Ejercicio 1Dificultad: BásicoDeterminar si la función f(z)=z4f(z) = z^4f(z)=z4 es analítica y calcular su derivada.Ver solución paso a paso3 pasosPaso 1Expresar la función en términos de xxx e yyyf(z)=(x+iy)4f(z) = (x + iy)^4f(z)=(x+iy)4Desarrollando el binomio:(x+iy)4=x4+4x3(iy)+6x2(iy)2+4x(iy)3+(iy)4(x + iy)^4 = x^4 + 4x^3(iy) + 6x^2(iy)^2 + 4x(iy)^3 + (iy)^4(x+iy)4=x4+4x3(iy)+6x2(iy)2+4x(iy)3+(iy)4=x4+4ix3y−6x2y2−4ixy3+y4= x^4 + 4ix^3y - 6x^2y^2 - 4ixy^3 + y^4=x4+4ix3y−6x2y2−4ixy3+y4=(x4−6x2y2+y4)+i(4x3y−4xy3)= (x^4 - 6x^2y^2 + y^4) + i(4x^3y - 4xy^3)=(x4−6x2y2+y4)+i(4x3y−4xy3)Por tanto: u(x,y)=x4−6x2y2+y4u(x,y) = x^4 - 6x^2y^2 + y^4u(x,y)=x4−6x2y2+y4 y v(x,y)=4x3y−4xy3v(x,y) = 4x^3y - 4xy^3v(x,y)=4x3y−4xy3Paso 2Verificar las condiciones de Cauchy-Riemann∂u∂x=4x3−12xy2\frac{\partial u}{\partial x} = 4x^3 - 12xy^2∂x∂u=4x3−12xy2∂v∂y=4x3−12xy2\frac{\partial v}{\partial y} = 4x^3 - 12xy^2∂y∂v=4x3−12xy2 ✓\checkmark✓∂u∂y=−12x2y+4y3\frac{\partial u}{\partial y} = -12x^2y + 4y^3∂y∂u=−12x2y+4y3∂v∂x=12x2y−4y3\frac{\partial v}{\partial x} = 12x^2y - 4y^3∂x∂v=12x2y−4y3−∂v∂x=−12x2y+4y3-\frac{\partial v}{\partial x} = -12x^2y + 4y^3−∂x∂v=−12x2y+4y3 ✓\checkmark✓Paso 3Calcular la derivadaf′(z)=∂u∂x+i∂v∂x=(4x3−12xy2)+i(12x2y−4y3)f'(z) = \frac{\partial u}{\partial x} + i\frac{\partial v}{\partial x} = (4x^3 - 12xy^2) + i(12x^2y - 4y^3)f′(z)=∂x∂u+i∂x∂v=(4x3−12xy2)+i(12x2y−4y3)=4(x3−3xy2)+4i(3x2y−y3)=4[x3−3xy2+i(3x2y−y3)]= 4(x^3 - 3xy^2) + 4i(3x^2y - y^3) = 4[x^3 - 3xy^2 + i(3x^2y - y^3)]=4(x3−3xy2)+4i(3x2y−y3)=4[x3−3xy2+i(3x2y−y3)]=4[x(x2−3y2)+iy(3x2−y2)]=4z3= 4[x(x^2 - 3y^2) + iy(3x^2 - y^2)] = 4z^3=4[x(x2−3y2)+iy(3x2−y2)]=4z3
Ejercicio 2Dificultad: IntermedioVerificar si la función f(z)=e2zf(z) = e^{2z}f(z)=e2z satisface las condiciones de Cauchy-Riemann y encontrar su derivada.Ver solución paso a paso3 pasosPaso 1Expresar f(z)f(z)f(z) en forma rectangularf(z)=e2(x+iy)=e2x+2iy=e2x(cos(2y)+isin(2y))f(z) = e^{2(x+iy)} = e^{2x+2iy} = e^{2x}(\cos(2y) + i\sin(2y))f(z)=e2(x+iy)=e2x+2iy=e2x(cos(2y)+isin(2y))Por tanto: u(x,y)=e2xcos(2y)u(x,y) = e^{2x}\cos(2y)u(x,y)=e2xcos(2y) y v(x,y)=e2xsin(2y)v(x,y) = e^{2x}\sin(2y)v(x,y)=e2xsin(2y)Paso 2Calcular las derivadas parciales∂u∂x=2e2xcos(2y)\frac{\partial u}{\partial x} = 2e^{2x}\cos(2y)∂x∂u=2e2xcos(2y)∂v∂y=2e2xcos(2y)\frac{\partial v}{\partial y} = 2e^{2x}\cos(2y)∂y∂v=2e2xcos(2y) ✓\checkmark✓∂u∂y=−2e2xsin(2y)\frac{\partial u}{\partial y} = -2e^{2x}\sin(2y)∂y∂u=−2e2xsin(2y)∂v∂x=2e2xsin(2y)\frac{\partial v}{\partial x} = 2e^{2x}\sin(2y)∂x∂v=2e2xsin(2y)−∂v∂x=−2e2xsin(2y)-\frac{\partial v}{\partial x} = -2e^{2x}\sin(2y)−∂x∂v=−2e2xsin(2y) ✓\checkmark✓Paso 3Las condiciones se cumplen en todo C\mathbb{C}C y las derivadas parciales son continuas, por tanto es analítica en todo C\mathbb{C}Cf′(z)=∂u∂x+i∂v∂x=2e2xcos(2y)+i(2e2xsin(2y))f'(z) = \frac{\partial u}{\partial x} + i\frac{\partial v}{\partial x} = 2e^{2x}\cos(2y) + i(2e^{2x}\sin(2y))f′(z)=∂x∂u+i∂x∂v=2e2xcos(2y)+i(2e2xsin(2y))=2e2x(cos(2y)+isin(2y))=2e2xe2iy=2e2(x+iy)=2e2z= 2e^{2x}(\cos(2y) + i\sin(2y)) = 2e^{2x}e^{2iy} = 2e^{2(x+iy)} = 2e^{2z}=2e2x(cos(2y)+isin(2y))=2e2xe2iy=2e2(x+iy)=2e2z
Ejercicio 3Dificultad: AvanzadoAnalizar la diferenciabilidad de la función f(z)=z2zˉf(z) = z^2\bar{z}f(z)=z2zˉ y determinar dónde es analítica.Ver solución paso a paso3 pasosPaso 1Expresar la función en términos de xxx e yyyf(z)=(x+iy)2(x−iy)=(x2−y2+2ixy)(x−iy)f(z) = (x + iy)^2(x - iy) = (x^2 - y^2 + 2ixy)(x - iy)f(z)=(x+iy)2(x−iy)=(x2−y2+2ixy)(x−iy)=(x2−y2)x−(x2−y2)(iy)+2ixy⋅x−2ixy⋅(iy)= (x^2 - y^2)x - (x^2 - y^2)(iy) + 2ixy \cdot x - 2ixy \cdot (iy)=(x2−y2)x−(x2−y2)(iy)+2ixy⋅x−2ixy⋅(iy)=x(x2−y2)−i(x2−y2)y+2ix2y+2xy2= x(x^2 - y^2) - i(x^2 - y^2)y + 2ix^2y + 2xy^2=x(x2−y2)−i(x2−y2)y+2ix2y+2xy2=x3−xy2+2xy2−i(x2−y2)y+2ix2y= x^3 - xy^2 + 2xy^2 - i(x^2 - y^2)y + 2ix^2y=x3−xy2+2xy2−i(x2−y2)y+2ix2y=x3+xy2+i[2x2y−(x2−y2)y]= x^3 + xy^2 + i[2x^2y - (x^2 - y^2)y]=x3+xy2+i[2x2y−(x2−y2)y]=x3+xy2+i(2x2y−x2y+y3)=x3+xy2+i(x2y+y3)= x^3 + xy^2 + i(2x^2y - x^2y + y^3) = x^3 + xy^2 + i(x^2y + y^3)=x3+xy2+i(2x2y−x2y+y3)=x3+xy2+i(x2y+y3)Por tanto: u(x,y)=x3+xy2u(x,y) = x^3 + xy^2u(x,y)=x3+xy2 y v(x,y)=x2y+y3v(x,y) = x^2y + y^3v(x,y)=x2y+y3Paso 2Verificar las condiciones de Cauchy-Riemann∂u∂x=3x2+y2\frac{\partial u}{\partial x} = 3x^2 + y^2∂x∂u=3x2+y2∂v∂y=x2+3y2\frac{\partial v}{\partial y} = x^2 + 3y^2∂y∂v=x2+3y2Para que se cumpla: 3x2+y2=x2+3y2⇒2x2=2y2⇒x2=y23x^2 + y^2 = x^2 + 3y^2 \Rightarrow 2x^2 = 2y^2 \Rightarrow x^2 = y^23x2+y2=x2+3y2⇒2x2=2y2⇒x2=y2∂u∂y=2xy\frac{\partial u}{\partial y} = 2xy∂y∂u=2xy∂v∂x=2xy\frac{\partial v}{\partial x} = 2xy∂x∂v=2xy−∂v∂x=−2xy-\frac{\partial v}{\partial x} = -2xy−∂x∂v=−2xyPara que se cumpla: 2xy=−2xy⇒4xy=0⇒x=02xy = -2xy \Rightarrow 4xy = 0 \Rightarrow x = 02xy=−2xy⇒4xy=0⇒x=0 o y=0y = 0y=0Paso 3Análisis conjuntoLas condiciones se cumplen cuando x2=y2x^2 = y^2x2=y2 Y (x=0(x = 0(x=0 o y=0)y = 0)y=0)Esto ocurre solo en el punto (0,0)(0{,}0)(0,0). Como las derivadas parciales son continuas, la función es diferenciable únicamente en el origen. Como no existe ningún entorno del origen en el que sea diferenciable, fff no es analítica en ningún punto.
Ejercicio 4Dificultad: ExpertoDemostrar que si f(z)=u(x,y)+iv(x,y)f(z) = u(x,y) + iv(x,y)f(z)=u(x,y)+iv(x,y) es analítica en un dominio DDD, entonces las funciones ∣f(z)∣2|f(z)|^2∣f(z)∣2 y Re(f(z))\text{Re}(f(z))Re(f(z)) no son analíticas en DDD (excepto casos triviales).Ver solución paso a paso4 pasosPaso 1Analizar g(z)=∣f(z)∣2=f(z)f(z)‾g(z) = |f(z)|^2 = f(z)\overline{f(z)}g(z)=∣f(z)∣2=f(z)f(z)Si f(z)=u+ivf(z) = u + ivf(z)=u+iv, entonces g(z)=(u+iv)(u−iv)=u2+v2g(z) = (u + iv)(u - iv) = u^2 + v^2g(z)=(u+iv)(u−iv)=u2+v2Para g(z)g(z)g(z): U(x,y)=u2+v2U(x,y) = u^2 + v^2U(x,y)=u2+v2 y V(x,y)=0V(x,y) = 0V(x,y)=0Las condiciones de Cauchy-Riemann son:∂U∂x=∂V∂y=0\frac{\partial U}{\partial x} = \frac{\partial V}{\partial y} = 0∂x∂U=∂y∂V=0∂U∂y=−∂V∂x=0\frac{\partial U}{\partial y} = -\frac{\partial V}{\partial x} = 0∂y∂U=−∂x∂V=0Paso 2Calcular las derivadas de UUU∂U∂x=2u∂u∂x+2v∂v∂x\frac{\partial U}{\partial x} = 2u\frac{\partial u}{\partial x} + 2v\frac{\partial v}{\partial x}∂x∂U=2u∂x∂u+2v∂x∂vComo fff es analítica: ∂u∂x=∂v∂y\frac{\partial u}{\partial x} = \frac{\partial v}{\partial y}∂x∂u=∂y∂v y ∂v∂x=−∂u∂y\frac{\partial v}{\partial x} = -\frac{\partial u}{\partial y}∂x∂v=−∂y∂u∂U∂x=2u∂v∂y+2v(−∂u∂y)=2(u∂v∂y−v∂u∂y)\frac{\partial U}{\partial x} = 2u\frac{\partial v}{\partial y} + 2v(-\frac{\partial u}{\partial y}) = 2(u\frac{\partial v}{\partial y} - v\frac{\partial u}{\partial y})∂x∂U=2u∂y∂v+2v(−∂y∂u)=2(u∂y∂v−v∂y∂u)Para que ∂U∂x=0\frac{\partial U}{\partial x} = 0∂x∂U=0: u∂v∂y=v∂u∂yu\frac{\partial v}{\partial y} = v\frac{\partial u}{\partial y}u∂y∂v=v∂y∂uPaso 3Condición para analiticidadSimilarmente, ∂U∂y=2(u∂u∂y+v∂v∂y)=−2(u∂v∂x−v∂u∂x)=0\frac{\partial U}{\partial y} = 2(u\frac{\partial u}{\partial y} + v\frac{\partial v}{\partial y}) = -2(u\frac{\partial v}{\partial x} - v\frac{\partial u}{\partial x}) = 0∂y∂U=2(u∂y∂u+v∂y∂v)=−2(u∂x∂v−v∂x∂u)=0Esto implica u∂v∂x=v∂u∂xu\frac{\partial v}{\partial x} = v\frac{\partial u}{\partial x}u∂x∂v=v∂x∂uCombinando ambas condiciones y usando Cauchy-Riemann:u∂u∂x+v∂v∂x=0u\frac{\partial u}{\partial x} + v\frac{\partial v}{\partial x} = 0u∂x∂u+v∂x∂v=0 y u∂u∂y+v∂v∂y=0u\frac{\partial u}{\partial y} + v\frac{\partial v}{\partial y} = 0u∂y∂u+v∂y∂v=0Esto significa ∇(u2+v2)=0\nabla(u^2 + v^2) = 0∇(u2+v2)=0, es decir, ∣f(z)∣|f(z)|∣f(z)∣ es constante.Por tanto, ∣f(z)∣2|f(z)|^2∣f(z)∣2 es analítica solo si f(z)f(z)f(z) es constante.Paso 4Analizar h(z)=Re(f(z))=u(x,y)h(z) = \text{Re}(f(z)) = u(x,y)h(z)=Re(f(z))=u(x,y)Para h(z)h(z)h(z): U1(x,y)=u(x,y)U_1(x,y) = u(x,y)U1(x,y)=u(x,y) y V1(x,y)=0V_1(x,y) = 0V1(x,y)=0Las condiciones requieren: ∂u∂x=0\frac{\partial u}{\partial x} = 0∂x∂u=0 y ∂u∂y=0\frac{\partial u}{\partial y} = 0∂y∂u=0Esto implica que uuu es constante, y por las condiciones de Cauchy-Riemann de fff, también vvv es constante.Por tanto, Re(f(z))\text{Re}(f(z))Re(f(z)) es analítica solo si f(z)f(z)f(z) es constante.