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C HAPTER 5: L INEAR D IFFERENTIAL E QUATIONS S ECTION 5.3 — C OMPLEX S OLUTIONS Dr. Bisher M. Iqelan [email protected] Department of Mathematics The Islamic University of Gaza 2016-2017, Semester 2 size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 1/10 B ASIC P ROPERTIES OF C OMPLEX NUMBERS FACT 1 A complex number z = a + ib, where a is a real part and b is √ an imaginary part and i = −1. 2 Any real number a is complex since a = a + 0i, so R ⊆ C. 3 z1 = a + ib, z2 = c + id are equal iff a = c, and b = d. 4 A complex function w (x ) = u (x ) + iv (x ) and its derivative w 0 (x ) = u 0 (x ) + iv 0 (x ), for example if: w (x ) = e2x + i ln(2x ), then w 0 (x ) = 2e2x + i x1 . 5 If w (x ) = u (x ) + iv (x ) is a complex solution of the homogeneous DE L[y ] = 0, then both u (x ) and v (x ) are real solutions of the same DE L[y ] = 0. size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 2/10 E ULER ’ S F ORMULA FACT (E ULER ’ S FORMULA : S OME PROPERTIES ) 1 Euler’s formula: The exponential function ei θ is written as ei θ = cos θ + i sin θ . 2 e−i θ = ei (−θ ) = cos(−θ ) + i sin(−θ ) ⇒ e−i θ = cos θ − i sin θ. 3 ex +iy = ex .eiy = ex (cos y + i sin y ) = ex cos y + iex sin y 4 ei π = cos π + i sin π = −1. 5 For any real number b, eibx + e−ibx = cos bx + i sin bx + cos bx − i sin bx i 1 h ibx =2 cos bx ⇒ cos bx = e + e−ibx 2 Similarly, sin bx = 2i1 eibx − e−ibx . size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 3/10 n − TH O RDER H OMOGENEOUS DE For the (Hc) DE, 0 a0 y (n) + a1 y (n−1) + · · · + an−1 y + an y = 0 (Hc) The auxiliary (characteristic) polynomial of the DE (Hc) is a0 r n + a1 r n−1 + · · · + an−1 r + an = 0 (ChP) If the roots of (Hc) are complex, then every pair are conjugate, that is, if r1 = α + i β then r2 = α − i β. size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 4/10 p (D ) H AS T WO C ONJUGATE C OMPLEX R OOTS α ± i β Suppose p (D ) has two conjugate complex roots r1 = α + i β, r2 = α − i β, α, β ∈ R If we slightly extend our discussion to complex-valued DE, it is not hard to see that the previous method works again and we get a general (complex-valued) solution y = c1 er1 x + c2 er2 x c1 , c2 ∈ C Still we need to get back to the real domain ... So, lets do some further manipulation by using the fact that ei θ = cos θ + i sin θ size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 5/10 p (D ) H AS T WO C ONJUGATE C OMPLEX R OOTS α ± i β The general solution to Ly = 0 where L = p (D ) is y =C1 e(α+i β)x + C2 e(α−i β)x = C1 eαx ei βx + C2 eαx e−i βx =C1 eαx (cos βx + i sin βx ) + C2 eαx (cos βx − i sin βx ) =(C1 + C2 )eαx cos βx + i (C1 − C2 )eαx sin βx To get a real-valued solution, there are two choices: • Pick C1 + C2 = 1, C1 − C2 = 0 : we get y = f1 (x ) = eαx cos βx • Pick C1 + C2 = 0, C1 − C2 = −i : we get y = f2 (x ) = eαx sin βx Since f1 and f2 are linearly independent, the general real-valued solution to Ly = 0 where L = p (D ) is c1 eαx cos βx + c2 eαx sin βx , c1 , c2 ∈ R. size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 6/10 E XAMPLE Find the general solution of the DE (D 2 + 4D + 5)y = 0 Answer: Let y = erx be a solution, then Dy = r erx , D 2 y = r 2 erx The characteristic equation is r 2 + 4r + 5 = 0, solving we have √ −4 ± 2i −4 ± 16 − 4.1.5 = = −2 ± i r= 2 2 The general solution is y = e−2x [c1 cos x + c2 sin x ] size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 7/10 E XAMPLE Find the general solution of the DE (D 5 − 16D )y = 0 Answer: Let y = erx be a solution, then the characteristic equation is r 5 − 16r = 0, solving we have r 5 − 16r = r (r 4 − 16) = 0 ⇒ r (r 2 − 4)(r 2 + 4) = r (r − 2)(r + 2)(r 2 + 4)0 ⇒ r = 0, r = 2, r = −2, r = ±2i The general solution is y = c1 + c2 e2x + c3 e−2x + c4 cos 2x + c5 sin 2x size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 8/10 E XAMPLE Solve the IVP of the DE y 00 + 16y = 0, y (0) = 2, y 0 (0) = −2 Answer: Let y = erx be a solution, then the characteristic equation is r 2 + 16 = 0, solving we have r = ±4i The general solution is y =c1 cos 4x + c2 sin 4x, y (0) = 2 ⇒ c1 = 2 y 0 = − 4c1 sin 4x + 4c2 cos 4x, y 0 ( 0 ) = − 2 ⇒ c2 = − 1 2 Thus the particular solution is y = 2 cos 4x − 1 sin 4x 2 size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 9/10 H OME W ORK S EC .5.3 HW. (E X . S EC .5.3) Solve: Q3 (a, b, c ), Q7 , Q8 . size= Dr. Bisher M. Iqelan Lecture 25: Sec 5.3 — Complex Solutions 10/10