, J ) ) ) ), issue.1

, IP? IF(0( l,J)-l. 058,50,59 58 COI I, «TD/RD on 5 I=3,K n'i 5 J=4

, Gn Tn, vol.5, p.59

, NI (I. MPI )=NI(1.NP2) NKI.NP? )=NI(I,NP4) N I ( NP 3 . ? ) =N l ( NP3 . 4 ) Nt(NP3, 1)=NI(NP3,5 )

, N! ( MM ,NP3) =NI ( NP1 ,NP4) NI (Nf'I ,2)=NI ( NP1 ,4) NI (MPI . 1 )=M( NP1 ,5)

, Ui( I ,J )-0.C)7f ,71 ,7 70 !F(UT( I.JI-!).C)72.b4, Jlrt.J)-1, vol.74

+. Ni-(-i-+2 and J. , IOOl I , J?-1 . )*GO( I . J)-Nl, vol.2, issue.1-1

, J) )*U+, vol.1, issue.1-1

, I ) )*2.*R( I ) )

, IFCul ( I , J)-l .0)7-»,79.79 7ti ?

, I ) )*2.*(U+V) )

*. and J. ?/(c'h-i, J )+f?0( l ) ) )?( ( NI ( 1+ 1 .Jl+Nl ( 1-1 , J) )*U+(NI ( I , 3+({NI(I+l, J) )*F, vol.1, issue.1-1

, *2 *R ( I ) ) )

, GO Tn, vol.00, issue.1, p.85

, J) )*U+, vol.1, issue.1-1

, ) )+D0( I ) ) *2

+. , N! ( i + l ,j ) +ni { :-i ,j) )*u + (nk i, j + l )

, ( I ) )*2.*R( I ) ) ) GO TO 90 9

, J)**, vol.2, issue.1

*. , Jl/CCOl I ? J1+1ÏOC I ) ) ) 1 + (NI ( l + l, J 1 + N 1 t-1, J ) )*U+

, (C0( 1 J ) +DQ t )*2.*R( I ) ) ) 90 CCfTtNUF 4 FPf-fcTS+ABS(Nl ( I ,J)-HPLOT) lF(FI?S.Lr.ffPSV|AX )G0 TO 6 IF( ITf-t, p.0

. I=1,

, ITF ( 3,301 )(Nl( 1 ,J) ,J=l ,NP3) 91

. Table and . Probt, Coaputad valu»» of probe currant for values of K»jmold» nusbar from 5 to 60

, FICOU 1.3 àpprtmimmf root* et probe condition* for varleus eonttmraa flovini platau. la .n of tboue applleatloas, typleal Mjmoldt mmbmn rang* froa 10, p.10

, FIGURE 5.3d Angle dependence of local current for various surface potentiels. Re-10

, RE 5.3e Angle dependence of local current for various surface potentiels. Re-10

, FIGURE 5.3f Ancle dependence of local current for various surface potentiels. Re-40

, FIGl'RE 5.3g Anale dependence of local current for various surface potentiels. Re-100, scc.O.l . FIG'-RE 5.3h Angle dependence of local current for various surface potentiels. Re-100

, Angle dependence of local current to cvllnder in eroasflov for various Reynolds numbers. (a) Scc-l,%/?ln A .0 (b) scc-l,«^*ln A -4 (c) Scc-l,*?p*ln, p.102

, IDAlin A -0 (e) Sc -102,t?/tln A -4 (fi Sc c -10 't p /« In, p.2

, SCc-l02, 4?/t -0 -FIGURE 5.4e Angle dependence of local eurrent for various Revnolds numbers. SCc-102, FIGURE 5.4d Angle dependence of local current for various Revnolds numbers

, 13 Roodlmenslonal probe current as a fonction of Reynolds IlUllbar for varions charged partlcle Schmldt numbers for cyllnder In cross-flou et apace potentiel, FICURE 5

, 14 Nondlmenslonal probe current as a funetlon of charged partlcle Schmldt number for various Reynolds numbers for cyllnder in eross-flov et apace potentiel, FICURE 5

, FIGURE 6.7c Angle dep.»d«n« of locel current for verjous ehergad partlcle Scheddt nuobers et Re-40, t, p.2

, FIGURE 6.8 Mondlnenslonal probe current 09 a function of chsrged pertlcle Schmldt nunber for varlous surfece potentiels for .phere, Re.S . experlaents at space potentiel .R^Aj-O, cyllnder in croee-f lev.Tbeories:(l)_ -présent vork for Sec

. Frtedlender, Eaperln»mts:?s*oooDobry and Plan ? KM) fer SCc.1200 (b)eee Colline end Wllllane (1939% fer Se -0.73 (c)--experlnentel corrélation» of Jenecn and _81

, Coaperleon of local current of présent nork vith theory of Demie et el (1973) fer spbere et space potentiel «J^-O and R /Ag-0. (a) Re-20