﻿Waves of Magnetic Flux along Iron Wires. 461 



Table XXI.— Specimen D. T=-0515. 



C=0790 sin ai^+0050 sin 3(^-5346) +00 >6sin 5(«*-64-86 . 

 F = /"i sin (u>t-0)+f 3 sin 3 (W-0-/3,) + /- sin 5 (wt-0-S- . 



.. 



73 



10.. 



15.. 



20.. 



25.. 



30.. 



40.. 



50.. 



GO.. 



70.. 



80.. 

 100.. 

 120., 

 140.. 

 160.. 

 170.. 

 180.. 



fv 



fjfv 



9472 



065 



7592 



077 



6700 



•0S3 



! 5193 



098 ! 



4167 



115 



! 3319 



•123 



! 2560 



•136 



1414 



153 



736 



159 



358 



•165 



1629 



•155 



78-7 



•152 



23-7 



•131 



9-76 



121 



501 



107 



292 



•099 



2-20 



•099 



1-13 



•093 



folfv 



•((12 

 •iU3 

 IH4 

 •017 

 •016 

 •019 

 (>22 

 033 

 •032 

 •039 

 •036 

 •038 

 028 

 026 

 014 

 023 

 023 

 020 



0. 



.: . 



o- 9 x -0 o . 



16 92 

 1990 

 2168 

 2515 

 27-78 

 8009 

 3216 

 3600 

 38-16 

 39-00 

 3838 

 3691 

 33-11 

 3006 



28-73 



28-26 

 26-27 

 25-65 



1980 



i4-:» 



1383 



10-83 



9-34 



S-81 



8-00 



7 "75 



659 



7 42 



8-22 



ii-33 



10-42 



11-16 



12-78 



10-25 



14 24 



14-62 



28 61 



28-83 

 23-91 

 22-3S 

 17-68 

 1750 

 1505 

 1365 

 1431 

 14-35 

 14-39 

 18-50 

 22-35 

 19-78 

 22-50 

 2S24 

 296 S 



o 



2-9ti 



4 70 



8-23 



10-86 



1317 



15-24 



1908 



2124 



2208 



21-46 



1999 



16-49 



1314 



11-81 



11-34 



9-35 



8*73 



•0304 

 0454 

 •0510 

 •0441 

 ( >4 .- 5 

 051'.' 

 ■0594 

 •0653 

 •0721 

 0789 

 •0727 



0443 

 0333 | 

 ■0269 

 •< (354 



•0596 



Table XXII.— Specimen D. Static Leak. T= x . 



Magnetizing Current. C='09I5 (obs.). 



x.. j 



F... 9775 



73 



10 15 



25 



30 40 50 60 75 90 100 ! llo 120 



7700 6517 5235 4154 3267 2542 1429 740 355 120 456 269 15S 114 



X... -0327 -0617 0439 0462 -0481 0502 -0576 '0658 0735 0723 0644 0528 -0533 0531 



specimens; and the results given in the tables show that as 

 we move away from the magnetizing coil we find (a) that 

 the ratios f-Jf\ and f h \f x first increase, then both attain a 

 maximum at approximately the same place, and after this 

 diminish, and this maximum point is the same as that at 



