the stead}' state has been established, In the discussion it will bo assumed thai the motion of the ions 1% determined wMl* by their positional and velocity eo^unhnule.s at emission and by the electric field. The hnres e\eited by flu* inns on ouch other1 and by moleeules <>t~ ;»;i:> into whose spheres of notion they may ehamv t*» penetrate an* lett <»ut ni armunt, These conditions art* reali/ed it'therunouie entrant ;*»i moderate size are experimented with m hi;*h \arna, In filler tu avoid complications arisinjj1 out <»i i'(*eotnbiu;ttion we shall also sup- pose the teni}x*ralure t'owlilious to be ».ut h that ions nf OIK* si^'n only oeenr, \Vc shall ni>w euu*«tdei the ;;ener,il pj'»tb!etu, usin|»* redantjular et»«urdiiiafes, Let thct eo-ordinatf*s ot'a p*»it»t <») the <.titt,j*e \ br* ij(r(, n aiul let an ion lu^ projeeteil fi«»iu inr( M with tlf v* !m ity t nju- pt>nents //ui?f,)*'i',f» I *et u?; seek the iutiditi«»n that lids shall strike the surface II, who »e rqn.itinu is $( i r- i «», , , » . f (^|i within an infiniteMinal lvin;j *»ix arbitraiy lun'.i.iut . ults^haie deter, mined by th<: valuta **t'Fj frf, .,rv, ,»',.,%, \ff^r elijninatnoi ul the* time tlune rctutlt two etfti.ttlott'* wliiili may be wiit 'Jlie curvt? in which the ?ais face, *!», and uill theie* fore b