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A18.3 Data

In this section, the data is presented. Further discussion and results are presented in section 18.4.

A18.3.1 SST-416/APL

For yoke SST-416/APL measurements of the magnetic field intensity were taken at separations of 0.10 inches in three planes (X, Y = +.1, Z), (X, Y = 0, Z) and (X, Y = -.1, Z). The data for Configuration I are presented in Figures A18-4 through A18-6 and for Configuration II in Figures A18-7 through A18-9. In the formats shown, the yoke outline indicates the outside dimensions to scale and the magnet outline is a projection onto the Y = 0 plane. Also shown in this format is the location of the solid-state detector. It can be seen that the peak field in the Y = 0 plane is 1840 Gauss at X = 0.7 inches from the front surface into the yoke.

Figure A18-4 Yoke SST 416/APL, Configuration I, Magnets 1 and 2, Y=+0.1"
Figure A18-5 Yoke SST 416/APL, Configuration I, Magnets 1 and 2, Y=0
Figure A18-6 Yoke SST 416/APL, Configuration I, Magnets 1 and 2, Y=-0.1"
Figure A18-7 Yoke SST 416/APL, Configuration II, Magnets 1 and 2, Y=+0.1"
Figure A18-8 Yoke SST 416/APL, Configuration II, Magnets 1 and 2, Y=0
Figure A18-9 Yoke SST 416/APL, Configuration II, Magnets 1 and 2, Y=-0.1"

The data is presented in a different format in Figures A18-10 through A18-12 for Configuration I and Figures A18-13 through A18-15 for Configuration II. This format is similar to the Voyager magnet presentations. Again, it can be seen that for Configuration I, the peak field is 1840 Gauss at X = 0.7 inches in the Y = 0 plane, while for configuration II the peak field is 1480 Gauss at X = 0.9 inches from the front plate. In general, the shape of the field intensity curve is similar to that of the Voyager magnets.

Figure A18-10 Yoke SST 416/APL, Configuration I, Magnets 1 and 2, Y=+0.1" , graphical form
Figure A18-11 Yoke SST 416/APL, Configuration I, Magnets 1 and 2, Y=0, graphical form
Figure A18-12 Yoke SST 416/APL, Configuration I, Magnets 1 and 2, Y=-0.1", graphical form
Figure A18-13 Yoke SST 416/APL, Configuration II, Magnets 1 and 2, Y=+0.1", graphical form
Figure A18-14 Yoke SST 416/APL, Configuration II, Magnets 1 and 2, Y=0, graphical form
Figure A18-15 Yoke SST 416/APL, Configuration II, Magnets 1 and 2, Y=-0.1", graphical form

With this yoke in Configuration I, field intensities were measured along the centerline for different pairs of magnets. This data is presented in tabular form, rather than a graph, in Table A18-1.

Table A18-1 Solar Polar Magnetic Field Survey Yoke: SST416/APL (w/o hole). Magnet configuration I. Magnetic field (Gauss)

      Magnet Pairs
X (in) Y (in) Z (in) 1 & 2 3 & 4 5 & 6 7 & 8
-0.4 0 0 28 28.4 27.8 26.1
-0.3 0 0 44 46.3 45.3 42.0
-0.2 0 0 74 76.9 75.5 69.8
-0.1 0 0 123 126 124 115
0 0 0 204 207 205 189
0.1 0 0 324 332 324 303
0.2 0 0 505 520 508 473
0.3 0 0 770 788 765 714
0.4 0 0 1080 1110 1070 1010
0.5 0 0 1420 1470 1390 1340
0.6 0 0 1720 1780 1660 1630
0.7 0 0 1840 1920 1760 1760
0.8 0 0 1720 1790 1610 1670
0.9 0 0 1330 1390 1210 1310
1.0 0 0 876 905 772 870
1.1 0 0 492 505 423 492
1.2 0 0 242 246 206 246
1.3 0 0 94.5 92.4 76.7 97.5

A18.3.2 SST-416/UCB

Yoke SST-416/UCB is similar to SST-416/APL except that it has a hole in the yoke which could accommodate a detector mount. Measurements of the magnetic field intensity were made only along the yoke centerline for Configuration I, but using the same magnet pair as used for the SST-416/APL yoke measurements. The data is presented in tabular form in Figure A18-16 and in graphical form in Figure A18-17. It can be seen that although the peak fields occur in the same location--0.7 inches from the front surface--the magnitude of SST-416/UCB is only 1750 Gauss compared to 1840 Gauss for SST-416/APL. This is probably due to an increase in leakage flux in the vicinity of the detector mounting hole and thereby a reduction in field in the center of the yoke.

Figure A18-16 Yoke SST 416/UCB, Configuration I, Magnets 1 and 2, Y=0
Figure A18-17 Yoke SST 416/UCB, Configuration I, Magnets 1 and 2, Y=0, graphical form

A18.3.3 C49/APL

Because of the high value of leakage flux from the stainless steel, a yoke of higher permeability material--Carpenter 49--was constructed. The initial C49 yoke had heavy wall thicknesses and no hole for a detector mount. The only magnetic field intensity measurements for the C49/APL yoke were made along the centerline in Configuration I. This data is presented in Figure A18-18 and in graphical form in Figure A18-19. It can be seen that the peak field value is 1890 Gauss, located at 0.7 inches from the front surface.

Figure A18-18 Carpenter 49/APL, Configuration I, Magnets 1 and 2, Y=0
Figure A18-19 Carpenter 49/APL, Configuration I, Magnets 1 and 2, Y=0, graphical form

Next: A18.3.4 C49/Mod I

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Updated 11/19/02, T. Hunt-Ward
Figure reconstruction by T. Manweiler.