1549301742-The_Theory_of_Difference_Schemes__Samarskii

(jair2018) #1
Other iterative inethods

vVhen providing current nrnnipulations with

2 2
1 - p2 + a 2 = 1 - p2 + x ( 1 - po )
o o 1 _ x2

1 - PZ
1-x^2

a2
x2 ,

we find that

a2(x+po)
CY=----
x (1 - p~)

1 + XPo


l+CY=---1-x (^2) '
1


B=--


l +CY

x(x +Po)
1 - x^2

and, consequently, the expression for the function

1 1 p^2 +cy-a~ 'I
f(B)= l+CYPo+ l+CY JCY2+a2= o.
( 1 + CY) Po

Taking into account that


2? 2 2 a^2
p 0 +CY - Ci~ = ( 1 +CY) - ( l - p 0 +a ) = l +CY - 2
x

it is plain to show that


II

x+ Po


Sii:::; --


1 + XPo


1 - PZ Po+ X
1 - x2 = Po 1 - x2 ,

1-x^2


for T = T 0 ---


1 + XPo


739

The meaning of this is that a solution of problem (30) satisfies the
estin1ate


with


(39)
x+Po
p=
1 + x Po '


11 Yn - 1l 11 < P^71 11 Yo - U 11


T 0 ( 1 - x")

x = ----;====;;o /3 T=T=----


J11 12 + ,; '

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