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International Refereed Journal of Engineering and Science (IRJES)
ISSN (Online) 2319-183X, (Print) 2319-1821
Volume 2, Issue 2(February 2013), PP.25-29
www.irjes.com

         Schwarz-Christoffel Transformation On A Half Plane
                                      Abdualah Ibrahim Sultan
                    Mathematics Department of Brawijaya University Malang, Indonesia.
                Mathematics Department of, Faculty of Science, Khoms, Al-Mergeb University ,
                                              Khoms, Libya.


ABSTRACT :The Schwarz-Christoffel transformation has been studied by many reseachers due to a huge of
its application in solving Laplace's equations and studying fluid flow phenomenas ( see [3],[4]). The proof of
this theorem can find in (see for example [5]). Their method depend on the tangent of 𝑇𝑗 = 1 + 𝑖0 and the
rotation of     𝑇𝑗 from 0 to 𝜋 on points (𝑥, 0) . In this paper we would like to prove the Shwarz-
Christoffeltransformation directly by using the arguments identity of complex number, rotation of it from 0 to
2𝜋 and conformal mapping.
Keywords : Complex function, half plane, polygon, analytic function, transformation, Conformal mapping.

                                           I.    INTRODUCTION
         The Schwarz-Christoffel transformation known as a map from the upper half-plane to simply
connected polygon with or without corners at infinity in the complex planes.The Schwarz-Christoffel
transformation has been studied by many reseachers due to a huge of its application for example used in
physical applications involving fluid movement, heat conduction and electrostatic pontential, as well asthe
studying of Laplace's equations (see [3],[4]) and also from mathematical point of views ( see [1],[2],[6]).
          In this paper we study about the proof of the Schwarz-Christoffel theorem. The prove of this theorem
can found in (see for example [5]). Their method depend on the tangent of 𝑇𝑗 = 1 + 𝑖0 and the rotation of 𝑇𝑗
from 0 to 𝜋 on points (𝑥, 0). In this paper we would like to prove the Shwarz-Christoffel transformation
directly by using the arguments identity of complex number, rotation of it from 0 to 2𝜋 and conformal
mapping.

                                          II.    PRELIMINARIES
             We need to review some important definitions and theorems which will be used later from complex
analysis to understand the Schwarz-Christoffeltheorem.These definitions and theorems below can be found in
the refences ( see [3], [4] ).
Definition 2.1 A complex number is a number of the form 𝑧 = 𝑎 + 𝑖𝑏 where the imaginary unit is defined as
 𝑖 = −1and𝑎 is the real part of 𝑧, 𝑎 = 𝑅𝑒(𝑧), and 𝑏 is the imaginary part of 𝑧 , 𝑏 = 𝐼𝑚(𝑧). The set of all
complex number is written by 𝐶.
Definition 2.2. Arguments of complex number
Let r and θ be polar coordinates of the point 𝑎, 𝑏 that corresponds to a nonzero complex number 𝑧 = 𝑎 + 𝑖𝑏.
Since 𝑎 = cos 𝜃and 𝑏 = sin 𝜃, the number 𝑧can be written in polar form as 𝑧 = r (cos 𝜃 + 𝑖 sin 𝜃) = 𝑧 𝑒 𝑖𝜃 ,
where 𝑧 is a positive real number called the modulus of 𝑧, and 𝜃 is real number called the argument of 𝑧, and
written by arg 𝑧.The real number𝜃 represents the angle and measured in radians.
Theorem 2.1. Law of arguments of products .
Let 𝑏, 𝑐 ∈ 𝐶. Then
                                          arg 𝑏𝑐 = arg b + arg c.                                         (1.1)
Theorem 2.2. Law of arguments of power
Let 𝑏, 𝑐 ∈ 𝐶. Then
                                                arg 𝑏 𝑐 = 𝑐 arg 𝑏.                                       (1.2)
Definition 2.3.Complex Function. A complex function is a function 𝑓 whose domain and range are subsets of
the set 𝐶 of complex numbers.
Definition 2.4.Conformal mapping. Let 𝑤 = 𝑓 (𝑧) be a complex mapping defined in a domain 𝐷 and let 𝑧0 be
a point in 𝐷. Then we say that 𝑤 = 𝑓 (𝑧) is conformal at 𝑧0 if for every pair of smoothoriented curves𝐶1 and 𝐶2
in 𝐷 intersecting at 𝑧0 the angle between 𝐶1 and 𝐶2 at𝑧0 is equal tothe angle between the image curves 𝐶 ′ 1 and
  𝐶 ′ 2 at 𝑓 (𝑧0 ) in both magnitude and sense.


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Schwarz-Christoffel Transformation On A Half Plane




                                  Figure 1.1 The angle between𝐶1 and 𝐶2 (see [4])

In other words a mapping 𝑤 = 𝑓 (𝑧) preserves both angle and shape but it cannot in general the size. Moreover
a mapping that is conformal at every point in a domain D is called conformal in D, the conformal mapping relies
on the properties of analytic function. The angle between any two intersecting arcs in the z-plane is equal to the
angle between the images of the arcs in the w-plane under a linear mapping.
Definition 2.5. Analytic Function.A function 𝑓 (𝑧) is said to be analytic in a region 𝑅 of the complex plane if
 𝑓 (𝑧) has a derivative at each point of 𝑅. In addition, analytic function is conformal at 𝑧0 if and only if 𝑓 ′ (𝑧) ≠
0.
Definition 2.6.Polygon. A polygon is a plane figure that is bounded by closed path, composed of a finite
sequence of straight-line segments (i.e. a closed polygonal chain or circuit). These segments are called its edges
or sides, and the points where two edges meet are the polygon’s vertices (singular: vertex) or corners.

                                           III.        MAIN THEOREM
Theorem (Schwarz-christoffel)
Let 𝑃 be a polygon in the 𝑤-plane with vertices 𝑤1 , 𝑤2 , … , 𝑤 𝑛 and exterior angles 𝛼 𝑘 , where – 𝜋 < 𝛼 𝑘 <
 𝜋 .There exists a one-to-one conformal mapping 𝑤 = 𝑓 (𝑧) from the upper half plane, 𝐼𝑚 𝑧 > 0 onto 𝐺 that
satisfies the boundary conditions in equations 𝑤 𝑘 = 𝑓 (𝑥 𝑘 ) for 𝑘 = 1,2 … . 𝑛 − 1 and 𝑤 𝑛 = 𝑓 ∞ ,
where 𝑥1 < 𝑥2 < 𝑥3 < ⋯ < 𝑥 𝑛−1 < ∞. Derivative 𝑓 ′ (𝑧) is
                                         − 𝛼1         − 𝛼2                − 𝛼 𝑛 −1                     (1.3)
                       𝑓 ′ 𝑧 = 𝐴 𝑧 − 𝑥1 ) 𝜋    𝑧 − 𝑥2 𝜋 … 𝑧 − 𝑥 𝑛 −1         𝜋



and the function f can be expressed as an indefinite integral
                                                       − 𝛼1             − 𝛼2                  − 𝛼 𝑛 −1          (1.4)
             𝑓 𝑧 = 𝐵 + 𝐴 ∫ 𝑓 ′ 𝑧 = 𝐴 𝑧 − 𝑥1 )            𝜋     𝑧 − 𝑥2     𝜋    … 𝑧 − 𝑥 𝑛 −1      𝜋       𝑑𝑧

where 𝐴 and 𝐵 are suitably chosen constants. Two of the points {𝑥 𝑘 } may be chosen arbitrarily, and the
constants 𝐴 and 𝐵 determine the size and position of 𝑃.

                                     IV.     PROVE OF THE THEOREM

A transformation 𝑤 = 𝑓 𝑧 constructed by mapping each point on the 𝑥 axis in 𝑧 -plane z on 𝑤 -plane,
with 𝑥1 , 𝑥2 , … , 𝑥 𝑛−1 , 𝑥 𝑛 are the points on the 𝑥-axis and 𝑥1 < 𝑥2 < 𝑥3 < ⋯ < 𝑥 𝑛 −1 < 𝑥 𝑛 where the points on the
plane 𝑧 is the domain of the transformation. These points are mapped in to points on the 𝑛-side, is 𝑤𝑗 =
 𝑓(𝑥 𝑗 ), 𝑗 = 1, 2, . . . , 𝑛 -1 and 𝑤 𝑛 = 𝑓 ∞ in
 𝑤-plane. The function 𝑓chosen so that arg 𝑓 ′ 𝑧 different constant value
                                  𝑓 ′ 𝑧 = 𝐴(𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛 −1 )−𝑘 𝑛 −1                     (1.5)

where A is a complex constant and each 𝑘 𝑗 , with 𝑗 = 1, 2, 3, 𝑛 − 1 are real constants.
From equation (1.5) we taking the absolute value, then we have
                                𝑓 ′ 𝑧 = 𝐴(𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛−1 ) 𝑘 𝑛 −1
             −𝑘 1          −𝑘 2
= 𝐴 (𝑧 − 𝑥1 )     (𝑧 − 𝑥2 )        … (𝑧 − 𝑥 𝑛 −1 )−𝑘 𝑛 −1
                                                 𝐴        1             1
                                         =         𝑘1
                                            (𝑧−𝑥 1 )        𝑘2 …
                                                        (𝑧−𝑥 2 )           𝑘 𝑛 −1 ,
                                                                        (𝑧−𝑥 𝑛 −1 )

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Schwarz-Christoffel Transformation On A Half Plane

                                                                 −𝑘                                                           𝜋                              3𝜋
by using (𝑧 − 𝑥𝑗 )−𝑘 𝑗 = 𝑧 − 𝑥𝑗 𝑗
                                  exp −𝑖𝑘 𝑗 𝜃𝑗 , (− < 𝜃𝑗 <                                                                                                         )where𝜃𝑗 = arg 𝑧 − 𝑥𝑗 and j = 1, 2,..., n –
                                                       2                                                                                                      2
         ′
1, then 𝑓 𝑧 is analytic everywhere in the half plane, so
                                                                                       −𝑖𝑘                                −𝑖𝑘
                                                                                  𝐴𝑒         1    𝜃1                  𝑒                   2        𝜃2              𝑒 −𝑖𝑘 𝑛 −1   𝜃 𝑛 −1
                                                            𝑓′ 𝑧         =                                                                                  …
                                                                                       (𝑧−𝑥 1 ) 𝑘 1                (𝑧−𝑥 2 ) 𝑘 2                                      (𝑧−𝑥 𝑛 −1 ) 𝑘 𝑛 −1
          −𝑖𝑘        𝜃1          −𝑖𝑘       𝜃2
    𝐴 𝑒         1            𝑒         2                  𝑒 −𝑖𝑘 𝑛 −1     𝜃 𝑛 −1
=                   𝑘1                     𝑘2   …                             𝑘 𝑛 −1
        𝑧−𝑥 1                𝑧−𝑥 2                          𝑧−𝑥 𝑛 −1
          𝐴                  1                               1                                                                                                                                                  (1.6)
<               𝑘1           𝑘2            …                         𝑘 𝑛 −1
    𝑧−𝑥 1            𝑧−𝑥 2                       𝑧−𝑥 𝑛 −1
                     −𝑖𝑘 𝜃
By using 𝑒              1𝑗 𝑗               =1             and
                                                                                         2
                                                                                              < 𝑧 − 𝑥𝑗 < 2 𝑍 and
                                                                                          𝑍
                                                                                              1       1      2
                                                                                                 <         <
                                                                                             2 𝑍    𝑍 − 𝑥𝑗   𝑍
to equation (1.6) we have that
                             2𝐴        1        1
 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛 1.6 <                 𝑘1
                                   <     𝑘2
                                            …
                           𝑧         𝑧        𝑧 𝑘 𝑛 −1
            2𝐴
=     𝑘 1 𝑘 2 +⋯+𝑘 𝑛 −1 . Since 𝑘1 + 𝑘2 + ⋯ + 𝑘 𝑛−1 + 𝑥 𝑛 = 2,−1< 𝑘 𝑗 < 1 , (𝑗 = 1.2, … , 𝑛) then
    𝑧
                                                2𝐴                            2𝐴
                                           𝑘 1 𝑘 2 +⋯+𝑘 𝑛 −1         =          2−𝑘 𝑛         . It means, that there exist 𝑀 = 2𝐴 > 0 such that
                                       𝑧                                  𝑧
                                                                                                                                      𝑀                                                                          (1.7)
                                                                                          𝑓′ 𝑧          ≤                             2−𝑘 𝑛         .
                                                                                                                  𝑧
Using equation (1.7) and
                                                                                                                                               𝑧
                                                                                                                                                                                                                 (1.8)
                                                                          lim        lim
                                                                              𝐹 𝑧 =                                                                 𝑓 ′ 𝑠 𝑑𝑠
                                                                         𝑧→∞        𝑧→∞
                                                                                                                                          𝑧0
                                                                                                                                           𝑧
                                                                                                         lim
                                                                                                 ≤                                                 𝑓 ′ 𝑠 𝑑𝑠
                                                                                                        𝑧→∞
                                                                                                                                       𝑧0
                                                                                                                                  𝑧

                                                                                                  ≤ lim                                             𝑓′ 𝑠            𝑑𝑠
                                                                                                        𝑧 →∞
                                                                                                                      𝑧0
                                                                                                              𝑧
                                                                                           lim                                                          𝑀
                                                                                   ≤                                                                    2−𝑘 𝑛
                                                                                                                                                                     𝑑𝑠
                                                                                          𝑧→∞                                             𝑧
                                                                                                         𝑧0
                                                                                                                          𝑧                    1
                                                                                          = 𝑀 lim ∫𝑧                                               2−𝑘 𝑛      𝑑𝑠,
                                                                                                       𝑧→∞                0           𝑧
                                                 𝑧           1
since 2 − 𝑘 𝑛 > 1, then ∫𝑧                                   2−𝑘 𝑛       𝑑𝑠 → 0, that means the limit of the integral (1.7) exists as 𝑧 tend to infinity .
                                                 0    𝑧
So there exists a number 𝑤 𝑛 such that                                          𝑓 ∞ =: lim 𝐹(∞) = 𝑤 𝑛 ,𝐼𝑚 𝑧 ≥ 0 . Next we will prove the equation
                                                                                                  𝑧→∞
(1.3). After taking the argument to the equation (1.5) we have
arg     𝑓 ′ 𝑧 = arg 𝐴 − 𝑘1 arg 𝑧 − 𝑥1 − 𝑘2 arg 𝑧 − 𝑥2 − … − 𝑘 𝑛−1 arg⁡ − 𝑥 𝑛−1 )
                                                                           (𝑧
then by using identity (1.1),(1.2) yields
              arg     𝑓 ′ 𝑧 = arg       𝐴 + arg(𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 − ⋯ − arg(𝑧 − 𝑥 𝑛−1 )−𝑘 𝑛 −1
                             ′
                    arg     𝑓 𝑧 = arg        𝐴 (𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛 −1 )−𝑘 𝑛 −1
                               ′
                              𝑓 𝑧 =     𝐴 (𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛−1 )−𝑘 𝑛 −1
             −𝛼 1
Let −𝑘1 =         then we have
                         𝑥
                                                                                                 − 𝛼1                                               − 𝛼2                                  − 𝛼 𝑛 −1
                                           𝑓′ 𝑧 =                𝐴        (𝑧 − 𝑥1 )               𝑥
                                                                                                            (𝑧 − 𝑥2 )                                𝑥
                                                                                                                                                              …          (𝑧 − 𝑥 𝑛 −1 )      𝑥
                                                                                                                                                                                                     , and
                                                                                                        − 𝛼1                                            − 𝛼2                              − 𝛼 𝑛 −1
                                                          𝑓′ 𝑧 =                𝐴 (𝑧 − 𝑥1 )              𝑥
                                                                                                                  (𝑧 − 𝑥2 )                              𝑥
                                                                                                                                                                   … (𝑧 − 𝑥 𝑛 −1 )          𝑥

                                                                                                        − 𝛼1                                                − 𝛼2                          − 𝛼 𝑛 −1
                                                                                                         𝑥                                                   𝑥                              𝑥
                                                 𝑓 𝑧 + 𝑐=                         𝐴 (𝑧 − 𝑥1 )                         (𝑧 − 𝑥2 )                                    … (𝑧 − 𝑥 𝑛 −1 )
                                                                                                  − 𝛼1                                         − 𝛼2                               − 𝛼 𝑛 −1
                                                                                                   𝑥                                            𝑥                                   𝑥
                                                     𝑓 𝑧 =               𝐴 (𝑧 − 𝑥1 )                     (𝑧 − 𝑥2 )                                          … (𝑧 − 𝑥 𝑛 −1 )                   − 𝑐
If – 𝑐 = 𝐵 then
                                                                                                       − 𝛼1                                             − 𝛼2                             − 𝛼 𝑛 −1
                                                                                                        𝑥                                                𝑥                                 𝑥
                                                𝑓 𝑧 = 𝐵+                      𝐴 (𝑧 − 𝑥1 )                         (𝑧 − 𝑥2 )                                     … (𝑧 − 𝑥 𝑛 −1 )                      𝑑𝑧

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Schwarz-Christoffel Transformation On A Half Plane
                                                    − 𝛼1              − 𝛼2               − 𝛼 𝑛 −1
                              = 𝐵 + ∫ 𝐴 (𝑧 − 𝑥1 ) 𝑥 (𝑧 − 𝑥2 ) 𝑥 … (𝑧 − 𝑥 𝑛 −1 ) 𝑥            𝑑𝑧.
Next, since the argument of a product of the complex numbers are equal to the number of arguments of each
factor, from equation (1.5) we have
              arg𝑓 ′ 𝑧 = arg𝐴 − 𝑘1 arg 𝑧 − 𝑥1 − 𝑘2 arg 𝑧 − 𝑥2 − ⋯ − 𝑘 𝑛−1 arg 𝑧 − 𝑥 𝑛 −1 .                          (1.9)
The real numbers 𝑥1 , 𝑥2 , … , 𝑥 𝑛−1 , 𝑥 𝑛 take on the real axis z-plane. If 𝑧 is a real number, then the number
                                                    𝑁𝑗 = 𝑧 − 𝑥𝑗 ,                                                (1.10)
is positive if 𝑧 is greater than 𝑥𝑗 and negative if𝑧 is less than 𝑥𝑗 and
                                                          0,      if 𝑧 > 𝑥𝑗                                      (1.11)
                                        arg 𝑧 − 𝑥𝑗 =
                                                             𝜋, if 𝑧 < 𝑥𝑗 .

If 𝑧 = 𝑥 and 𝑥 < 𝑥𝑗 , 𝑗 = 1,2,3, … , 𝑛 − 1 then

                              arg 𝑧 − 𝑥1 = arg 𝑧 − 𝑥2 = ⋯ = arg 𝑧 − 𝑥 𝑛−1 = 𝜋.                                        (1.12)

If 𝑧 = 𝑥 and 𝑥 𝑟−1 < 𝑥 < 𝑥 𝑟 , j = 1, 2, ..., r – 1, r, r + 1, ..., n –1 and let
                                              𝜙 𝑟−1 = arg𝑓 ′ (𝑧)                                                       (1.13)

then according to equation (1.9) and (1.11) and (1.13)
               arg𝑓 ′ 𝑧 = arg𝐴 − 𝑘1 arg 𝑧 − 𝑥1 − 𝑘2 arg 𝑧 − 𝑥2 − ⋯ − 𝑘 𝑛−1 arg⁡ − 𝑥 𝑛−1 )
                                                                                      (𝑧
              𝜙 𝑟−1 = arg𝐴 − 𝑘 𝑟 arg 𝑧 − 𝑥 𝑟 − 𝑘 𝑟+1 arg 𝑧 − 𝑥 𝑟+1 − ⋯ − 𝑘 𝑛−1 arg⁡ − 𝑥 𝑛−1 )
                                                                                       (𝑧
                                 = arg𝐴 − 𝑘 𝑟 𝜋 − 𝑘 𝑟+1 𝜋 − 𝑘 𝑟+2 𝜋 − ⋯ − 𝑘 𝑛−1 𝜋
                             = arg𝐴 − (𝑘 𝑟 − 𝑘 𝑟+1 − 𝑘 𝑟+2 − ⋯ − 𝑘 𝑛−1 )𝜋                                              (1.14)
and
             𝜙 𝑟 = arg𝐴 − 𝑘 𝑟+1 arg 𝑧 − 𝑥 𝑟+1 − 𝑘 𝑟+2 arg 𝑧 − 𝑥 𝑟+2 − ⋯ − 𝑘 𝑛−1 arg 𝑧 − 𝑥 𝑛−1
                               = arg𝐴 − 𝑘 𝑟+1 𝜋 − 𝑘 𝑟+2 𝜋 − 𝑘 𝑟+3 𝜋 − ⋯ − 𝑘 𝑛−1 𝜋
                                      = arg𝐴 − (𝑘 𝑟+1 − 𝑘 𝑟+2 − 𝑘 𝑟+3 − ⋯ − 𝑘 𝑛−1 )𝜋                                  (1.15)
Then
      𝜙 𝑟 − 𝜙 𝑟 −1 = [arg𝐴 − (𝑘 𝑟+1 − 𝑘 𝑟+2 − 𝑘 𝑟+3 − ⋯ − 𝑘 𝑛−1 )𝜋]                                                   (1.16)
                      −                              [arg𝐴 − (𝑘 𝑟 − 𝑘 𝑟+1 − 𝑘 𝑟+2 − ⋯ − 𝑘 𝑛−1 )𝜋]

𝜙   𝑟   − 𝜙   𝑟 −1 =𝑘 𝑟   𝜋 ,with 𝑗 = 1,2,3, ⋯ , 𝑟 − 1, 𝑟, ⋯ , 𝑛 − 1.

Such that, if 𝑧 = 𝑥 then 𝑥𝑗 −1 < 𝑥 < 𝑥𝑗 , 𝑗 = 1,2, … , 𝑛 − 1 in the real axis 𝑧-plane from the left point 𝑥𝑗 to his
right, then the vector𝜏 in 𝑤-plane change with angle 𝑘 𝑗 𝜋, on the point of the image 𝑥𝑗 ,as shown in Figure 1.2.
angle 𝑘 𝑗 𝜋 is outside the terms of the 𝑧-plane at the point𝑊𝑗 .


                                                                  V
                              Y                                                     W1

                                                                                         W                  Wn
                                                                        W2

                                                                             k 2                          W4
                                                                                     
                          z                                                                         k 3
                                                                                         W3
                                                              X                                                  U
        x1    x2     t            x 3 x4             x n 1
                        Figure 1.2. Mapping 𝑓 (𝑧) with 𝑧 = 𝑥 and 𝑥𝑗 −1 < 𝑥 < 𝑥𝑗 (see [3])
It is assumed that the sides of the 𝑧-plane do not intersect each other and take opposite corners clockwise.
Outside corners can be approximated by the angle between𝜋 and - 𝜋, so that
−1 < 𝑘 𝑗 < 1, If the terms of n-closed, the number of outer corner is 2𝜋.To prove it is seen to
have sided closed (n + 1), see Figure 1.3


                                                         www.irjes.com                                               28 | Page
Schwarz-Christoffel Transformation On A Half Plane

                                    V
                                                            W2               k1
                                                  k 2
                                                                                   W1

                                                                                   k n 1

                                                                            Wn 1
                                                         Wn         k n
                                                                                             U

                                 Figure 1.3.Closed 𝑛-image has (𝑛 + 1) plane ( see [3]).

It has known that 𝑘 𝑗 𝜋 is the magnitude of the outer corner at the point 𝑊𝑗 which is the image of a point 𝑥𝑗 .If
many terms have side n + 1, then
                                                   𝑘 2 𝜋 = 𝜙2 − 𝜙1
                                                   𝑘 3 𝜋 = 𝜙3 − 𝜙2
                                                     𝑘 4 𝜋 = 𝜙4 − 𝜙3
                                                           ⋮
                                                 𝑘 𝑛 𝜋 = 𝜙 𝑛 − 𝜙 𝑛−1
While the angle 𝑘 1 𝜋 = 𝜙1 − 𝜙 𝑛+1 and 𝑘 𝑛+1 𝜋 = 𝜙 𝑛+1 + 2𝜋 − 𝜙 𝑛 .
In terms of -n. 𝑘 𝑛+1 𝜋 = 0 so that 𝜙 𝑛 = 𝜙 𝑛+1 + 2𝜋 . Thus, the
 𝑘1 𝜋 + 𝑘2 𝜋 + 𝑘3 𝜋 + ⋯ + 𝑘 𝑛 𝜋 = (𝜙1 − 𝜙 𝑛+1 ) + (𝜙2 − 𝜙1 ) + (𝜙3 − 𝜙2 ) + ⋯ + (𝜙 𝑛 − 𝜙 𝑛+1 )
                                    (𝑘1 + 𝑘2 + 𝑘3 + ⋯ + 𝑘 𝑛 )𝜋 = (𝜙 𝑛 − 𝜙 𝑛+1 )
                                                                 = 2𝜋
                                        𝑘1 + 𝑘2 + 𝑘3 + ⋯ + 𝑘 𝑛 = 2                                      (1.17)

So it is clear that 𝑘 𝑗 with 𝑗 = 1, 2, 3, . . . , 𝑛satisfy the condition
                                      𝑘1 + 𝑘2 + 𝑘3 + ⋯ + 𝑘 𝑛 = 2 , −1 < 𝑘 𝑗 < 1.
End of proof.

                                            V.       ACKNOWLEDGEMENTS
I would like to thankProf.Dr.Marjono and Dr. Bagus, for theencouragements.

                                                         REFERENCES
[1].   Mark J. Ablowitz Athanassios S.fokas. Complex variables : Introduction andapplications, Second edition.Cambridge texts in
       applied mathematics,2003.
[2].   Howell, L.H. Computation of conformal maps by modified Schwarz-Christoffel transformations, 1990.
[3].   James Ward Brown and Ruel V.Churchil. Complex Variables and Applictions, Eighth Edition, McGraw-Hill, 2009.
[4].   Dennis G.Zill. Complex Analysis with Applications, Jones and Bartlett Publisher, 2003.
[5].   Jhon Mathews and Russell Howell. Complex analysis for mathmatics and engineering sixth edition,Jones and Bartlett Publisher,
       2012.
[6].   Tobin A.Driscoll and Lloyd N. Thefethen. Schwarz-Christoffel Mapping, Cambridge Monographs on Applied and Computational
       Mathematics, 2002.
[7].   Gonzalo Riera , Herna ́n Carrasco , and Rube ́n Preiss .The Schwarz-Christoffel conformal mapping for ′′Polygons′′ with Infinitely
       Many Sides,InternationalJournal of Mathematics and Mathematical, Sciences Volume 2008, Hindawi Publishing Corporation, 2008.




                                                            www.irjes.com                                                   29 | Page

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  • 1. International Refereed Journal of Engineering and Science (IRJES) ISSN (Online) 2319-183X, (Print) 2319-1821 Volume 2, Issue 2(February 2013), PP.25-29 www.irjes.com Schwarz-Christoffel Transformation On A Half Plane Abdualah Ibrahim Sultan Mathematics Department of Brawijaya University Malang, Indonesia. Mathematics Department of, Faculty of Science, Khoms, Al-Mergeb University , Khoms, Libya. ABSTRACT :The Schwarz-Christoffel transformation has been studied by many reseachers due to a huge of its application in solving Laplace's equations and studying fluid flow phenomenas ( see [3],[4]). The proof of this theorem can find in (see for example [5]). Their method depend on the tangent of 𝑇𝑗 = 1 + 𝑖0 and the rotation of 𝑇𝑗 from 0 to 𝜋 on points (𝑥, 0) . In this paper we would like to prove the Shwarz- Christoffeltransformation directly by using the arguments identity of complex number, rotation of it from 0 to 2𝜋 and conformal mapping. Keywords : Complex function, half plane, polygon, analytic function, transformation, Conformal mapping. I. INTRODUCTION The Schwarz-Christoffel transformation known as a map from the upper half-plane to simply connected polygon with or without corners at infinity in the complex planes.The Schwarz-Christoffel transformation has been studied by many reseachers due to a huge of its application for example used in physical applications involving fluid movement, heat conduction and electrostatic pontential, as well asthe studying of Laplace's equations (see [3],[4]) and also from mathematical point of views ( see [1],[2],[6]). In this paper we study about the proof of the Schwarz-Christoffel theorem. The prove of this theorem can found in (see for example [5]). Their method depend on the tangent of 𝑇𝑗 = 1 + 𝑖0 and the rotation of 𝑇𝑗 from 0 to 𝜋 on points (𝑥, 0). In this paper we would like to prove the Shwarz-Christoffel transformation directly by using the arguments identity of complex number, rotation of it from 0 to 2𝜋 and conformal mapping. II. PRELIMINARIES We need to review some important definitions and theorems which will be used later from complex analysis to understand the Schwarz-Christoffeltheorem.These definitions and theorems below can be found in the refences ( see [3], [4] ). Definition 2.1 A complex number is a number of the form 𝑧 = 𝑎 + 𝑖𝑏 where the imaginary unit is defined as 𝑖 = −1and𝑎 is the real part of 𝑧, 𝑎 = 𝑅𝑒(𝑧), and 𝑏 is the imaginary part of 𝑧 , 𝑏 = 𝐼𝑚(𝑧). The set of all complex number is written by 𝐶. Definition 2.2. Arguments of complex number Let r and θ be polar coordinates of the point 𝑎, 𝑏 that corresponds to a nonzero complex number 𝑧 = 𝑎 + 𝑖𝑏. Since 𝑎 = cos 𝜃and 𝑏 = sin 𝜃, the number 𝑧can be written in polar form as 𝑧 = r (cos 𝜃 + 𝑖 sin 𝜃) = 𝑧 𝑒 𝑖𝜃 , where 𝑧 is a positive real number called the modulus of 𝑧, and 𝜃 is real number called the argument of 𝑧, and written by arg 𝑧.The real number𝜃 represents the angle and measured in radians. Theorem 2.1. Law of arguments of products . Let 𝑏, 𝑐 ∈ 𝐶. Then arg 𝑏𝑐 = arg b + arg c. (1.1) Theorem 2.2. Law of arguments of power Let 𝑏, 𝑐 ∈ 𝐶. Then arg 𝑏 𝑐 = 𝑐 arg 𝑏. (1.2) Definition 2.3.Complex Function. A complex function is a function 𝑓 whose domain and range are subsets of the set 𝐶 of complex numbers. Definition 2.4.Conformal mapping. Let 𝑤 = 𝑓 (𝑧) be a complex mapping defined in a domain 𝐷 and let 𝑧0 be a point in 𝐷. Then we say that 𝑤 = 𝑓 (𝑧) is conformal at 𝑧0 if for every pair of smoothoriented curves𝐶1 and 𝐶2 in 𝐷 intersecting at 𝑧0 the angle between 𝐶1 and 𝐶2 at𝑧0 is equal tothe angle between the image curves 𝐶 ′ 1 and 𝐶 ′ 2 at 𝑓 (𝑧0 ) in both magnitude and sense. www.irjes.com 25 | Page
  • 2. Schwarz-Christoffel Transformation On A Half Plane Figure 1.1 The angle between𝐶1 and 𝐶2 (see [4]) In other words a mapping 𝑤 = 𝑓 (𝑧) preserves both angle and shape but it cannot in general the size. Moreover a mapping that is conformal at every point in a domain D is called conformal in D, the conformal mapping relies on the properties of analytic function. The angle between any two intersecting arcs in the z-plane is equal to the angle between the images of the arcs in the w-plane under a linear mapping. Definition 2.5. Analytic Function.A function 𝑓 (𝑧) is said to be analytic in a region 𝑅 of the complex plane if 𝑓 (𝑧) has a derivative at each point of 𝑅. In addition, analytic function is conformal at 𝑧0 if and only if 𝑓 ′ (𝑧) ≠ 0. Definition 2.6.Polygon. A polygon is a plane figure that is bounded by closed path, composed of a finite sequence of straight-line segments (i.e. a closed polygonal chain or circuit). These segments are called its edges or sides, and the points where two edges meet are the polygon’s vertices (singular: vertex) or corners. III. MAIN THEOREM Theorem (Schwarz-christoffel) Let 𝑃 be a polygon in the 𝑤-plane with vertices 𝑤1 , 𝑤2 , … , 𝑤 𝑛 and exterior angles 𝛼 𝑘 , where – 𝜋 < 𝛼 𝑘 < 𝜋 .There exists a one-to-one conformal mapping 𝑤 = 𝑓 (𝑧) from the upper half plane, 𝐼𝑚 𝑧 > 0 onto 𝐺 that satisfies the boundary conditions in equations 𝑤 𝑘 = 𝑓 (𝑥 𝑘 ) for 𝑘 = 1,2 … . 𝑛 − 1 and 𝑤 𝑛 = 𝑓 ∞ , where 𝑥1 < 𝑥2 < 𝑥3 < ⋯ < 𝑥 𝑛−1 < ∞. Derivative 𝑓 ′ (𝑧) is − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 (1.3) 𝑓 ′ 𝑧 = 𝐴 𝑧 − 𝑥1 ) 𝜋 𝑧 − 𝑥2 𝜋 … 𝑧 − 𝑥 𝑛 −1 𝜋 and the function f can be expressed as an indefinite integral − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 (1.4) 𝑓 𝑧 = 𝐵 + 𝐴 ∫ 𝑓 ′ 𝑧 = 𝐴 𝑧 − 𝑥1 ) 𝜋 𝑧 − 𝑥2 𝜋 … 𝑧 − 𝑥 𝑛 −1 𝜋 𝑑𝑧 where 𝐴 and 𝐵 are suitably chosen constants. Two of the points {𝑥 𝑘 } may be chosen arbitrarily, and the constants 𝐴 and 𝐵 determine the size and position of 𝑃. IV. PROVE OF THE THEOREM A transformation 𝑤 = 𝑓 𝑧 constructed by mapping each point on the 𝑥 axis in 𝑧 -plane z on 𝑤 -plane, with 𝑥1 , 𝑥2 , … , 𝑥 𝑛−1 , 𝑥 𝑛 are the points on the 𝑥-axis and 𝑥1 < 𝑥2 < 𝑥3 < ⋯ < 𝑥 𝑛 −1 < 𝑥 𝑛 where the points on the plane 𝑧 is the domain of the transformation. These points are mapped in to points on the 𝑛-side, is 𝑤𝑗 = 𝑓(𝑥 𝑗 ), 𝑗 = 1, 2, . . . , 𝑛 -1 and 𝑤 𝑛 = 𝑓 ∞ in 𝑤-plane. The function 𝑓chosen so that arg 𝑓 ′ 𝑧 different constant value 𝑓 ′ 𝑧 = 𝐴(𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛 −1 )−𝑘 𝑛 −1 (1.5) where A is a complex constant and each 𝑘 𝑗 , with 𝑗 = 1, 2, 3, 𝑛 − 1 are real constants. From equation (1.5) we taking the absolute value, then we have 𝑓 ′ 𝑧 = 𝐴(𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛−1 ) 𝑘 𝑛 −1 −𝑘 1 −𝑘 2 = 𝐴 (𝑧 − 𝑥1 ) (𝑧 − 𝑥2 ) … (𝑧 − 𝑥 𝑛 −1 )−𝑘 𝑛 −1 𝐴 1 1 = 𝑘1 (𝑧−𝑥 1 ) 𝑘2 … (𝑧−𝑥 2 ) 𝑘 𝑛 −1 , (𝑧−𝑥 𝑛 −1 ) www.irjes.com 26 | Page
  • 3. Schwarz-Christoffel Transformation On A Half Plane −𝑘 𝜋 3𝜋 by using (𝑧 − 𝑥𝑗 )−𝑘 𝑗 = 𝑧 − 𝑥𝑗 𝑗 exp −𝑖𝑘 𝑗 𝜃𝑗 , (− < 𝜃𝑗 < )where𝜃𝑗 = arg 𝑧 − 𝑥𝑗 and j = 1, 2,..., n – 2 2 ′ 1, then 𝑓 𝑧 is analytic everywhere in the half plane, so −𝑖𝑘 −𝑖𝑘 𝐴𝑒 1 𝜃1 𝑒 2 𝜃2 𝑒 −𝑖𝑘 𝑛 −1 𝜃 𝑛 −1 𝑓′ 𝑧 = … (𝑧−𝑥 1 ) 𝑘 1 (𝑧−𝑥 2 ) 𝑘 2 (𝑧−𝑥 𝑛 −1 ) 𝑘 𝑛 −1 −𝑖𝑘 𝜃1 −𝑖𝑘 𝜃2 𝐴 𝑒 1 𝑒 2 𝑒 −𝑖𝑘 𝑛 −1 𝜃 𝑛 −1 = 𝑘1 𝑘2 … 𝑘 𝑛 −1 𝑧−𝑥 1 𝑧−𝑥 2 𝑧−𝑥 𝑛 −1 𝐴 1 1 (1.6) < 𝑘1 𝑘2 … 𝑘 𝑛 −1 𝑧−𝑥 1 𝑧−𝑥 2 𝑧−𝑥 𝑛 −1 −𝑖𝑘 𝜃 By using 𝑒 1𝑗 𝑗 =1 and 2 < 𝑧 − 𝑥𝑗 < 2 𝑍 and 𝑍 1 1 2 < < 2 𝑍 𝑍 − 𝑥𝑗 𝑍 to equation (1.6) we have that 2𝐴 1 1 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛 1.6 < 𝑘1 < 𝑘2 … 𝑧 𝑧 𝑧 𝑘 𝑛 −1 2𝐴 = 𝑘 1 𝑘 2 +⋯+𝑘 𝑛 −1 . Since 𝑘1 + 𝑘2 + ⋯ + 𝑘 𝑛−1 + 𝑥 𝑛 = 2,−1< 𝑘 𝑗 < 1 , (𝑗 = 1.2, … , 𝑛) then 𝑧 2𝐴 2𝐴 𝑘 1 𝑘 2 +⋯+𝑘 𝑛 −1 = 2−𝑘 𝑛 . It means, that there exist 𝑀 = 2𝐴 > 0 such that 𝑧 𝑧 𝑀 (1.7) 𝑓′ 𝑧 ≤ 2−𝑘 𝑛 . 𝑧 Using equation (1.7) and 𝑧 (1.8) lim lim 𝐹 𝑧 = 𝑓 ′ 𝑠 𝑑𝑠 𝑧→∞ 𝑧→∞ 𝑧0 𝑧 lim ≤ 𝑓 ′ 𝑠 𝑑𝑠 𝑧→∞ 𝑧0 𝑧 ≤ lim 𝑓′ 𝑠 𝑑𝑠 𝑧 →∞ 𝑧0 𝑧 lim 𝑀 ≤ 2−𝑘 𝑛 𝑑𝑠 𝑧→∞ 𝑧 𝑧0 𝑧 1 = 𝑀 lim ∫𝑧 2−𝑘 𝑛 𝑑𝑠, 𝑧→∞ 0 𝑧 𝑧 1 since 2 − 𝑘 𝑛 > 1, then ∫𝑧 2−𝑘 𝑛 𝑑𝑠 → 0, that means the limit of the integral (1.7) exists as 𝑧 tend to infinity . 0 𝑧 So there exists a number 𝑤 𝑛 such that 𝑓 ∞ =: lim 𝐹(∞) = 𝑤 𝑛 ,𝐼𝑚 𝑧 ≥ 0 . Next we will prove the equation 𝑧→∞ (1.3). After taking the argument to the equation (1.5) we have arg 𝑓 ′ 𝑧 = arg 𝐴 − 𝑘1 arg 𝑧 − 𝑥1 − 𝑘2 arg 𝑧 − 𝑥2 − … − 𝑘 𝑛−1 arg⁡ − 𝑥 𝑛−1 ) (𝑧 then by using identity (1.1),(1.2) yields arg 𝑓 ′ 𝑧 = arg 𝐴 + arg(𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 − ⋯ − arg(𝑧 − 𝑥 𝑛−1 )−𝑘 𝑛 −1 ′ arg 𝑓 𝑧 = arg 𝐴 (𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛 −1 )−𝑘 𝑛 −1 ′ 𝑓 𝑧 = 𝐴 (𝑧 − 𝑥1 )−𝑘 1 (𝑧 − 𝑥2 )−𝑘 2 … (𝑧 − 𝑥 𝑛−1 )−𝑘 𝑛 −1 −𝛼 1 Let −𝑘1 = then we have 𝑥 − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 𝑓′ 𝑧 = 𝐴 (𝑧 − 𝑥1 ) 𝑥 (𝑧 − 𝑥2 ) 𝑥 … (𝑧 − 𝑥 𝑛 −1 ) 𝑥 , and − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 𝑓′ 𝑧 = 𝐴 (𝑧 − 𝑥1 ) 𝑥 (𝑧 − 𝑥2 ) 𝑥 … (𝑧 − 𝑥 𝑛 −1 ) 𝑥 − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 𝑥 𝑥 𝑥 𝑓 𝑧 + 𝑐= 𝐴 (𝑧 − 𝑥1 ) (𝑧 − 𝑥2 ) … (𝑧 − 𝑥 𝑛 −1 ) − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 𝑥 𝑥 𝑥 𝑓 𝑧 = 𝐴 (𝑧 − 𝑥1 ) (𝑧 − 𝑥2 ) … (𝑧 − 𝑥 𝑛 −1 ) − 𝑐 If – 𝑐 = 𝐵 then − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 𝑥 𝑥 𝑥 𝑓 𝑧 = 𝐵+ 𝐴 (𝑧 − 𝑥1 ) (𝑧 − 𝑥2 ) … (𝑧 − 𝑥 𝑛 −1 ) 𝑑𝑧 www.irjes.com 27 | Page
  • 4. Schwarz-Christoffel Transformation On A Half Plane − 𝛼1 − 𝛼2 − 𝛼 𝑛 −1 = 𝐵 + ∫ 𝐴 (𝑧 − 𝑥1 ) 𝑥 (𝑧 − 𝑥2 ) 𝑥 … (𝑧 − 𝑥 𝑛 −1 ) 𝑥 𝑑𝑧. Next, since the argument of a product of the complex numbers are equal to the number of arguments of each factor, from equation (1.5) we have arg𝑓 ′ 𝑧 = arg𝐴 − 𝑘1 arg 𝑧 − 𝑥1 − 𝑘2 arg 𝑧 − 𝑥2 − ⋯ − 𝑘 𝑛−1 arg 𝑧 − 𝑥 𝑛 −1 . (1.9) The real numbers 𝑥1 , 𝑥2 , … , 𝑥 𝑛−1 , 𝑥 𝑛 take on the real axis z-plane. If 𝑧 is a real number, then the number 𝑁𝑗 = 𝑧 − 𝑥𝑗 , (1.10) is positive if 𝑧 is greater than 𝑥𝑗 and negative if𝑧 is less than 𝑥𝑗 and 0, if 𝑧 > 𝑥𝑗 (1.11) arg 𝑧 − 𝑥𝑗 = 𝜋, if 𝑧 < 𝑥𝑗 . If 𝑧 = 𝑥 and 𝑥 < 𝑥𝑗 , 𝑗 = 1,2,3, … , 𝑛 − 1 then arg 𝑧 − 𝑥1 = arg 𝑧 − 𝑥2 = ⋯ = arg 𝑧 − 𝑥 𝑛−1 = 𝜋. (1.12) If 𝑧 = 𝑥 and 𝑥 𝑟−1 < 𝑥 < 𝑥 𝑟 , j = 1, 2, ..., r – 1, r, r + 1, ..., n –1 and let 𝜙 𝑟−1 = arg𝑓 ′ (𝑧) (1.13) then according to equation (1.9) and (1.11) and (1.13) arg𝑓 ′ 𝑧 = arg𝐴 − 𝑘1 arg 𝑧 − 𝑥1 − 𝑘2 arg 𝑧 − 𝑥2 − ⋯ − 𝑘 𝑛−1 arg⁡ − 𝑥 𝑛−1 ) (𝑧 𝜙 𝑟−1 = arg𝐴 − 𝑘 𝑟 arg 𝑧 − 𝑥 𝑟 − 𝑘 𝑟+1 arg 𝑧 − 𝑥 𝑟+1 − ⋯ − 𝑘 𝑛−1 arg⁡ − 𝑥 𝑛−1 ) (𝑧 = arg𝐴 − 𝑘 𝑟 𝜋 − 𝑘 𝑟+1 𝜋 − 𝑘 𝑟+2 𝜋 − ⋯ − 𝑘 𝑛−1 𝜋 = arg𝐴 − (𝑘 𝑟 − 𝑘 𝑟+1 − 𝑘 𝑟+2 − ⋯ − 𝑘 𝑛−1 )𝜋 (1.14) and 𝜙 𝑟 = arg𝐴 − 𝑘 𝑟+1 arg 𝑧 − 𝑥 𝑟+1 − 𝑘 𝑟+2 arg 𝑧 − 𝑥 𝑟+2 − ⋯ − 𝑘 𝑛−1 arg 𝑧 − 𝑥 𝑛−1 = arg𝐴 − 𝑘 𝑟+1 𝜋 − 𝑘 𝑟+2 𝜋 − 𝑘 𝑟+3 𝜋 − ⋯ − 𝑘 𝑛−1 𝜋 = arg𝐴 − (𝑘 𝑟+1 − 𝑘 𝑟+2 − 𝑘 𝑟+3 − ⋯ − 𝑘 𝑛−1 )𝜋 (1.15) Then 𝜙 𝑟 − 𝜙 𝑟 −1 = [arg𝐴 − (𝑘 𝑟+1 − 𝑘 𝑟+2 − 𝑘 𝑟+3 − ⋯ − 𝑘 𝑛−1 )𝜋] (1.16) − [arg𝐴 − (𝑘 𝑟 − 𝑘 𝑟+1 − 𝑘 𝑟+2 − ⋯ − 𝑘 𝑛−1 )𝜋] 𝜙 𝑟 − 𝜙 𝑟 −1 =𝑘 𝑟 𝜋 ,with 𝑗 = 1,2,3, ⋯ , 𝑟 − 1, 𝑟, ⋯ , 𝑛 − 1. Such that, if 𝑧 = 𝑥 then 𝑥𝑗 −1 < 𝑥 < 𝑥𝑗 , 𝑗 = 1,2, … , 𝑛 − 1 in the real axis 𝑧-plane from the left point 𝑥𝑗 to his right, then the vector𝜏 in 𝑤-plane change with angle 𝑘 𝑗 𝜋, on the point of the image 𝑥𝑗 ,as shown in Figure 1.2. angle 𝑘 𝑗 𝜋 is outside the terms of the 𝑧-plane at the point𝑊𝑗 . V Y W1 W Wn W2 k 2 W4  z k 3 W3 X U x1 x2 t x 3 x4 x n 1 Figure 1.2. Mapping 𝑓 (𝑧) with 𝑧 = 𝑥 and 𝑥𝑗 −1 < 𝑥 < 𝑥𝑗 (see [3]) It is assumed that the sides of the 𝑧-plane do not intersect each other and take opposite corners clockwise. Outside corners can be approximated by the angle between𝜋 and - 𝜋, so that −1 < 𝑘 𝑗 < 1, If the terms of n-closed, the number of outer corner is 2𝜋.To prove it is seen to have sided closed (n + 1), see Figure 1.3 www.irjes.com 28 | Page
  • 5. Schwarz-Christoffel Transformation On A Half Plane V W2 k1 k 2 W1 k n 1 Wn 1 Wn k n U Figure 1.3.Closed 𝑛-image has (𝑛 + 1) plane ( see [3]). It has known that 𝑘 𝑗 𝜋 is the magnitude of the outer corner at the point 𝑊𝑗 which is the image of a point 𝑥𝑗 .If many terms have side n + 1, then 𝑘 2 𝜋 = 𝜙2 − 𝜙1 𝑘 3 𝜋 = 𝜙3 − 𝜙2 𝑘 4 𝜋 = 𝜙4 − 𝜙3 ⋮ 𝑘 𝑛 𝜋 = 𝜙 𝑛 − 𝜙 𝑛−1 While the angle 𝑘 1 𝜋 = 𝜙1 − 𝜙 𝑛+1 and 𝑘 𝑛+1 𝜋 = 𝜙 𝑛+1 + 2𝜋 − 𝜙 𝑛 . In terms of -n. 𝑘 𝑛+1 𝜋 = 0 so that 𝜙 𝑛 = 𝜙 𝑛+1 + 2𝜋 . Thus, the 𝑘1 𝜋 + 𝑘2 𝜋 + 𝑘3 𝜋 + ⋯ + 𝑘 𝑛 𝜋 = (𝜙1 − 𝜙 𝑛+1 ) + (𝜙2 − 𝜙1 ) + (𝜙3 − 𝜙2 ) + ⋯ + (𝜙 𝑛 − 𝜙 𝑛+1 ) (𝑘1 + 𝑘2 + 𝑘3 + ⋯ + 𝑘 𝑛 )𝜋 = (𝜙 𝑛 − 𝜙 𝑛+1 ) = 2𝜋 𝑘1 + 𝑘2 + 𝑘3 + ⋯ + 𝑘 𝑛 = 2 (1.17) So it is clear that 𝑘 𝑗 with 𝑗 = 1, 2, 3, . . . , 𝑛satisfy the condition 𝑘1 + 𝑘2 + 𝑘3 + ⋯ + 𝑘 𝑛 = 2 , −1 < 𝑘 𝑗 < 1. End of proof. V. ACKNOWLEDGEMENTS I would like to thankProf.Dr.Marjono and Dr. Bagus, for theencouragements. REFERENCES [1]. Mark J. Ablowitz Athanassios S.fokas. Complex variables : Introduction andapplications, Second edition.Cambridge texts in applied mathematics,2003. [2]. Howell, L.H. Computation of conformal maps by modified Schwarz-Christoffel transformations, 1990. [3]. James Ward Brown and Ruel V.Churchil. Complex Variables and Applictions, Eighth Edition, McGraw-Hill, 2009. [4]. Dennis G.Zill. Complex Analysis with Applications, Jones and Bartlett Publisher, 2003. [5]. Jhon Mathews and Russell Howell. Complex analysis for mathmatics and engineering sixth edition,Jones and Bartlett Publisher, 2012. [6]. Tobin A.Driscoll and Lloyd N. Thefethen. Schwarz-Christoffel Mapping, Cambridge Monographs on Applied and Computational Mathematics, 2002. [7]. Gonzalo Riera , Herna ́n Carrasco , and Rube ́n Preiss .The Schwarz-Christoffel conformal mapping for ′′Polygons′′ with Infinitely Many Sides,InternationalJournal of Mathematics and Mathematical, Sciences Volume 2008, Hindawi Publishing Corporation, 2008. www.irjes.com 29 | Page