... 3664STEINIETZONHYSTERESIS.[Sept.27,affordingapathfor the magnetism.TheseNorwayironcylin-derswerebalancedbyanequalpair of cylindersat the otherside of the iinstrument,anid the amalgamtestedthen. The dimiiensions of the testedpiece of amalgamwere,Length,4cm.Cross-section,4.45cm.2,cylinder.Althoughshowingstrongattractionagainstamagnet-pole, the .amalgamhadonlyabouttwice the permeability of air.TableXXXV.gives the magneticcharacteristic of the amal-gamcontaining11percent. of iron,with the usualdenotation,Lmetallicinduction,pmetallicreluctivity.TABLEXXXV.MAGNaTICCHARACTERISTIC OF AMALGAM OF IRON,'.FL,cbs.calc.20229094049866o76790801037750I00130769120157764:140:184761I6021I759<2180238756200265755IV220290759II24031ro7740o28o3287922803452i430036o833320374856340387879362399902[AbsoluteSatura-tion ... of threecells of storagebat-tery,givingapproxiinatelyV0-6volts. The M.Al.F. Of the continuouspart of the currentisgivenasF,,andamountedto22.93,22.2to17.8,3.415anid3.488ampere-turnspercm.respectively. The magneticinductionexcitedbythisMvl.MF.,F,,ifnoalternatingM.M.F.issuperposed,isgivenbyB.,andamountedto14.30,14.15l13.70,4.60and4.70kilo-ines of magmieticforcepercmi.trespectively.In the secondset of tests the E.M.F. of the storagebatteryfelloffsomewhat.VgivestlheE.M.F. of the alternrbator,whichwassuperposedupoli the VT6volts,involtsefective.Fgives the M.M.F. of the alterlnatinqpart of the current,in1892.1631ÆTHERFORCE AIagferreadat the sixrty-ninthmneeting of the AmericanInstitute of ElectricalEngineers,NewYork,SefStember27th,1892,Vice-PresidentHammerin the Chair.ON THE LAW OF HYSTERESIS (PART IL)ANDOTHERPHENOMENA OF THE MAGNETICCIRCUIT.BYCHARLESPROTEUSSTEINMETZ.At the sixty-thirdmeeting of thisInstituLte,onJanuary19th,1892,inapaper,"On the Law of Hysteresis,"1Ihaveshownthat the energyconvertedintoheatduringacompletecycle of nagnetizationcanbeexpressedby the empiricalformulaHT=B-l6,where±Bis the maximummagneticinductionreachedduring the eycylicprocess,and§a"coefficient of hysteresis."Ihavegiven the numericalvalues of thiscoefficient,^q,fordif-ferentmaterials,varyingforWrought-iron,between.002and0045Cast-iron.016Annealedsteel.008to.012anduptoHardenedsteel.025to.082inmanganesesteelAMagnetite.020Ihaveslhownthatthis"coefficient of hysteresis,"~,isappar-entlyindependent of the speed of reversalsinpracticallimits,be-ing the samneforslowreversalsasforrapidalternationsuptosomewhatover200comnpleteperiodspersecond. The testspub-lishedthere,coveredtlhewholerange,fromverylowmagnetiza-tion,B-80lines of magneticforcepercm.2uptosaturationsashiighasB±19,000lines of magneticforcepercm.2givingfairagreementwith the law of the 1.6thpower.UnderconditionswhereeddyorFoucaultcurrentswereinduced1.TRANSACTIONS,VO1.ix,p.1,ÆTHERFORCE ... of threecells of storagebat-tery,givingapproxiinatelyV0-6volts. The M.Al.F. Of the continuouspart of the currentisgivenasF,,andamountedto22.93,22.2to17.8,3.415anid3.488ampere-turnspercm.respectively. The magneticinductionexcitedbythisMvl.MF.,F,,ifnoalternatingM.M.F.issuperposed,isgivenbyB.,andamountedto14.30,14.15l13.70,4.60and4.70kilo-ines of magmieticforcepercmi.trespectively.In the secondset of tests the E.M.F. of the storagebatteryfelloffsomewhat.VgivestlheE.M.F. of the alternrbator,whichwassuperposedupoli the VT6volts,involtsefective.Fgives the M.M.F. of the alterlnatinqpart of the current,in1892.1631ÆTHERFORCE...