The eact solutions take the following form: i b0 ( i 4) ep ( ξ ) ep (-ξ ) u = b0 ( i ) ep ( ξ ) b 0 ep (-ξ ) w= b0 ( i ) ep ( ξ)-b 0 ep (- ξ) b0( A i ) b0( A)( i ) [A ep ( ξ) ep (- ξ)] (.65) where ξ = ( 6i A ) t.
11 ISSN: International Journal of Nonlinear Sciences & Numerical Simulation (4): Case. b0( ab0 5ab0 a0 a0) β = (a b0 a0) ab0 a = B = b = b0 b0 B = b = B0 = b0 Ab 0 b0 A = = (a b a ) 0 0 A0= a0 Ab 0 a b0 V = {(8 ) a b0 aab 0 (a b0 a0) ( ) aba 0 0 a 0Ab 0 a0} (.66) where A b 0 a 0 are arbitrary constants. The eact solutions take the following form: ab0 aep( ξ) a0 ep( ξ) u = b0 ep( ξ) b0 ep( ξ) Ab 0 Aep( ξ ) a0 Ab 0 ab0 ep( ξ ) w = b0 ep( ξ) b0 ep( ξ) (.67) where t ξ = {(8 ) ab 0 aab 0 (a b0 a0) ( ) a ba a Ab a} Note that there are other cases which are omitted here. We think that the Ep- function method is very simple but its results are very cumbersome (see [7] the references cited therein). The results of the ( G / G)-epansion method contain more arbitrary constants compared to the results of the Ep- function method. The performance of the ( G / G) epansion method is reliable simple direct concise gives more eact solutions compared to the Epfunction method. Finally the ( G / G) epansion method allows us to solve more complicated nonlinear PEs compared to the Ep- function method. References [] M.J. Ablowitz P.A. Clarkson Solitons nonlinear Evolution Equations Inverse Scattering Transform Cambridge Univ. Press Cambridge 99. [] Z.Y.Bin L.Chao Commu. Theor. Phys. 5(009) [] E.G. Fan Phys.Lett. A 77 (000) - 8. [4] C.A.Gomez Appl. Math.Comput.89 (007) [5] J.H.He X.H.Wu Chaos Solitons Fractals 0 (006) [6] A.K. Kalkanli S.Y. Sakovich T. Yurdusen J. Math.Phys. 44 (00) [7] N.A. Kudryashov N.B. Loguinova Commu. Nonlinear Sci. Numer. Simul. 4 (009) [8] B.Li Y.Zhang Chaos Solitons Fractals 8 (008) [9] M.R.Miura Backlund Transformation Springer-Verlag Berlin 978. [0] C. Rogers W.F. Shadwick Backlund Transformations Academic Press New York 98. [] M.Wang X.Li Chaos Solitons Fractals 4 (005) [] M.L.WangX.Z.Li J.L.Zhang Phys. Lett. A 7 (008) [] M.Wazwaz Appl. Math. Comput.67 (005) [4] M. Wazwaz Appl. Math.Comput. 84 (007) [5] T.Xu J.Li H.Zhang Y.X.Zhang Z.Z.Yao B. Tian Phys. Lett. A 69 (007) [6] Z.Y.Yan H.Q.Zhang Phys. Lett. A 85 (00) [7] E.M.E. Zayed H.A. Zedan K.A. Gepreel Int. J. Nonlinear Sci. Nume.Simul.5 (004) - 4. [8] E.M.E. Zayed S. Al-Joudi AIP Conference Proceeding Amer. Institute of Phys. Vol 68 (009) [9] E.M.E.Zayed J.Appl. Math. Computing 0 (009) [0] S. Zhang T.C. Xia Appl. Math. Comput. 8 (006)
12 Freund Publishing House Ltd. International Journal of Nonlinear Sciences & Numerical Simulation (4):
New Soliton and Periodic Solutions for Nonlinear Wave Equation in Finite Deformation Elastic Rod. 1 Introduction
ISSN 1749-3889 print), 1749-3897 online) International Journal of Nonlinear Science Vol.15013) No.,pp.18-19 New Soliton and Periodic Solutions for Nonlinear Wave Equation in Finite Deformation Elastic
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 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 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 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 περισσότεραEnvelope Periodic Solutions to Coupled Nonlinear Equations
Commun. Theor. Phys. (Beijing, China) 39 (2003) pp. 167 172 c International Academic Publishers Vol. 39, No. 2, February 15, 2003 Envelope Periodic Solutions to Coupled Nonlinear Equations LIU Shi-Da,
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 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 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 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 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 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 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 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 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 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 περισσότεραA summation formula ramified with hypergeometric function and involving recurrence relation
South Asian Journal of Mathematics 017, Vol. 7 ( 1): 1 4 www.sajm-online.com ISSN 51-151 RESEARCH ARTICLE A summation formula ramified with hypergeometric function and involving recurrence relation Salahuddin
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 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 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 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 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 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 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 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 περισσότερα6.1. 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 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 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 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 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 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 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 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 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 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 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 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 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 περισσότεραThe Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points
Applied Mathematical Sciences, Vol. 3, 009, no., 6-66 The Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points A. Neamaty and E. A. Sazgar Department of Mathematics,
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 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 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 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 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 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 περισσότεραIf 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 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 περισσότεραIf 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 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 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 περισσότεραExact Two Waves Solutions with Variable Amplitude to the KdV Equation 1
International Mathematical Forum, Vol. 9, 2014, no. 3, 137-144 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/imf.2014.312238 Exact Two Waves Solutions with Variable Amplitude to the KdV Equation
Διαβάστε περισσότεραTrigonometry 1.TRIGONOMETRIC RATIOS
Trigonometry.TRIGONOMETRIC RATIOS. If a ray OP makes an angle with the positive direction of X-axis then y x i) Sin ii) cos r r iii) tan x y (x 0) iv) cot y x (y 0) y P v) sec x r (x 0) vi) cosec y r (y
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 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 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 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 περισσότεραDiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation
DiracDelta Notations Traditional name Dirac delta function Traditional notation x Mathematica StandardForm notation DiracDeltax Primary definition 4.03.02.000.0 x Π lim ε ; x ε0 x 2 2 ε Specific values
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 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 περισσότεραMock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =
Mock Eam 7 Mock Eam 7 Section A. Reference: HKDSE Math M 0 Q (a) ( + k) n nn ( )( k) + nk ( ) + + nn ( ) k + nk + + + A nk... () nn ( ) k... () From (), k...() n Substituting () into (), nn ( ) n 76n 76n
Διαβάστε περισσότεραLanczos and biorthogonalization methods for eigenvalues and eigenvectors of matrices
Lanzos and iorthogonalization methods for eigenvalues and eigenvetors of matries rolem formulation Many prolems are redued to solving the following system: x x where is an unknown numer А a matrix n n
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 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 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 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 περισσότεραNew Exact Solutions of Two Nonlinear Physical Models
Commun. Theor. Phys. Beijing China 53 00 pp. 596 60 c Chinese Physical Society and IOP Publishing Ltd Vol. 53 No. April 5 00 New Exact Solutions of Two Nonlinear Physical Models M.M. Hassan Mathematics
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 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 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 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 περισσότερα(, ) (SEM) [4] ,,,, , Legendre. [6] Gauss-Lobatto-Legendre (GLL) Legendre. Dubiner ,,,, (TSEM) Vol. 34 No. 4 Dec. 2017
34 4 17 1 JOURNAL OF SHANGHAI POLYTECHNIC UNIVERSITY Vol. 34 No. 4 Dec. 17 : 11-4543(174-83-8 DOI: 1.1957/j.cnki.jsspu.17.4.6 (, 19 :,,,,,, : ; ; ; ; ; : O 41.8 : A, [1],,,,, Jung [] Legendre, [3] Chebyshev
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 περισσότεραLecture 26: Circular domains
Introductory lecture notes on Partial Differential Equations - c Anthony Peirce. Not to be copied, used, or revised without eplicit written permission from the copyright owner. 1 Lecture 6: Circular domains
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 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 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 περισσότεραEQUATIONS OF DEGREE 3 AND 4.
EQUATIONS OF DEGREE AND 4. IAN KIMING Consider the equation. Equations of degree. x + ax 2 + bx + c = 0, with a, b, c R. Substituting y := x + a, we find for y an equation of the form: ( ) y + py + 2q
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 περισσότεραCommutative Monoids in Intuitionistic Fuzzy Sets
Commutative Monoids in Intuitionistic Fuzzy Sets S K Mala #1, Dr. MM Shanmugapriya *2 1 PhD Scholar in Mathematics, Karpagam University, Coimbatore, Tamilnadu- 641021 Assistant Professor of Mathematics,
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 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 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 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 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 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 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 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 περισσότεραFirst-order Second-degree Equations Related with Painlevé Equations
( Will be set by the publisher ) ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol. xx (2008) No. xx, pp. xxx-xxx First-order Second-degree Equations Related with
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 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 περισσότεραSpace Physics (I) [AP-3044] Lecture 1 by Ling-Hsiao Lyu Oct Lecture 1. Dipole Magnetic Field and Equations of Magnetic Field Lines
Space Physics (I) [AP-344] Lectue by Ling-Hsiao Lyu Oct. 2 Lectue. Dipole Magnetic Field and Equations of Magnetic Field Lines.. Dipole Magnetic Field Since = we can define = A (.) whee A is called the
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 περισσότεραES440/ES911: CFD. Chapter 5. Solution of Linear Equation Systems
ES440/ES911: CFD Chapter 5. Solution of Linear Equation Systems Dr Yongmann M. Chung http://www.eng.warwick.ac.uk/staff/ymc/es440.html Y.M.Chung@warwick.ac.uk School of Engineering & Centre for Scientific
Διαβάστε περισσότεραMath 5440 Problem Set 4 Solutions
Math 544 Math 544 Problem Set 4 Solutions Aaron Fogelson Fall, 5 : (Logan,.8 # 4) Find all radial solutions of the two-dimensional Laplace s equation. That is, find all solutions of the form u(r) where
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 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 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 περισσότεραThe k-α-exponential Function
Int Journal of Math Analysis, Vol 7, 213, no 11, 535-542 The --Exponential Function Luciano L Luque and Rubén A Cerutti Faculty of Exact Sciences National University of Nordeste Av Libertad 554 34 Corrientes,
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 περισσότερα