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Commit a394f8c6 authored by Michal Maciejewski's avatar Michal Maciejewski
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Introduced documentation for IPDs

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.idea/lhc-sm-hwc.iml
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<module type="PYTHON_MODULE" version="4">
<component name="NewModuleRootManager">
<content url="file://$MODULE_DIR$" />
<orderEntry type="jdk" jdkName="Python 3.7 (lhc-sm-hwc)" jdkType="Python SDK" />
<orderEntry type="sourceFolder" forTests="false" />
</component>
</module>
\ No newline at end of file
600A/AN_600A_RCBXHV_FPA.ipynb
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600A/AN_600A_RCDO_FPA.ipynb
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600A/AN_600A_with_without_EE_FPA.ipynb
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README.ipynb
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......@@ -125,21 +125,150 @@
"|RQX.L2, RQX.R2, RQX.L8, RQX.R8|7180 A| 4780 A|550 A|\n",
"|RQX.L1, RQX.R1, RQX.L5, RQX.R5|6800 A| 4600 A|550 A|\n",
"\n",
"\n",
"Nominal operating currents for 7 TeV of the three PC’s as given in the LHC design report volume I. For the nominal current during HWC see EDMS 1375861.\n",
 
"\n",
 
 
"source: Test Procedure and Acceptance Criteria for the Inner Triplet Circuits in the LHC, MP3 Procedure, <a href=\"https://edms.cern.ch/document/874886/2.1\">https://edms.cern.ch/document/874886/2.1</a>\n",
"\n",
"|Type|Test|Current|Description|Notebook|Example report|\n",
 
 
"|----|----|-------|-----------|--------|--------------|\n",
"|HWC|PCC.T4|~|Power Converter Configuration part 2|AN\\_IT\\_PCCT4|-|\n",
"|HWC|PIC|~|Powering Interlock Controller check with standby current|AN\\_IT\\_PIC|-|\n",
"|HWC|PNO.D12|10% of I\\_PNO|Powering Failure at +10% of nominal current|AN\\_IT\\_PNO.D12|-|\n",
"|HWC|PNO.D13|10% of I\\_PNO|Powering Failure at -10% of nominal current|AN\\_IT\\_PNO.D13|-|\n",
"|HWC|PLI3.F6|I_PLI3|Heater Discharge Request at 2nd intermediate current (Note that I\\_RTQX1=0A|[AN\\_IT\\_PLI3.F6](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PLI3.F6.ipynb)|-|\n",
"|HWC|PNO.D14|50% of I\\_PNO|Powering Failure at +50% of nominal current during a SPA|[AN\\_IT\\_PNO.D14](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PNO.D14.ipynb)|-|\n",
"|HWC|PNO.D15|50% of I\\_PNO|Powering Failure at -50% of nominal current|AN\\_IT\\_PNO.D15|-|\n",
"|HWC|PNO.A9|I\\_PNO+I\\_DELTA|Training and plateau at nominal current|[AN\\_IT\\_PNO.A9](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PNO.A9.ipynb)|-|\n",
"|HWC|PNO.D16|90% of I\\_PNO|Powering Failure at +90% of nominal current|[AN\\_IT\\_PNO.D16](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PNO.D16.ipynb)|-|\n",
"|HWC|PNO.D17|90% of I\\_PNO|Powering Failure at -90% of nominal current|AN\\_IT\\_PNO.D17|-|\n",
"|Operation|FPA|I\\_PNO|FPA during operation with magnets quenching|[AN\\_IT\\_FPA](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_FPA.ipynb)|-|\n"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# 5. IPD - Beam Separation Dipoles D1-D4\n",
"This section is a copy of a document created by Alexandre Erokhin (https://twiki.cern.ch/twiki/pub/MP3/General_Info_IPD/separation_dipole.pdf)\n"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"|Magnets in the Circuit|Temperature|Position|General information|\n",
"|----------------------|-----------|--------|-------------------|\n",
"|MBX (D1)|1.9 K| RD1.R2, RD1.R8|I Nominal: 5800A, I_Ultimate: 6100A|\n",
"| | | |L tot: 26 mH, L per aperture: 26 mH|\n",
"| | | |max(di/dt): 17.453 A/s|\n",
"|MBRC (D2)|4.5 K| RD2.L1, RD2.R1, RD2.L5, RD2.R5|I Nominal: 4400A, I_Ultimate: 4670A|\n",
"| | | RD2.L2, RD2.R2, RD2.L8, RD2.R8|I Nominal: 6000A, I_Ultimate: 6500A|\n",
"| | | |L tot: 52 mH, L per aperture: 26 mH|\n",
"| | | |max(di/dt): 18.147 A/s|\n",
"|MBRS (D3)|4.5 K| RD3.L4, RD3.R4|I Nominal: 5520A, I_Ultimate: 6000A|\n",
"| | | |L tot: 26 mH, L per aperture: 26 mH|\n",
"| | | |max(di/dt): 18.147 A/s|\n",
"|MBRB (D4)|4.5 K| RD4.L4, RD4.R4|I Nominal: 5520A, I_Ultimate: 6000A|\n",
"| | | |L tot: 26 mH, L per aperture: 26 mH|\n",
"| | | |max(di/dt): 18.147 A/s|"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Superconducting beam separation dipoles of four different types are required in the Experimental Insertions (IR 1, 2, 5 and 8) and the RF insertion (IR 4). Single aperture dipoles D1 (MBX) and twin aperture dipoles D2 (MBRC) are utilized in the Experimental Insertions. They bring the two beams of the LHC into collision at four separate points then separate the beams again beyond the collision point. In the RF Insertions two types of twin aperture dipoles, each type with two different aperture spacings are used: D3 (MBRS) and D4 (MBRB). The D3 and D4 magnets increase the separation of the beams in IR 4 from the nominal spacing 194 mm to 420 mm. D2 and D4 are the twin apertures magnets with common iron core for both apertures. D3 is a twin apertures magnet with independent iron cores for each aperture.\n"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"The MBRC dipole consists of two individually powered apertures assembled in a common yoke structure."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"- MBX – D1 \n",
"Single aperture of the magnet powered with one power supply.\n",
"<img src=\"figures/ipd/IPD_MBX_D1.png\" width=75%>"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"- MBRC – D2 \n",
"Apertures B1 and B2 of the magnet are powered in series with one power supply.\n",
"<img src=\"figures/ipd/IPD_MBRC_D2_MBRB_D4.png\" width=75%>"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"- MBRS - D3 \n",
"Apertures B1 and B2 of the magnet are powered in series with one power supply but series connection done in the DFBA.\n",
"<img src=\"figures/ipd/IPD_MBRS_D3.png\" width=75%>"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"- MBRB – D4 \n",
"Apertures B1 and B2 of the magnet are powered in series with one power supply.\n",
"<img src=\"figures/ipd/IPD_MBRC_D2_MBRB_D4.png\" width=75%>"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Quench Detection System"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"**Quench Detector Type** \n",
"DQQDC - current leads quench detector \n",
"DQAMG - controller attached to global protection "
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"**Current Leads:**\n",
"- Typical resistance for U_RES: 7 uOhm\n",
"- Threshold for U_HTS: 3 mV, 1s\n",
"- Polarity convention: Arrows show how signals are measured. If I > 0, LD1: U_RES > 0, LD2: U_RES < 0\n",
"- PM file\n",
" - Buffer range 0 to 250, event at point 50\n",
" - Time range: -10 to 40 s\n",
" - Frequency: 5 Hz (dt = 200 ms)\n",
" \n",
"**Magnet:**\n",
"- See polarity convention in the circuit schematics\n",
"- U_RES_B1 = U_1_B1 + U_2_B1\n",
"- Threshold on U_RES_B1: 100 mV, 10 ms\n",
"- U_RES_B2, U_1_B2, U_2_B2 and U_INDUCT_B2 are given for diagnostics only\n",
"- Signals are measured with -2.5 V offset and with the gain factor = 0.0012\n",
"- *Attention: B1 signals and B2 singals can be shifted by 4 ms from each other*\n",
"- If pure inductive signal and di/dt < 0:\n",
" - U_1_B1 = L di/dt < 0\n",
" - U_2_B1 = -L di/dt < 0\n",
" \n",
"- PM file\n",
" - Buffer range 501 to 1500, event at point 1000\n",
" - Time range: -2 to 2 s\n",
" - Frequency: 250 Hz (dt = 4 ms)"
]
},
{
......@@ -275,11 +404,21 @@
"1. Select from the top menu: Kernel -> Interrupt and execute the problematic cell again (either a run button (cf. Figure above) or Ctrl+Enter).\n",
"2. In case the first option does not help, select from the top menu Kernel -> Restart & Clear Output. Thenall cells prior to the problematic one have to be executed again (multiple cell selection is possible byclicking on the left of a cell to select it and afterwards selecting others with pressed Shift button). After this operation one needs to reconnect to the NXCALS Spark cluster."
]
},
{
"\n",
"cell_type": "markdown",
"metadata": {},
"source": [
"# Analysis Notebook for Operation\n",
"Quench analysis assumptions:\n",
"1. We consider standard analysis scenarios, i.e., all signals can be queried from the respective databases. Depending on what signal is missing, an analysis can raise a warning and continue or an error and abort the analysis.\n",
"2. In case an analyzed signal can’t be queried, a particular analysis is skipped. In other words, all signals have to be available in order to perform an analysis.\n",
"3. It is recommended to execute each cell one after another. However, since the signals are queried prior to an analysis, any order of execution is allowed. In case an analysis cell is aborted, the following ones may not be executed (e.g. I_MEAS not present).\n",
"\n",
"# Analysis Workflow\n",
"\n",
"An FPA analysis workflow consists of four steps: (i) finding of an FGC Post Mortem timestamp (ii) executing analysis cells on the cluster (iii); (iv) storing output files on EOS; see Figure below.\n",
"\n",
"<center><img src=\"https://gitlab.cern.ch/LHCData/lhc-sm-hwc/raw/master/figures/fpa-analysis-workflow.png\" width=75%></center>\n",
"\n",
"The RB FPA Analysis notebook is organized into 11 chapters:\n",
......@@ -300,17 +439,17 @@
"|Analysis|Automatic (each cell executed without user input); Manual (some analysis steps take expert comment)|\n",
"|Done by|NICE login of a person executing the analysis|\n",
"|Find FGC PM entries|Button triggering a search of FGC PM entries|\n",
"|Query progress bar|Displays progress of querying days in between indicated datesFGC PM EntriesList of FGC PM timestamps|\n",
"\n",
"# Analysis Notebook for HWC\n",
"**Please note that in order to execute any of the following cells, there should be at least one entry in the FGC PM Entries list. The list is populated after clicking [Find FGC PM entries button].**\n",
"\n",
 
"Figure below shows the GUI after clicking button [Find FGC PM entries] with the default settings. Note that the list only contains FGC PM timestamps surrounded by QPS timestamps (1 minute before and 5 minutes after an FGC PM timestamp).\n",
"\n",
"<center><img src=\"https://gitlab.cern.ch/LHCData/lhc-sm-hwc/raw/master/figures/swan-rb-fpa-analysis-fgc-pm-browser.png\" width=75%></center>\n",
"\n",
 
 
"In order to avoid delays between analyses, the necessary signals are queried prior to performing the analysis.\n",
"3. Timestamps \n",
"Table of timestamps main systems representing the sequence of events for a given analysis.\n",
"4. Schematic \n",
"Interactive schematic of the RB circuit composed of: power converter, two energy extraction systems, current leads, magnets, and nQPS crates. Hovering a mouse over a center of a box representing a system provides additional pieces of information. Location of quenched magnets is highlighted. Slider below the schematic enables its scrolling.\n",
......
README.md
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......@@ -97,7 +97,7 @@ The main quadrupole magnet circuits of the 8 Inner Triplet (IT) systems in the L
<img src="https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/raw/master/figures/it/IT.png" width=75%>
Main quadrupole magnet circuit of the Inner Triplet system for IT’s at points 1 and 5 (left) and IT’s at points 2 and 8 (right).
Note that the configuration for the IT’s in points 1 and 5 is different from the configuration in points 2 and 8. An earth detection system is present at the minus of the RTQX2 converter. Detailed information concerning the converters is given in EDMS 1054483.
Note that the configuration for the IT’s in points 1 and 5 is different from the configuration in points 2 and 8. An earth detection system is present at the minus of the RTQX2 converter. Detailed information concerning the converters is given in EDMS 1054483.
The two magnets Q1 and Q3 are type MQXA and the two combined magnets Q2a and Q2b are type MQXB. Q1 is located towards the interaction point.
......@@ -121,11 +121,11 @@ source: Test Procedure and Acceptance Criteria for the Inner Triplet Circuits in
|HWC|PIC|~|Powering Interlock Controller check with standby current|AN\_IT\_PIC|-|
|HWC|PNO.D12|10% of I\_PNO|Powering Failure at +10% of nominal current|AN\_IT\_PNO.D12|-|
|HWC|PNO.D13|10% of I\_PNO|Powering Failure at -10% of nominal current|AN\_IT\_PNO.D13|-|
|HWC|PLI3.F6|I_PLI3|Heater Discharge Request at 2nd intermediate current (Note that I\_RTQX1=0A|AN\_IT\_PNO.F6|-|
|HWC|PNO.D14|50% of I\_PNO|Powering Failure at +50% of nominal current during a SPA|AN\_IT\_PNO.D14|-|
|HWC|PLI3.F6|I_PLI3|Heater Discharge Request at 2nd intermediate current (Note that I\_RTQX1=0A|[AN\_IT\_PLI3.F6](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PLI3.F6.ipynb)|-|
|HWC|PNO.D14|50% of I\_PNO|Powering Failure at +50% of nominal current during a SPA|[AN\_IT\_PNO.D14](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PNO.D14.ipynb)|-|
|HWC|PNO.D15|50% of I\_PNO|Powering Failure at -50% of nominal current|AN\_IT\_PNO.D15|-|
|HWC|PNO.A9|I\_PNO+I\_DELTA|Training and plateau at nominal current|AN\_IT\_PNO.A9|-|
|HWC|PNO.D16|90% of I\_PNO|Powering Failure at +90% of nominal current|AN\_IT\_PNO.D16|-|
|HWC|PNO.A9|I\_PNO+I\_DELTA|Training and plateau at nominal current|[AN\_IT\_PNO.A9](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PNO.A9.ipynb)|-|
|HWC|PNO.D16|90% of I\_PNO|Powering Failure at +90% of nominal current|[AN\_IT\_PNO.D16](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_PNO.D16.ipynb)|-|
|HWC|PNO.D17|90% of I\_PNO|Powering Failure at -90% of nominal current|AN\_IT\_PNO.D17|-|
|Operation|FPA|I\_PNO|FPA during operation with magnets quenching|[AN\_IT\_FPA](https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/blob/master/it/AN_IT_FPA.ipynb)|-|
......@@ -267,7 +267,17 @@ The RQ analysis notebook follows the same structure except for the lack of schem
### Notebook Output
The notebook creates three output files in the folder //cern.ch/eos/project/l/lhcsm/operation/RB/circuit_name/\*}, e.g., //cern.ch/eos/project/l/lhcsm/operation/RB/RB.A12/\*:
The notebook creates three output files in the folder (path with Windows convention)
```
\\cernbox-smb\eos\project\l\operation\$circuit_type$\$circuit_name$\
```
e.g.,
```
\\cernbox-smb\eos\project\l\lhcsm\operation\RB\RB.A12\
```
- HTML report file with the snapshot of the entire notebook - [fgc-timestamp]-[analysis-execution-date]-[notebook-name]\_report.html;
- CSV file with MP3 results table with a subset analysis results - [fgc-timestamp]-[analysis-execution-date]-[notebook-name]\_mp3\_results\_table.csv};
- CSV file with full results table - [fgc-timestamp]-[analysis-execution-date]-[notebook-name]\_results_table.csv};
......@@ -290,13 +300,13 @@ The remainder of each notebook depends on the particular test to be performed. A
## Notebook Output
The notebook creates three output files in the folder
The notebook creates three output files in the folder (path with Windows convention)
```
//cern.ch/eos/project/l/lhcsm/hwc/RB/ circuit_name/hwc_test/hwc_campaign/*,
\\cernbox-smb\eos\project\l\lhcsm\hwc\$circuit_type$\$circuit_name$\$hwc_test$\$hwc_campaign$\,
```
e.g.,
```
//cern.ch/eos/project/l/lhcsm/hwc/ RB/RB.A12/PNO.b2/HWC_2014/*:
\\cernbox-smb\eos\project\l\lhcsm\hwc\RB\RB.A12\PNO.b2\HWC_2014\:
```
- HTML report file with the snapshot of the entire notebook - [test-start]-[test-end]\_report.html;
......
ipd/AN_IPD_FPA.ipynb 0 → 100644
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{
"cells": [
{
"cell_type": "code",
"execution_count": null,
ipd/IPD_Run2.txt 0 → 100644
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,Circuit name,Date,Time,Status
RD2.R8,31/01/2015,08:45:08,
RD2.R8,31/01/2015,16:51:10,
RD2.R2,31/01/2015,10:06:31,
RD2.L1,10/02/2015,20:52:00,
RD1.R2,10/02/2015,21:55:16,
RD1.L2,15/02/2015,08:00:22,
RD2.R1,14/02/2015,17:38:22,
RD2.L8,15/02/2015,10:24:41,
RD2.L1,14/02/2015,08:25:38,
RD2.L2,27/02/2015,08:17:58,
RD4.L4,27/02/2015,20:46:40,
RD3.L4,28/02/2015,07:59:06,
RD3.L4,28/02/2015,12:23:47,
RD4.L4,28/02/2015,14:22:45,
RD1.R8,28/02/2015,16:19:30,
RD3.L4,28/02/2015,21:09:40,
RD4.R4,07/03/2015,01:48:29,
RD2.L5,15/03/2015,08:15:58,
RD4.R4,09/03/2015,23:23:14,
RD2.R5,10/03/2015,17:00:20,
RD2.R8,25/04/2015,04:46:41,
RD2.L5,15/06/2015,14:28:29,
RD2.L1,15/06/2015,14:28:29,
RD2.R5,15/06/2015,14:28:29,
RD4.R4,06/03/2016,10:53:39,
RD2.R8,29/04/2016,05:32:16,
RD2.R5,08/08/2017,13:42:07,
RD2.L8,03/12/2018,13:13:07,
RD3.R4,03/12/2018,13:59:59,
\ No newline at end of file
ipq/PC.ipynb
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it/AN_IT_FPA.ipynb
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it/AN_IT_PLI3.F6.ipynb
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......@@ -26,14 +26,16 @@
 
 
### PLI3.F6: RQX and RTQX2, Heater Discharge Request
The aim of this test is to check the performance of the QPS system during a heater induced quench. In 2-converter configuration the test is done with current in the RQX and RTQX2 converters, while the RTQX1 converter is not connected, but turned ON in voltage mode. In 3-converter configuration the RTQX1 converter is connected but not powered, see figures below.
 
<img src="../figures/it/PLI3.F6_current_pcs.png" width=75%>
<img src="../figures/it/PLI3.F6_current_magnets.png" width=75%>
<img src="https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/raw/master/figures/it/PLI3.F6_current_pcs.png" width=75%>
<img src="https://gitlab.cern.ch/LHCData/lhc-sm-hwc/-/raw/master/figures/it/PLI3.F6_current_magnets.png" width=75%>
 
Currents vs time for test PLI3.F6. The RTQX1 converter is only connected if the test is performed in 3-converter configuration. Note that the current in Q1 is equal to the current in Q3.
<center>Currents vs time for test PLI3.F6. The RTQX1 converter is only connected if the test is performed in 3-converter configuration. Note that the current in Q1 is equal to the current in Q3.</center>
The offline analysis is given in the table below:
 
|Responsible|Type of analysis|Criteria|
|-----------|----------------|--------|
|PC|Verification of the voltage and current of RQX, RTQX2, RTQX1 (if in 3-converter configuration) during the quench. Check that the three converters are in FAULT (PIC_FASTPA)|-|
|MP3|Verify the heater discharge and delays|U_HDS_1-8 within 5% of the reference signals.|
......@@ -83,11 +85,11 @@
from lhcsmapi.Time import Time
from lhcsmapi.Timer import Timer
from lhcsmapi.pyedsl.QueryBuilder import QueryBuilder
from lhcsmapi.analysis.ItCircuitQuery import ItCircuitQuery
from lhcsmapi.analysis.ItCircuitAnalysis import ItCircuitAnalysis
from lhcsmapi.analysis.CircuitAnalysis import get_expert_decision
from lhcsmapi.analysis.expert_input import get_expert_decision
 
# GUI
from lhcsmapi.gui.qh.DateTimeBaseModule import DateTimeBaseModule
from lhcsmapi.gui.pc.FgcPmSearchModuleMediator import FgcPmSearchModuleMediator
from lhcsmapi.gui.pc.ItFgcPmSearchBaseModule import ItFgcPmSearchBaseModule
......
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