8-ID
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ID Date Author Type Category Subject
  65   Tue Jun 13 15:17:06 2006 Suresh8-ID GeneralManualsKepco GPIB and 19200 Serial Card
All,

The new KEPCO we have also has a RS232 with 19200 but the GPIB is atleast 10 times or more faster (per Kepco).


Suresh
Attachment 1: 26346-r2.pdf
  64   Thu Jun 8 11:34:56 2006 Alec8-ID-ISetupsI monochromator mono beam height change with angle/energy
As the monochromatic energy selected by the new I mono is changed, the beam moves vertically by a small but not insignificant amount.

The vertical offset versus monochromator Bragg angle is given by:
deltaZ = Crystal Gap * 2 * cos(theta_Bragg) = 3.1 * 2 * cos(theta_Bragg) using the current best estimate of the gap = 3.1 mm

So to calculate the vertical change between 2 energies, just take the difference between calculations at the 2 different Bragg angles. Incidentally, the I mono Bragg angle can be retrieved from the soft motor monoth = 8idi:sm32
  63   Wed Jun 7 17:43:24 2006 Suresh8-ID-IDetectorsShutter open and close times - rough numbers
Full Frame:
OPEN_DELAY = 0.08
CLOSE_DELAY=0.08


Kinetics:
OPEN_DELAY = 0.052
CLOSE_DELAY=0.05
  62   Tue Jun 6 13:39:23 2006 xuefa li8-ID GeneralSetupsfinal diam postions
for (111):
diamth diamchi diamx diamz
17.03 -0.01 -14.35 14.24

for (220):
diamth diamchi diamx diamz
26.5 -0.85 -16.40 -15.0
  61   Sat Jun 3 15:21:09 2006 Michael Sprung8-ID GeneralSetupsmeasured flux at 8-ID-I plus misc. mirror notes
1) there seems to be a problem going negative on the mirror translation (needs further investigation)
2) for each mirror height position it is nessary to tweak the ta2fine motor
3) changed mirror height ta2_z from 12.05mm to 10.0mm. There seems to be fine structure.

FLUX NUMBERS
E_1 set = 7.45 keV and E_1 meas = 7.35 keV, 17.6mm Undulator gap
  • full mono beam flux (Si1 1000h x 1000v microns) is 7.5e12 on pind1 (493kHz at 500micro Amps/V)
  • mono beam flux through the defining slit size (Si1: 250h x 250v microns) is 1.0e12 on pind1 (335kHz at 100micro Amps/V) with the diamond crystal out.
  • mono beam flux through the defining slit size (Si1: 250h x 250v microns) is 6.7e11 on pind1 (221kHz at 100micro Amps/V) with the diamond crystal in.
  • mono beam flux through the defining slit size (Si2: 20h x 20v microns) is 4.9e09 on pind2 (80kHz at 2micro Amps/V) with diamond crystal in

E_1 set = 11.1 keV and E_1 meas = 11.0 keV, 23.8 mm undulator gap
  • mono beam flux through the defining slit size (Si1: 250h x 250v microns) is 6.7e11 on pind1 (263kHz at 100micro Amps/V) with the diamond crystal in.
  • mono beam flux through the defining slit size (Si2: 20h x 20v microns) is 4.3e09 on pind2 (93kHz at 2micro Amps/V) with diamond crystal in

E_1 set = 6.1 keV and E_1 meas = 6.0 keV, 15.67 mm undulator gap
  • mono beam flux through the defining slit size (Si1: 250h x 250v microns) is 5.8e11 on pind1 (158kHz at 100micro Amps/V) with the diamond crystal in.
  • mono beam flux through the defining slit size (Si2: 20h x 20v microns) is 2.9e09 on pind2 (40kHz at 2micro Amps/V) with diamond crystal in


E_1 set = 9.1 keV and E_1 meas = 9.0 keV, 20.1 mm undulator gap
  • mono beam flux through the defining slit size (Si1: 250h x 250v microns) is 7.7e11 on pind1 (303kHz at 100micro Amps/V) with the diamond crystal in.
  • mono beam flux through the defining slit size (Si2: 20h x 20v microns) is 4.4e09 on pind2 (88kHz at 2micro Amps/V) with diamond crystal in


E_1 set = 10.1 keV and E_1 meas = 10.0 keV, 21.8 mm undulator gap
  • mono beam flux through the defining slit size (Si1: 250h x 250v microns) is 8.2e11 on pind1 (345kHz at 100micro Amps/V) with the diamond crystal in.
  • mono beam flux through the defining slit size (Si2: 20h x 20v microns) is 4.6e09 on pind2 (97kHz at 2micro Amps/V) with diamond crystal in
  60   Fri Jun 2 18:52:18 2006 Suresh8-ID GeneralSetupsI Monochromator Commissioning results part3
The foll. things were observed while measuring images on the cool snap.

1. The beam had very bright structure at the position of ta2_z=12.3 mm and it was very close to the height of the mirror table. We shifted the height to ta2_z=10.00 mm. We found that the beam is similar over the range of 9 to 12 mm. These images are recorded and saved.

2. There is a problem in ta2_x motion. At each position of ta2_x, ta2fine had to be optimised. It was also found that ta2_x moves better in the +ve direction (moving outboard).

3. Mono beam flux was measured under the foll. conditions:

(i) 1000 um x 1000 um on Si1: 493kHz on pind1 @500 uA/V @17.6 gap (flux=7.5e12 ph/s) - diamond was out of the beam
(i) 250 um x 250 um on Si1: 336kHz on pind1 @500 uA/V @17.6 gap (flux=1.0e12 ph/s) - diamond was out of the
beam
(i) 250 um x 250 um on Si1: 221kHz on pind1 @100 uA/V @17.6 gap (flux=6.7e11 ph/s) - diamond was in the beam
  58   Fri Jun 2 13:11:48 2006 xuefa li8-ID GeneralSetupsdiam positions
Beam goes through the centers of both G- and E-beamline. Here are the positions of the D-Mono:

For G-line (111)

diamth : 17.01
diamchi : 0.17
diamx : -14.30
diamz : 14.24
Flux : 1.5x10^12 photons/s


For E-line (220)

diamth : 26.43
diamchi : -0.45
diamx : -16.30
diamz : -15.00
Flux : 5.0x10^11 photons/s
  57   Thu Jun 1 19:13:30 2006 Michael Sprung8-ID GeneralSetupsI Monochromator commissioning results - part 2
1) Encountered a problem with the nano motion stage while trying do measure a table to convert the translation [mm] to angle [deg.]. It seems that the "PID" parameter for the stage are not optimal yet. A reduction of the position gain seemed to improve the scanning behavior, but this not the final solution yet. Needs further investigation.

2) Replace gonio1 motor driver in the D station. After this replacement we were able to get beam at the E setup. However, before we found the defective motor driver,we moved already the E Be window. The right slit1 position has still to found for this beamline.

3) an energy calibration has be done between 5.99 keV (Cr) to 9.66 keV (Zn). A preliminary analysis indicates that it is easily possible to create pseudo motors for the monochromator energy and monochromator bragg angles.
Attachment 1: translation2angle_conversion_table.txt
Element   x-ray energy [eV]   Undulator gap [mm]   Ge(111) bragg angle [deg]   measured translation [mm]

normal    ~7350(7450 und)     17.60                14.96                       -5.55

Cr        5989                tbd                  18.48                       +8.64
Mn        6539                tbd                  16.87                       +2.20
Fe        7112                tbd                  15.48                       -3.52
Co        7709                18.26                14.25                       -8.52
Ni        8333                tbd                  13.17                       -12.92
Cu        8979                tbd                  12.20                       -16.85
Zn        9659                tbd                  11.33                       -20.39

a conversion between bragg angle [deg.] to translation [mm] can be done by:

alpha [deg.] = 0.24517 * translation [mm] + 16.334
  56   Wed May 31 13:58:44 2006 Michael and Suresh8-ID-ISetupsMono Beam Table Positions - May 2006
The pseudo channel cut mono was aligned to mono beam. The table heights were set using transit and the table-z positions are as follows:

Pink beam was aligned to the nominal pink beam mark on the floor. In order to do this, ta2fine was reduced in angle by 45 microrad. Beam was found on G line (Si(111)) with these settings but we could not find the beam on the E line yet (Si(220)) and needs further investigation by making sure the slit ss1 is not blocking the beam.

mono beam table heights:
ti1_z : 6.25 mm [si1 250 x 250 microns]
ti2_z : 23.00 mm
ti3_z : 28.70 mm
ti4_z : 14.35 mm
pink beam offsets: ti1_z : -3.00 mm ti2_z : -6.05 mm ti3_z : -6.05 mm ti4_z : -6.05 mm After switching from pink beam to mono beam it was found that the center of mass positions were within less than 30 microns horizontally (Si1 250 (h) x 2000 (v) microns). horizontal positions (pind1 & pind2 centered on beam): ti1_x : 5.87 mm ti2_x : - 3.00 mm bewinx : - 7.50 mm si1x : -17.50 mm filterx: - 3.00 mm ti3_x : 6.50 mm ti4_x : 13.12 mm Thursday: a) removed twist of monochromator table; the upstream end was moved outboard by 1.75 mm
  55   Wed May 24 17:35:24 2006 Alec8-ID-EPSTemporary control of the 8-ID-G valve - Valve 11
The EPS HMI interface is not currently connected to the Valve 11 (8-ID-G) vacuum valve open and close signals. A temporary fix is to open and close this valve via EPICS (the EPS will still close this valve if necessary, it is only the HMI interface that is not working). To open and close Valve 11, do the following

1) From the HMI, Valve Control screen, Enable EPICS Valve Control

2) Use 'probe' and "Adjust"
to set the PV 8ida:V2001_4 to On (Open) and 8ida:V2001_5 to Off (Closed) ---- To open the valve
and the opposite for closing the valve
  54   Tue May 23 16:59:55 2006 Alec8-ID GeneralEPSEPS Programmer - John Servino - contact information
Code in the 8-ID EPS system is currently supported by John Servino - a consultant - from Professional Automation Services. Contact info for him is as follows:
APS extension - 2-3573 (not listed in the directory_
Cell - 847-519-1000
Pager - 708-242-6627
  53   Fri May 19 10:44:36 2006 Alec8-ID-ISetupsI Mono mapped positions and table potentiometers after coarse reposition
Mapped I optical table after rough x-ray beam alignment was completed at end of 2006-1. Mapped positions shown in word doc. Then did coarse reposition of the optical table and returned via motorized stages to mapped positions. Optical table potentiometers after this return to mapped position was complete are shown in the powerpoint slide.
Attachment 1: SurveyMapping_20060519.doc
Attachment 2: ti1_table_potentiometer_20060519.ppt
  52   Thu May 18 14:17:56 2006 Alec8-ID GeneralControls8-ID PV Archiver Delete List - 2006/05/18
Attachment 1: DELETE_8IDPVlist_20060517.txt
8ida:AD4enc1:count / ID:8:a:AD4enc1:count
08:ID:A:Tvac:CC1:Pres / ID:8:A:Tvac:CC1:Pres
08:ID:A:Tvac:CC2:Pres / ID:8:A:Tvac:CC2:Pres
08:ID:A:Tvac:CV1:Pres / ID:8:A:Tvac:CV1:Pres
08:ID:A:Tvac:CV2:Pres / ID:8:A:Tvac:CV2:Pres
8ida:D1Ch13_calc / ID:8:a:D1Ch13_calc
8ida:D1Ch13_raw / ID:8:a:D1Ch13_raw
8ida:D1Ch18_calc / ID:8:a:D1Ch18_calc
8ida:D1Ch18_raw / ID:8:a:D1Ch18_raw
8ida:D1Ch19_calc / ID:8:a:D1Ch19_calc
8ida:D1Ch19_raw / ID:8:a:D1Ch19_raw
8idd:m3 / ID:8:d:m3
8idd:m3.DVAL / ID:8:d:m3.DVAL
8idd:m4 / ID:8:d:m4
8idd:m4.DVAL / ID:8:d:m4.DVAL
8idd:m5 / ID:8:d:m5
8idd:m5.DVAL / ID:8:d:m5.DVAL
8idd:m6 / ID:8:d:m6
8idd:m6.DVAL / ID:8:d:m6.DVAL
8idd:m7 / ID:8:d:m7
8idd:m7.DVAL / ID:8:d:m7.DVAL
8idd:m8 / ID:8:d:m8
8idd:m8.DVAL / ID:8:d:m8.DVAL
8idd:m9 / ID:8:d:m9
8idd:m9.DVAL / ID:8:d:m9.DVAL
8idd:m9EncCalc / ID:8:d:m9EncCalc
8idd:sm2 / ID:8:d:sm2
8idd:sm2.DVAL / ID:8:d:sm2.DVAL
8idd:sm3 / ID:8:d:sm3
8idd:sm3.DVAL / ID:8:d:sm3.DVAL
8idd:sm4 / ID:8:d:sm4
8idd:sm4.DVAL / ID:8:d:sm4.DVAL
8idd:sm5 / ID:8:d:sm5
8idd:sm5.DVAL / ID:8:d:sm5.DVAL
8idd:sm6 / ID:8:d:sm6
8idd:sm6.DVAL / ID:8:d:sm6.DVAL
8idd:sm7 / ID:8:d:sm7
8idd:sm7.DVAL / ID:8:d:sm7.DVAL
8idd:sm8 / ID:8:d:sm8
8idd:sm8.DVAL / ID:8:d:sm8.DVAL
8idd:sm9 / ID:8:d:sm9
8idd:sm9.DVAL / ID:8:d:sm9.DVAL
8idd:sm10 / ID:8:d:sm10
8idd:sm10.DVAL / ID:8:d:sm10.DVAL
8idi:hsc1:b / ID:8:i:hsc1:b
8idi:hsc1:height / ID:8:i:hsc1:height
8idi:hsc1:t / ID:8:i:hsc1:t
8idi:hsc1:v0 / ID:8:i:hsc1:v0
8idi:hsc2:b / ID:8:i:hsc2:b
8idi:hsc2:height / ID:8:i:hsc2:height
8idi:hsc2:h0 / ID:8:i:hsc2:h0
8idi:hsc2:l / ID:8:i:hsc2:l
8idi:hsc2:r / ID:8:i:hsc2:r
8idi:hsc2:t / ID:8:i:hsc2:t
8idi:hsc2:v0 / ID:8:i:hsc2:v0
8idi:hsc2:width / ID:8:i:hsc2:width
  51   Thu May 18 14:17:18 2006 Alec8-ID GeneralControlsPV archiver add list - 2006-05-18
Attachment 1: ADD_8IDPVlist_20060517.txt
8ida:D1Ch31_calc / ID:8:a:D1Ch31_calc
8ida:D1Ch31_raw / ID:8:a:D1Ch31_raw
8ida:D1Ch32_calc / ID:8:a:D1Ch32_calc
8ida:D1Ch32_raw / ID:8:a:D1Ch32_raw
8idi:D1Ch1_calc / ID:8:i:D1Ch1_calc
8idi:D1Ch1_raw / ID:8:i:D1Ch1_raw
8idi:D1Ch2_calc / ID:8:i:D1Ch2_calc
8idi:D1Ch2_raw / ID:8:i:D1Ch2_raw
8idi:D1Ch3_calc / ID:8:i:D1Ch3_calc
8idi:D1Ch3_raw / ID:8:i:D1Ch3_raw
8idi:D1Ch4_calc / ID:8:i:D1Ch4_calc
8idi:D1Ch4_raw / ID:8:i:D1Ch4_raw
8idi:D1Ch5_calc / ID:8:i:D1Ch5_calc
8idi:D1Ch5_raw / ID:8:i:D1Ch5_raw
8idi:D1Ch13_calc / ID:8:i:D1Ch13_calc
8idi:D1Ch13_raw / ID:8:i:D1Ch13_raw
8idi:D1Ch18_calc / ID:8:i:D1Ch18_calc
8idi:D1Ch18_raw / ID:8:i:D1Ch18_raw
8idi:D1Ch21_calc / ID:8:i:D1Ch21_calc
8idi:D1Ch21_raw / ID:8:i:D1Ch21_raw
8idi:D1Ch22_calc / ID:8:i:D1Ch22_calc
8idi:D1Ch22_raw / ID:8:i:D1Ch22_raw
8idi:D1Ch24_calc / ID:8:i:D1Ch24_calc
8idi:D1Ch24_raw / ID:8:i:D1Ch24_raw
8idi:D1Ch25_calc / ID:8:i:D1Ch25_calc
8idi:D1Ch25_raw / ID:8:i:D1Ch25_raw
8idi:D1Ch27_calc / ID:8:i:D1Ch27_calc
8idi:D1Ch27_raw / ID:8:i:D1Ch27_raw
8idi:D1Ch28_calc / ID:8:i:D1Ch28_calc
8idi:D1Ch28_raw / ID:8:i:D1Ch28_raw
8idi:D1Ch29_calc / ID:8:i:D1Ch29_calc
8idi:D1Ch29_raw / ID:8:i:D1Ch29_raw
8idi:D1Ch30_calc / ID:8:i:D1Ch30_calc
8idi:D1Ch30_raw / ID:8:i:D1Ch30_raw
8idi:D1Ch31_calc / ID:8:i:D1Ch31_calc
8idi:D1Ch31_raw / ID:8:i:D1Ch31_raw
8idi:D1Ch32_calc / ID:8:i:D1Ch32_calc
8idi:D1Ch32_raw / ID:8:i:D1Ch32_raw
8idi:D1Ch33_calc / ID:8:i:D1Ch33_calc
8idi:D1Ch33_raw / ID:8:i:D1Ch33_raw
8idi:D1Ch34_calc / ID:8:i:D1Ch34_calc
8idi:D1Ch34_raw / ID:8:i:D1Ch34_raw
8idi:D1Ch35_calc / ID:8:i:D1Ch35_calc
8idi:D1Ch35_raw / ID:8:i:D1Ch35_raw
8idi:D1Ch36_calc / ID:8:i:D1Ch36_calc
8idi:D1Ch36_raw / ID:8:i:D1Ch36_raw
8idi:D1Ch37_calc / ID:8:i:D1Ch37_calc
8idi:D1Ch37_raw / ID:8:i:D1Ch37_raw
8idi:D1Ch38_calc / ID:8:i:D1Ch38_calc
8idi:D1Ch38_raw / ID:8:i:D1Ch38_raw
8idi:D1Ch40_calc / ID:8:i:D1Ch40_calc
8idi:D1Ch40_raw / ID:8:i:D1Ch40_raw
8idi:m49 / ID:8:i:m49
8idi:m49.DVAL / ID:8:i:m49.DVAL
8idi:m50 / ID:8:i:m50
8idi:m50.DVAL / ID:8:i:m50.DVAL
8idi:m51 / ID:8:i:m51
8idi:m51.DVAL / ID:8:i:m51.DVAL
8idi:m52 / ID:8:i:m52
8idi:m52.DVAL / ID:8:i:m52.DVAL
8idi:m53 / ID:8:i:m53
8idi:m53.DVAL / ID:8:i:m53.DVAL
8idi:m54 / ID:8:i:m54
8idi:m54.DVAL / ID:8:i:m54.DVAL
8idi:m55 / ID:8:i:m55
8idi:m55.DVAL / ID:8:i:m55.DVAL
8idi:m56 / ID:8:i:m56
8idi:m56.DVAL / ID:8:i:m56.DVAL
8idi:table3.AX / ID:8:i:table3.AX
8idi:table3.AY / ID:8:i:table3.AY
8idi:table3.AZ / ID:8:i:table3.AZ
8idi:table3.X / ID:8:i:table3.X
8idi:table3.Y / ID:8:i:table3.Y
8idi:table3.Z / ID:8:i:table3.Z
  50   Wed Apr 26 15:21:20 2006 Alec8-ID GeneralPresentationsNew ANL brand (2006) poster template
I have attached a poster template from Rich Fenner reflecting the new ANL brand (as of Feb. 2006 or so). I am guessing it will change soon because it does not look that polished, but in the meantime, this is what to use.
Attachment 1: APS_POSTER_TMPLT.ppt
  49   Wed Apr 26 13:17:54 2006 Alec8-ID GeneralPresentations2006/04/26 TRR Group Meeting presentation
Update presented to TRR group meeting on 4/26/06. Shutdown plans and I monochromator install update.
Attachment 1: TRR_Group_Meeting_Update_2006-04-24.ppt
Attachment 2: OldAndNewBeam.ppt
  48   Tue Apr 25 22:16:48 2006 Alec8-ID GeneralShutdown Activities2006-2 (May 2006) shutdown task list - ver 0.11
Revised shutdown task list from 8-Id Ops meeting on 4/25/2006
Attachment 1: Projects_v0-11.xls
Attachment 2: Projects_v0-11.pdf
  45   Tue Apr 4 17:07:17 2006 Larry8-ID-SetupsFeedback from Pollanen Aerogel SAXS run - March 2006
1) sg3 slits: I think you are already aware of the issue, but just in case I will re-iterate what we notice. At some point one of the blades on the sg3 slits was not moving properly (I think the sg3vgap top blade). I am pretty certain this is a communication issue not a mechanical issue, since the blade was 1mm off even though I was moving in 100 micron increments. It may be related to moving the slit blades too fast, which Michael did warn us not to do. When we hit the syncV and syncH buttons on the epics panel, and restricted our motion to 1s intervals this problem went away. However, perhaps it would make sense to figure out how fast the slits can go and then build this delay into the epics record somehow. One second move time seems rather arbitrary. If, for example, the slits work ok for ½ second it would be nice to know that so that all the scans could go twice as fast.

2) Stanford research amplifiers: We had some problems with adjusting the offset on the Stanford research amplifiers. At one point the offset on the pind4 amplifier would not allow itself to be changed. We tried all possible values up to 100 micro-amp offset, and so no difference. Finally we swapped amplifiers between pind4 and the pdbs and this seemed to fix the problem. Perhaps I once saw this problem with the pdbs amplifier as well. I think this is an epics record problem.

3) Beamstop. We had to modify your beamstop to put a lead block over the end so that we could get to smaller Q. The present design has the problem that the wires for the beamstop block part of the pattern. You probably shouldn’t leave our lead tape on there permanently since it could fall off. Perhaps you should make a permanent fixture with a triangular shaped block which would allow a wide angular access at small Q.

4) USAXS: We were particularly happy that we could get down to Q’s of around 6e-4 inv. ang. To do this we had to use the sg1 as the defining slit set to 100 microns, the sg2 as a trim slit set to 200 microns and the sg3 as a second trim set to 250 microns. This gave a beautiful, slit scatter free pattern down to within 4 pixels of the beam zero. We could not do this using just the sg2 and sg3’s. (I think they are just too close together)

5) MAR: The MAR worked really well. We did notice, however that there was a slight pattern in the upper central quadrant, which might have been burned in beamstop pattern from previous experiments. Also everyone seems to be leaving data on that computer. There needs to be a system to tell people to get rid of old data, and perhaps there should be a bigger hard disk. (20 gig is too small nowadays). It might be perfectly adequate (since the camera has a 3-sec readout anyway) to set up the computer to remotely mount one of the beamline disks.

6) Macros: The ccdmarseries macro doesn’t do what it is supposed to do. The camera control still opens the shutter for the dark images. I know that the common belief is that you don’t need to take darks for the MAR, but how accurately has that been tested? The fact that we could see this residual image makes me a little nervous. I certainly think it would be nice to at least have the option of measuring darks. Also, the macros for the mar at present do not mesh with the macros we use for the standard SAXS data collection macros on the I-station. Thus, you can’t set up (easily) to do a beam intensity normalization between frames, to automatically move the sample, and to dump a batchinfo file with the proper parameters. This would be nice to have. Finally, I wrote a ccdmarnewfile macro, which in the local_macros directory in case you want it.

7) Analysis software: The guys from NU were able to use the Igor based software without too much difficulty. However, it is a bit tedius to do angular averaging, since there is no equivalent to the automatic partitioning along phi which is done in Matts coherent software. I made a custom version of “coherent” that can read the mar files and do data analysis. This works, but still needs to be neatened up. I will try to improve the code and see if there is an easy way to integrate this with the main version of the software.

8) Limit switches: At one point we hit a limit switch on the samy motor. It was not possible to back of this limit except by cranking the motor by hand. This seems to me to be a bug in the epics motor record. It should allow you to move in the opposite direction of the motion limit when a limit is triggered. We can’t be the first person to have come across this issue, so there is probably a fix out there if you just know who to talk to.
  44   Tue Mar 28 17:26:39 2006 Alec8-ID-DControlsmoving diamchi, gonio1, gonio2, 8idd:sm1, 8idd:Table1
User access security has been enabled for these motors per http://8id.xor.aps.anl.gov/elog/8-ID/42.
To use these motors, you must start medm from the workstation glass.xor.aps.anl.gov and be logged in or su -l as s8idadm.
  43   Tue Mar 28 17:14:13 2006 Alec8-ID-DProblemmonochromator encoders-gonio2

Quote:
Moncohromator encoder on gonio2 does not update with moves


Problem was that gonio2 drive channel has was changed - from 8 -> 5 but the accompanying encoder cable plugged into the back of the StepPak was not moved. Once the encoder cable was moved, the encoder updated as expected.
ELOG V3.1.4-395e101