MCS 351 ENGINEERING MATHEMATICS SOLUTION OF ...
MCS 351 ENGINEERING MATHEMATICS SOLUTION OF ... MCS 351 ENGINEERING MATHEMATICS SOLUTION OF ...
∂u ∂θ = ∂u ∂x .∂x ∂θ + ∂u ∂y .∂y ∂θ = u x(−r sin θ) + u y (r cos θ) = −rv y sin θ − rv x cos θ 12-21 Harmonic functions: 12. u = xy ∂v ∂r = ∂v ∂x .∂x ∂r + ∂v ∂y .∂y ∂r = v x cos θ + v y sin θ ∂v ∂θ = ∂v ∂x .∂x ∂θ + ∂v ∂y .∂y ∂θ = v x(−r sin θ) + v y (r cos θ) =⇒ u r = 1 r v θ and v r = − 1 r u θ. u xx = 0 and u yy = 0 =⇒ u xx + u yy = 0 =⇒ u is harmonic. u x = v y =⇒ y = v y =⇒ v = y2 2 + h(x) =⇒ v x = dh dx u y = −v x =⇒ x = − dh x2 y2 dx =⇒ h(x) = − 2 + c =⇒ f(z) = xy + ( 2 − x2 2 + c)i. 13. v = xy v xx = 0, v yy = 0 =⇒ v xx + v yy = 0 =⇒ v is harmonic. v x = −u y =⇒ u y = −y =⇒ u = − y2 2 + h(x) =⇒ u x = dh dx . Since u x = v y = x, dh x2 dx = x =⇒ h(x) = 2 + c. =⇒ f(z) = − y2 2 + x2 2 + c + xyi. 14. v = − y x 2 +y 2 −u y = v x = 2xy , u (x 2 +y 2 ) 2 x = v y = y2 −x 2 (x 2 +y 2 ) 2 =⇒ v xx = −6x2 y+2y 3 (x 2 +y 2 ) 3 and v yy = 6x2 y−2y 3 (x 2 +y 2 ) 3 =⇒ v xx + v yy = 0 =⇒ v is harmonic. u = x x 2 +y 2 + c =⇒ f(z) = 15. u = ln |z| = ln √ x 2 + y 2 v y = u x = x 2(x 2 +y 2 ) , −v x = u y = x x 2 +y 2 + c + i y 2(x 2 +y 2 ) −y . x 2 +y 2 =⇒ u xx = y2 −x 2 2(x 2 +y 2 ) 2 and u yy = x2 −y 2 2(x 2 +y 2 ) 2 =⇒ u xx + u yy = 0 =⇒ u is harmonic. v = 1 2 arctan( y x ) + h(x) =⇒ v x = − =⇒ f(z) = ln |z| + 1 2 arctan( y x ) + c. 16. v = ln |z| = ln √ x 2 + y 2 −u y = v x = x 2(x 2 +y 2 ) , u x = v y = y 2(x 2 +y 2 ) + dh dx y 2(x 2 +y 2 ) dh =⇒ dx = 0 =⇒ h(x) = c. =⇒ v xx = y2 −x 2 2(x 2 +y 2 ) 2 and v yy = x2 −y 2 2(x 2 +y 2 ) 2 =⇒ v xx + v yy = 0 =⇒ v is harmonic. u = −1 2 arctan( y x ) + h(x) =⇒ u x = =⇒ f(z) = −1 2 arctan( y x ) + c + i ln |z|. 17. u = x 3 − 3xy 2 v y = u x = 3x 2 − 3y 2 , −v x = u y = −6xy y 2(x 2 +y 2 ) + dh dx =⇒ h(x) = c. =⇒ u xx = 6x and u yy = −6x =⇒ u xx + u yy = 0 =⇒ u is harmonic. v = 3x 2 y − y 3 + h(x) =⇒ v x = 6xy + dh dx =⇒ h(x) = c. 15
=⇒ f(z) = x 3 − 3xy 2 + i(3x 2 y − y 3 + c). 18. u = 1 x 2 +y 2 u x = − 2x , u (x 2 +y 2 ) 2 y = −2y (x 2 +y 2 ) 2 =⇒ u xx = 6x2 −2y 2 (x 2 +y 2 ) 3 and u yy = 6y2 −2x 2 (x 2 +y 2 ) 3 =⇒ u xx + u yy ≠ 0 =⇒ u isn’t harmonic. 19. v = (x 2 − y 2 ) 2 −u y = v x = 4x 3 − 4xy 2 , u x = v y = −4x 2 y + 4y 3 =⇒ v xx = 12x 2 −4y 2 and v yy = −4x 2 +12y 2 =⇒ When x, y ≠ 0v xx +v yy ≠ 0 =⇒ v isn’t harmonic. 20. u = cos x cosh y v y = u x = − sin x cosh y, −v x = u y = cos x sinh y =⇒ u xx = − cos x cosh y and u yy = cos x cosh y =⇒ u xx + u yy = 0 =⇒ u is harmonic. v = − sin x sinh y + h(x) =⇒ v x = − cos x sinh y + dh dx =⇒ h(x) = c. =⇒ f(z) = cos x cosh y − i sin x sinh y + c. 21. u = e −x sin 2y u x = −e −x sin 2y, u y = 2e −x cos 2y =⇒ u xx = e −x sin 2y and u yy = −4e −x sin 2y =⇒ When y ≠ kπ, u xx + u yy = −3e −x sin 2y ≠ 0 =⇒ u isn’t harmonic. 22-24 Harmonic conjugate: 22. u = e 3x cos ay harmonic =⇒ u xx + u yy = 0. u x = 3e 3x cos ay, u y = −ae 3x sin ay =⇒ u xx = 9e 3x cos ay and u yy = −a 2 e 3x cos ay =⇒ u xx +u yy = e 3x cos ay(9−a 2 ) = 0 =⇒ a = ∓3 When a = −3, u = e 3x cos(−3y) v y = u x = 3e 3x cos(−3y), −v x = u y = 3e 3x sin(−3y) =⇒ v = −e 3x sin(−3y) + h(x) =⇒ v x = −3e 3x sin(−3y) + dh dx =⇒ h(x) = c. =⇒ v = −e 3x sin(−3y) + c. When a = 3, u = e 3x cos(3y) v y = u x = 3e 3x cos(3y), −v x = u y = −3e 3x sin(3y) =⇒ v = e 3x sin(3y) + h(x) =⇒ v x = 3e 3x sin(3y) + dh dx =⇒ h(x) = c. v = e 3x sin(3y) + c 23. u = sin x cosh(cy) harmonic =⇒ u xx + u yy = 0. u x = cos x cosh(cy), u y = c sin x sinh(cy) =⇒ u xx = −sinx cosh(cy) and u yy = c 2 sin x cosh(cy) and u xx + u yy = 0 =⇒ c 2 − 1 = 0 =⇒ c = ∓1 When c = −1, u = sin x cosh(−y) 16
- Page 1 and 2: MCS 351 ENGINEERING MATHEMATICS SOL
- Page 3 and 4: a + b = 90 ◦ 3. z 1 = x 1 + iy 1
- Page 5 and 6: the fact that tan θ = π 2 , θ =
- Page 7 and 8: For this reason, tan α = 0 and so
- Page 9 and 10: k = 2 =⇒ z 2 = 3√ 5(cos(θ + 4
- Page 11 and 12: 4. Let’s now determine the region
- Page 13 and 14: 12-15 Function values: 12. For z =
- Page 15: 13.4 1-10 Cauchy-Riemann equations:
- Page 19 and 20: 13-17 Polar form: 13. z = √ i ⇒
- Page 21 and 22: then, cosh(z 1 + z 2 ) = cos(i(z 1
- Page 23 and 24: Then we obtain that e 2z + 1 = 0
- Page 25 and 26: ⇒ e x . cos y = − cos(1) and e
- Page 27 and 28: 4. z(t) = 1 + i + e −πit , 0 ≤
- Page 29 and 30: • t = 0 ⇒ z(0) = 0 • t = 2
- Page 31 and 32: • x = −1 ⇒ y = 4 − 4 = 0
- Page 33 and 34: f(z) = e 2z is analytic in C. So we
- Page 35 and 36: 27. z(t) = ( π 4 − t) + ti, (0
- Page 37 and 38: z 2 + 4 = 0 =⇒ z 2 = −4 =⇒ z
- Page 39 and 40: İf z = x + iy, dz = dx + idy = idy
- Page 41 and 42: Let D be the union of C and the int
- Page 43 and 44: Let g(z) = ln(z−1) z−5 . Singul
- Page 45 and 46: Hence we see that when k ∈ {0, 1,
- Page 47 and 48: Because lim n→∞ 1 √ n 2 + 1 =
- Page 49 and 50: 15.4 1-3 Taylor and Maclaurin serie
- Page 51: ∞∑ 11. Let n=1 (−1) n 2 n n z
∂u<br />
∂θ = ∂u<br />
∂x .∂x ∂θ + ∂u<br />
∂y .∂y ∂θ = u x(−r sin θ) + u y (r cos θ) = −rv y sin θ − rv x cos θ<br />
12-21 Harmonic functions:<br />
12. u = xy<br />
∂v<br />
∂r = ∂v<br />
∂x .∂x ∂r + ∂v<br />
∂y .∂y ∂r = v x cos θ + v y sin θ<br />
∂v<br />
∂θ = ∂v<br />
∂x .∂x ∂θ + ∂v<br />
∂y .∂y ∂θ = v x(−r sin θ) + v y (r cos θ)<br />
=⇒ u r = 1 r v θ and v r = − 1 r u θ.<br />
u xx = 0 and u yy = 0 =⇒ u xx + u yy = 0 =⇒ u is harmonic.<br />
u x = v y =⇒ y = v y =⇒ v = y2<br />
2 + h(x) =⇒ v x = dh<br />
dx<br />
u y = −v x =⇒ x = − dh<br />
x2<br />
y2<br />
dx<br />
=⇒ h(x) = −<br />
2<br />
+ c =⇒ f(z) = xy + (<br />
2 − x2<br />
2 + c)i.<br />
13. v = xy<br />
v xx = 0, v yy = 0 =⇒ v xx + v yy = 0 =⇒ v is harmonic.<br />
v x = −u y =⇒ u y = −y =⇒ u = − y2<br />
2 + h(x) =⇒ u x = dh<br />
dx .<br />
Since u x = v y = x, dh<br />
x2<br />
dx<br />
= x =⇒ h(x) =<br />
2 + c.<br />
=⇒ f(z) = − y2<br />
2 + x2<br />
2 + c + xyi.<br />
14. v = − y<br />
x 2 +y 2<br />
−u y = v x =<br />
2xy , u<br />
(x 2 +y 2 ) 2 x = v y = y2 −x 2<br />
(x 2 +y 2 ) 2<br />
=⇒ v xx = −6x2 y+2y 3<br />
(x 2 +y 2 ) 3 and v yy = 6x2 y−2y 3<br />
(x 2 +y 2 ) 3 =⇒ v xx + v yy = 0 =⇒ v is harmonic.<br />
u =<br />
x<br />
x 2 +y 2 + c =⇒ f(z) =<br />
15. u = ln |z| = ln √ x 2 + y 2<br />
v y = u x =<br />
x<br />
2(x 2 +y 2 ) , −v x = u y =<br />
x<br />
x 2 +y 2 + c + i<br />
y<br />
2(x 2 +y 2 )<br />
−y<br />
.<br />
x 2 +y 2<br />
=⇒ u xx = y2 −x 2<br />
2(x 2 +y 2 ) 2 and u yy = x2 −y 2<br />
2(x 2 +y 2 ) 2 =⇒ u xx + u yy = 0 =⇒ u is harmonic.<br />
v = 1 2 arctan( y x ) + h(x) =⇒ v x = −<br />
=⇒ f(z) = ln |z| + 1 2 arctan( y x ) + c.<br />
16. v = ln |z| = ln √ x 2 + y 2<br />
−u y = v x =<br />
x<br />
2(x 2 +y 2 ) , u x = v y =<br />
y<br />
2(x 2 +y 2 ) + dh<br />
dx<br />
y<br />
2(x 2 +y 2 )<br />
dh<br />
=⇒<br />
dx<br />
= 0 =⇒ h(x) = c.<br />
=⇒ v xx = y2 −x 2<br />
2(x 2 +y 2 ) 2 and v yy = x2 −y 2<br />
2(x 2 +y 2 ) 2 =⇒ v xx + v yy = 0 =⇒ v is harmonic.<br />
u = −1<br />
2 arctan( y x ) + h(x) =⇒ u x =<br />
=⇒ f(z) = −1<br />
2 arctan( y x<br />
) + c + i ln |z|.<br />
17. u = x 3 − 3xy 2<br />
v y = u x = 3x 2 − 3y 2 , −v x = u y = −6xy<br />
y<br />
2(x 2 +y 2 ) + dh<br />
dx<br />
=⇒ h(x) = c.<br />
=⇒ u xx = 6x and u yy = −6x =⇒ u xx + u yy = 0 =⇒ u is harmonic.<br />
v = 3x 2 y − y 3 + h(x) =⇒ v x = 6xy + dh<br />
dx<br />
=⇒ h(x) = c.<br />
15