R
z0
v
a
z0
*
v
v
a
a−
Ψ
= 0
Ψ
= 0
‘zyS’“•”f–æ—g˜R˜Í·™f~ ytlƒy~{•ng”fr6n•–ƒ”€k€ytry…¶{•kŒ„•”f–‡f–t{¨§}‚kŒn•–ƒ“guðy¡‚r”ˆi˜yz}‡–¡–‡uª ¯ –ær“gi€”zr}·6¤Y}‡i‚‚Æ }tySrp˜
v
a
v
a
v
a
v
a
v
a
d
......
Linha infinita de vortices
‘$yt’“•”z–t—g˜R˜š—gf}è y~{•p•kyƒ{g¤t{2yRiwk•}‡ruvy¡‚r”ziCyz}‡–pŠn•–y~{ji€–b{•CySn§kmn•– • ˜
™™
......
d
Ú
= vortice
= ponto de estagnacao (u,v) = (0,0)
‘$yt’“•”z–t—g˜R˜W•f}è y~{•p•kmŠn•–Í}pr”z”f–b{if–»„•km”€kskql~yƒ{•p§k·y~{™¤t{2ySi€k€n•–vy¡‚r”ziCyz}p–‡p˜
v
v
v
v
v
v
v
v
v
v
v
v
vv
vv
vv
vv
v
v
v
v
‘$yt’“•”z–t—g˜R˜¢—™f}è y~{•p•kmŠn•–Í}pr”z”f–b{if–»„•km”€kq“•uxk€¦drltp§k€ng–tymr”ziCyz}bytn§kmng–m˜
g˜
x
t
Molecula do
Metodo
n
n+1
j−1
w j
w
=pontos com os dados iniciais
X
x
X =
x neste ponto calculamos o valor da solucao c
j
wn
‘zyS’“•”f–e•˜e—™f}Èyy)km’”fkmuxkE}pru’ksuxkmlSp§k€„§km”fksrs„•”zré•lS–puxk€n2yts}p”f–i€r•˜
x
t
Molecula do
Metodo
j
y
1
= pontos com valores diferentes de zero
j+4
€
0 00000000
‘zyS’“•”f–e•˜ gf}Èyy)km’”fkmuxkE}pru’ksuxkmlSp§k€„§km”fksrs„•”zré•lS–puxk€n2yts}p”f–i€r•˜
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