| Lines 1-4 were replaced by lines 1-3 |
| - || Instrument || field direction\\parallel to beam || field direction\\perpendicular to beam |
| - |SANS-I | 11 Tesla | * |
| - |SANS-II| * | * |
| - |AMOR | 2 Tesla* | * |
| + max. allowed Force |
| + |horizontal|200N |
| + |vertical|500N |
| Line 6 was replaced by lines 5-34 |
| - * to be reevaluated |
| + || Instrument || field direction\\parallel to beam || field direction\\perpendicular to beam || Conditions |
| + |SANS-I | 11 Tesla | 11 Tesla | without spin flipper |
| + |SANS-II| 11 Tesla | 11 Tesla | |
| + |AMOR | 2 Tesla * | * | |
| + |RITA-II| 11 Tesla | 11 Tesla | 45 deg < a2 < 100 deg, d = 450 mm |
| + (*) to be reevaluated, ask [Markus Zolliker] |
| + |
| + On all other Intruments, MA11 can not yet be used. |
| + |
| + !Remarks for SANS-II |
| + Force measurements (29.5.08): |
| + * 8 kg at 4 Tesla perpendicular |
| + * 8 kg at 5 Tesla parallel |
| + It seems that most of the force is induced by a steel ring on the valve before the detector tank. |
| + |
| + With new detector gate valve (18.8.2015), at 7.8 Tesla:\\ |
| + horizontal (beam direction) < 50 N, ~ 80 N (perpendicular), 220 N vertical\\ |
| + extrapolate forces at 11 T: 160 N horiz., 440 N vertical |
| + |
| + ! Remarks for RITA-II |
| + Monochromator sample distance at least 450 mm |
| + |
| + [MA15RitaRestrictions/SampleTableDistance.jpg]\\ |
| + How the distance has to be measured. |
| + In this example the distance is around 400 mm. |
| + |
| + Force measurements 14.7.2009 at 8 Tesla: |
| + * 10 kg horizontal |
| + * < 5 kg vertical |
| + Extrapolation for 11 Tesla: 20 kg |
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