Complex Analysis

📐Complex Analysis Unit 2 – Complex Functions and Mappings

Complex functions and mappings form the foundation of complex analysis, bridging real and imaginary numbers. This unit explores how these functions behave in the complex plane, introducing key concepts like analyticity, conformal mappings, and singularities. Students learn to visualize complex functions as transformations between planes, applying techniques like the Cauchy-Riemann equations. The unit also covers practical applications in physics, engineering, and mathematics, demonstrating the power of complex analysis in solving real-world problems.

Key Concepts and Definitions

  • Complex numbers consist of a real part and an imaginary part, denoted as z=a+biz = a + bi, where aa and bb are real numbers and ii is the imaginary unit (i2=1i^2 = -1)
  • The complex plane is a 2D representation of complex numbers, with the real part on the horizontal axis and the imaginary part on the vertical axis
    • Each point in the complex plane corresponds to a unique complex number
    • The distance from the origin to a point zz is called the modulus or absolute value of zz, denoted as z|z|
  • Complex functions map complex numbers from one complex plane (the domain) to another complex plane (the codomain)
    • A complex function f(z)f(z) can be written as f(z)=u(x,y)+iv(x,y)f(z) = u(x, y) + iv(x, y), where uu and vv are real-valued functions and z=x+iyz = x + iy
  • Limit of a complex function f(z)f(z) as zz approaches a point z0z_0 is defined as limzz0f(z)=L\lim_{z \to z_0} f(z) = L if, for any ε>0\varepsilon > 0, there exists a δ>0\delta > 0 such that f(z)L<ε|f(z) - L| < \varepsilon whenever 0<zz0<δ0 < |z - z_0| < \delta
  • Continuity of a complex function f(z)f(z) at a point z0z_0 means that limzz0f(z)=f(z0)\lim_{z \to z_0} f(z) = f(z_0)
  • Differentiability of a complex function f(z)f(z) at a point z0z_0 means that the limit limh0f(z0+h)f(z0)h\lim_{h \to 0} \frac{f(z_0 + h) - f(z_0)}{h} exists, and this limit is called the derivative of ff at z0z_0, denoted as f(z0)f'(z_0)

Complex Functions and Their Properties

  • Complex functions can be represented by power series, such as the exponential function ez=n=0znn!e^z = \sum_{n=0}^{\infty} \frac{z^n}{n!} and the logarithmic function log(1+z)=n=1(1)n+1znn\log(1 + z) = \sum_{n=1}^{\infty} (-1)^{n+1} \frac{z^n}{n}
  • The composition of two complex functions f(z)f(z) and g(z)g(z) is defined as (fg)(z)=f(g(z))(f \circ g)(z) = f(g(z))
  • The inverse of a complex function f(z)f(z), denoted as f1(z)f^{-1}(z), satisfies f(f1(z))=f1(f(z))=zf(f^{-1}(z)) = f^{-1}(f(z)) = z
    • Not all complex functions have an inverse, and the existence of an inverse depends on the function being one-to-one (injective)
  • Complex functions can be even, satisfying f(z)=f(z)f(-z) = f(z) (cosine function), or odd, satisfying f(z)=f(z)f(-z) = -f(z) (sine function)
  • Periodic complex functions satisfy f(z+p)=f(z)f(z + p) = f(z) for some non-zero complex number pp, called the period (exponential function with imaginary argument)
  • Bounded complex functions have an upper limit on their absolute value, i.e., there exists an M>0M > 0 such that f(z)M|f(z)| \leq M for all zz in the domain (constant functions)

Analytic Functions and Cauchy-Riemann Equations

  • Analytic functions are complex functions that are differentiable at every point in their domain
    • Analyticity is a stronger condition than differentiability, as it requires the function to be differentiable in a neighborhood of each point
  • For a complex function f(z)=u(x,y)+iv(x,y)f(z) = u(x, y) + iv(x, y) to be analytic, it must satisfy the Cauchy-Riemann equations:
    • ux=vy\frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} and uy=vx\frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x}
    • These equations establish a relationship between the real and imaginary parts of an analytic function
  • Harmonic functions are real-valued functions that satisfy Laplace's equation 2ux2+2uy2=0\frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0
    • The real and imaginary parts of an analytic function are harmonic functions
  • Entire functions are analytic functions that are defined and analytic on the whole complex plane (exponential function, polynomials)
  • Meromorphic functions are analytic functions except at a set of isolated points, called poles, where they have singularities (rational functions)
  • The Cauchy-Riemann equations can be used to find the analytic continuation of a complex function defined on a limited domain to a larger domain

Mapping Techniques and Transformations

  • Complex functions can be visualized as mappings between two complex planes, transforming shapes and regions from the domain to the codomain
  • Linear transformations of the form f(z)=az+bf(z) = az + b, where a,bCa, b \in \mathbb{C} and a0a \neq 0, represent rotation, scaling, and translation in the complex plane
    • The multiplication by aa rotates and scales the plane, while the addition of bb translates the plane
  • Möbius transformations, also known as linear fractional transformations, are of the form f(z)=az+bcz+df(z) = \frac{az + b}{cz + d}, where a,b,c,dCa, b, c, d \in \mathbb{C} and adbc0ad - bc \neq 0
    • Möbius transformations map circles and lines to circles and lines, preserving angles (conformal mappings)
    • They are used in modeling physical systems and solving problems in geometry and physics
  • The exponential function eze^z maps horizontal lines to circles centered at the origin and vertical lines to radial lines emanating from the origin
  • The logarithmic function log(z)\log(z) maps the right half-plane to horizontal strips and the unit circle to the imaginary axis
  • The power function znz^n maps the complex plane to itself, wrapping it around the origin nn times
    • For fractional powers, the function is multi-valued, requiring branch cuts to maintain single-valuedness

Conformal Mappings and Applications

  • Conformal mappings are complex functions that preserve angles between curves at each point
    • Analytic functions with non-zero derivatives are conformal mappings
  • Conformal mappings have many applications in physics and engineering, such as:
    • Fluid dynamics: Mapping the flow around objects to simpler geometries
    • Electrostatics: Mapping the electric field around conductors to simpler geometries
    • Heat transfer: Mapping the temperature distribution in irregular shapes to simpler geometries
  • The Joukowsky transformation, given by f(z)=12(z+1z)f(z) = \frac{1}{2}(z + \frac{1}{z}), maps circles to airfoil shapes, which is useful in aerodynamics
  • The Schwarz-Christoffel transformation maps the upper half-plane to polygonal regions, which is useful in solving boundary value problems
  • Conformal mappings can be used to solve Laplace's equation in two dimensions by mapping the problem domain to a simpler domain where the solution is known
    • The solution in the original domain is then obtained by applying the inverse mapping
  • Conformal mappings preserve harmonic functions, meaning that if u(x,y)u(x, y) is harmonic, then u(f(z))u(f(z)) is also harmonic, where f(z)f(z) is a conformal mapping

Singularities and Residues

  • Singularities are points where a complex function is not analytic, and they can be classified into three types:
    • Removable singularities: The limit of the function exists at the point, and the function can be redefined to be analytic there (e.g., f(z)=sin(z)zf(z) = \frac{\sin(z)}{z} at z=0z = 0)
    • Poles: The limit of the function does not exist, but the limit of the product of the function and a power of (zz0)(z - z_0) does exist (e.g., f(z)=1zf(z) = \frac{1}{z} at z=0z = 0)
    • Essential singularities: The limit of the function does not exist, and the function behaves erratically near the point (e.g., f(z)=e1zf(z) = e^{\frac{1}{z}} at z=0z = 0)
  • The residue of a function f(z)f(z) at a pole z0z_0 is the coefficient of the (zz0)1(z - z_0)^{-1} term in the Laurent series expansion of f(z)f(z) around z0z_0
    • For a simple pole, the residue is given by limzz0(zz0)f(z)\lim_{z \to z_0} (z - z_0)f(z)
    • For a pole of order nn, the residue is given by 1(n1)!limzz0dn1dzn1((zz0)nf(z))\frac{1}{(n-1)!} \lim_{z \to z_0} \frac{d^{n-1}}{dz^{n-1}} ((z - z_0)^n f(z))
  • The residue theorem states that the integral of a function f(z)f(z) along a closed contour CC is equal to 2πi2\pi i times the sum of the residues of f(z)f(z) at the poles enclosed by CC
    • This theorem is useful for evaluating integrals of complex functions along closed contours
  • The argument principle relates the number of zeros and poles of a meromorphic function inside a closed contour to the change in the argument of the function along the contour
  • The Mittag-Leffler theorem states that any meromorphic function can be expressed as a sum of its principal part at each pole plus an entire function

Integration in the Complex Plane

  • Integration of complex functions is performed using contour integrals, which are integrals along a curve in the complex plane
    • The contour integral of a function f(z)f(z) along a curve CC is defined as Cf(z)dz\int_C f(z) dz
  • Cauchy's integral theorem states that if f(z)f(z) is analytic in a simply connected domain DD and CC is a closed contour lying entirely in DD, then Cf(z)dz=0\int_C f(z) dz = 0
    • This theorem is the foundation for many important results in complex analysis
  • Cauchy's integral formula states that if f(z)f(z) is analytic in a simply connected domain DD and z0z_0 is a point in DD, then f(z0)=12πiCf(z)zz0dzf(z_0) = \frac{1}{2\pi i} \int_C \frac{f(z)}{z - z_0} dz, where CC is a closed contour enclosing z0z_0
    • This formula allows the calculation of the value of an analytic function at a point using a contour integral
  • The residue theorem can be used to evaluate real integrals by extending the integrand to the complex plane and choosing an appropriate contour
    • This technique is particularly useful for evaluating improper integrals and integrals involving trigonometric or exponential functions
  • The Cauchy principal value of an improper integral is a method for assigning a finite value to an integral that would otherwise be undefined due to a singularity on the path of integration
  • The Jordan curve theorem states that a simple closed curve divides the complex plane into two distinct regions: the interior and the exterior
    • This theorem is important for understanding the behavior of complex functions and their integrals

Practical Applications and Examples

  • Complex analysis has numerous applications in various fields, such as:
    • Physics: Quantum mechanics, electromagnetism, fluid dynamics
    • Engineering: Signal processing, control theory, electrical networks
    • Mathematics: Number theory, algebraic geometry, differential equations
  • The Fourier transform, which is widely used in signal processing, can be viewed as a complex function that maps a time-domain signal to a frequency-domain representation
    • The inverse Fourier transform maps the frequency-domain representation back to the time-domain signal
  • The Laplace transform, used in solving differential equations and analyzing control systems, is a complex function that maps a time-domain function to a complex frequency-domain representation
    • The inverse Laplace transform maps the complex frequency-domain representation back to the time-domain function
  • The Gamma function, which is an extension of the factorial function to complex numbers, has applications in probability theory, combinatorics, and number theory
    • The Gamma function satisfies the functional equation Γ(z+1)=zΓ(z)\Gamma(z+1) = z\Gamma(z) and has poles at the non-positive integers
  • The Riemann zeta function, which is defined as ζ(s)=n=11ns\zeta(s) = \sum_{n=1}^{\infty} \frac{1}{n^s} for (s)>1\Re(s) > 1, has deep connections to prime numbers and the distribution of primes
    • The Riemann hypothesis, which states that the non-trivial zeros of the zeta function have real part equal to 12\frac{1}{2}, is one of the most important unsolved problems in mathematics
  • Conformal mappings are used in the design of airfoils and other aerodynamic shapes, as they allow the flow around the object to be studied in a simpler geometric setting
    • The Kutta-Joukowski theorem relates the lift generated by an airfoil to the circulation of the flow around it, which can be calculated using complex analysis techniques


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© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.