Branch Points and Branch Cuts

Slides:



Advertisements
Similar presentations
10.1 Complex Numbers Definition:
Advertisements

More Vectors.
ECE 6341 Spring 2014 Prof. David R. Jackson ECE Dept. Notes 36.
Prof. David R. Jackson ECE Dept. Spring 2014 Notes 29 ECE
Reflection and Mirrors Explain and discuss with diagrams, reflection, absorption, and refraction of light rays. Define and illustrate your understanding.
Prof. D. Wilton ECE Dept. Notes 22 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston. (used by Dr. Jackson,
Applied Electricity and Magnetism
Evaluation of Definite Integrals Via the Residue Theorem
11. Complex Variable Theory
Prof. David R. Jackson ECE Dept. Spring 2014 Notes 30 ECE
PARAMETRIC EQUATIONS AND POLAR COORDINATES 9. Usually, we use Cartesian coordinates, which are directed distances from two perpendicular axes. Here, we.
Objective 1 Interpret graphs. Slide Linear Equations in Two Variables; The Rectangular Coordinate System.
Prof. David R. Jackson Dept. of ECE Fall 2013 Notes 19 ECE 6340 Intermediate EM Waves 1.
Applied Electricity and Magnetism
Prof. David R. Jackson Dept. of ECE Fall 2013 Notes 17 ECE 6340 Intermediate EM Waves 1.
Prof. David R. Jackson Dept. of ECE Fall 2013 Notes 13 ECE 6340 Intermediate EM Waves 1.
Notes 13 ECE Microwave Engineering
Prof. David R. Jackson ECE Dept. Spring 2014 Notes 34 ECE
Notes 8 ECE Microwave Engineering Waveguides Part 5:
Prof. David R. Jackson ECE Dept. Spring 2014 Notes 33 ECE
D. R. Wilton ECE Dept. ECE 6382 Functions of a Complex Variable as Mappings 8/24/10.
Notes 11 ECE 2317 Applied Electricity and Magnetism Prof. D. Wilton
1 Spring 2011 Notes 20 ECE 6345 Prof. David R. Jackson ECE Dept.
Polar Coordinates Packet 1. Polar Coordinates  Recording the position of an object using the distance from a fixed point and an angle made from that.
Prof. David R. Jackson Dept. of ECE Notes 2 ECE Microwave Engineering Fall 2011 Smith Charts 1.
Prof. David R. Jackson ECE Dept. Spring 2014 Notes 32 ECE
1. Interpret graphs. 2. Write a solution as an ordered pair. 3. Decide whether a given ordered pair is a solution of a given equation. 4. Complete ordered.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 11 ECE 2317 Applied Electricity and Magnetism 1.
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 14 ECE 3318 Applied Electricity and Magnetism 1.
ECE 6382 Functions of a Complex Variable as Mappings David R. Jackson Notes are adapted from D. R. Wilton, Dept. of ECE 1.
Series Solutions of SOLDEs with Regular Singular Points ECE 6382 Notes are from D. R. Wilton, Dept. of ECE David R. Jackson 1.
Prof. David R. Jackson Dept. of ECE Fall 2015 Notes 22 ECE 6340 Intermediate EM Waves 1.
Prof. David R. Jackson Dept. of ECE Notes 2 ECE Microwave Engineering Fall 2015 Smith Charts 1.
The Steepest-Descent Method
Notes 19 ECE Microwave Engineering
Notes 16 ECE Microwave Engineering Fall 2015 Impedance Matching Prof. David R. Jackson Dept. of ECE 1.
Prof. David R. Jackson Dept. of ECE Notes 8 ECE Microwave Engineering Fall 2015 Waveguides Part 5: Transverse Equivalent Network (TEN) 1.
Power Series Representations ECE 6382 Notes are from D. R. Wilton, Dept. of ECE David R. Jackson 1.
Prof. David R. Jackson Dept. of ECE Fall 2015 Notes 3 ECE 6340 Intermediate EM Waves 1.
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 20 ECE
Evaluation of Definite Integrals via the Residue Theorem
ECE 6382 Integration in the Complex Plane David R. Jackson Notes are from D. R. Wilton, Dept. of ECE 1.
1 Asymptotic Series ECE 6382 David R. Jackson. Asymptotic Series 2 An asymptotic series (as z   ) is of the form Note the “asymptotically equal to”
Spring 2016 Notes 1 ECE 6341 Prof. David R. Jackson ECE Dept. 1.
Branch Points and Branch Cuts
Prof. David R. Jackson ECE Dept. Spring 2016 Notes 42 ECE 6341 Notes 43 1.
ECE 6382 Notes 3 Integration in the Complex Plane Fall 2016
Evaluation of Definite Integrals via the Residue Theorem
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 15.
ECE 6382 Notes 6 Power Series Representations Fall 2016
Applied Electricity and Magnetism
ECE 6345 Spring 2015 Prof. David R. Jackson ECE Dept. Notes 20.
The Steepest-Descent Method
Applied Electricity and Magnetism
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 33.
Notes 17 ECE 6340 Intermediate EM Waves Fall 2016
ECE 6382 Notes 2 Differentiation of Functions of a Complex Variable
Parallel Lines Discovery Activity
Notes 42 Notes 46 ECE 6341 Spring 2016 Prof. David R. Jackson
Parallel Lines Discovery Activity
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 42.
Objectives: After completing this module, you should be able to:
Chapter 34A - Reflection and Mirrors (Geometrical)
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 38.
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 32.
Notes 11 ECE 3318 Applied Electricity and Magnetism Gauss’s Law II
Homework: Study for Unit Test & Complete Test Prep Packet Learning Target: I can demonstrate how transformations and angle relationships impact geometric.
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 11.
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 34.
Reflection and Mirrors (Geometrical)
Presentation transcript:

Branch Points and Branch Cuts ECE 6382 Courtesy of Prof. David R. Jackson ECE Dept. Branch Points and Branch Cuts 8/24/10

Preliminary Consider Choose There are two possible values.

Branch Cuts and Points r = 1 The concept is illustrated for Consider what happens if we encircle the origin: r = 1

Branch Cuts and Points (cont.) We don’t get back the same result!

Branch Cuts and Points (cont.) Now consider encircling the origin twice: r = 1 r We now get back the same result! Hence the square-root function is a double-valued function.

Branch Cuts and Points (cont.) Now consider encircling a point z0 not at the origin Unlike encircling the origin, now we return to the same result! Only the point at the origin must be encircled twice to return to the starting value.

Branch Cuts and Points (cont.) The origin is called a branch point: we are not allowed to encircle it if we wish to make the square-root function single-valued. In order to make the square-root function single-valued, we insert a “barrier” or “branch cut”. branch cut Here the branch cut is chosen to lie on the negative real axis (an arbitrary choice)

Branch Cuts and Points (cont.) We must now choose what “branch” of the function we want. branch cut

Branch Cuts and Points (cont.) Here is the other branch choice. branch cut

Branch Cuts and Points (cont.) Note that the function is discontinuous across the branch cut. branch cut

Branch Cuts and Points (cont.) The shape of the branch cut is arbitrary. branch cut

Branch Cuts and Points (cont.) The branch cut does not even have to be a straight line In this case the branch is determined by requiring that the square-root function change continuously as we start from a specified value (e.g., z = 1). branch cut

Branch Cuts and Points (cont.) Branch points appear in pairs; here one is at z=0 and the other at z= ∞ as determined by examining ζ = 1/ z at ζ=0 Hence the branch cut for the square-root function connects the origin and the point at infinity

Branch Cuts and Points (cont.) Consider this function: What do the branch points and branch cuts look like for this function?

Branch Cuts and Points (cont.) There are two branch cuts: we are not allowed to encircle either branch point.

Branch Cuts and Points (cont.) Geometric interpretation

Branch Cuts and Points (cont.) We can rotate both branch cuts to the real axis.

Branch Cuts and Points (cont.) The two branch cuts “cancel” Note that the function is the same at the two points shown.

Branch Cuts and Points (cont.) Note: we are allowed to encircle both branch points, but not only one of them! An alternative branch cut

Branch Cuts and Points (cont.) 1 2 3 4 5 6 7 Suppose we agree that at point 1, 1 = 2 = 0. This should uniquely determine the branch of the function everywhere in the complex plane. Find the angles 1 and 2 at the other points labeled.

Branch Cuts and Points (cont.) 1 2 3 4 5 6 7

Riemann Surface A Riemann surface is a surface that combines the different sheets of a multi-valued function. It is useful since it displays all possible values of the function at one time.

Riemann Surface (cont.) The concept of the Riemann surface is illustrated for The Riemann surface is really two complex planes connected together. The function z½ is analytic everywhere on this surface (there are no branch cuts). It also assumes all possible values on the surface. Consider this choice: Top sheet: Bottom sheet:

Riemann Surface (cont.) top bottom top view side view

Riemann Surface (cont.) bottom sheet top sheet branch cut branch point

Riemann Surface (cont.) connection between sheets

Riemann Surface (cont.) escalator There are two “escalators” that now connect the top and bottom sheets of the surface.

Riemann Surface (cont.) top sheet: Define by 1 = 2 = 0 on real axis for x > 1 bottom sheet The angle 1 has changed by 2 as we go back to the point z = 2.

Other Multiple-Branch Functions three sheets five sheets infinite number of sheets infinite number of sheets The power is an irrational number.