Reference
Installation
Nothing special provided. See the header of this file for dependencies and download as needed. Note that jquery-ui, multisortable, and jrbWidgets are used by the designer.
Use
myOutputPivoted = jrbAnalytics.getGlobal('model.pivot')(myInputData, myParams);
where
myInputData and
myOutputPivoted are jrbAnalytics data objects, and
myParams is the configuration JSON (see below). Note that myParams IS MODIFIED with a '__ErrorMessages' object that displays in clear text configuration errors identified. Non-matching field or function names for example.
Helper functions:
myInputData = jrbAnalytics.getGlobal('utils.objectifyTable')(myTable);
where
myTable is a normal table object with a [{fieldName1:value1, fieldName2:value2, ..., {..}, ...] format;
jrbAnalytics.getGlobal('utils.renderSimpleTable')('someDIVid', myInputData);
renders an HTML table of a jrbAnalytics data object.
To use with the designer:
myParams = {}; //or preset with a configuration
jrbAnalytics.getGlobal('model.pivot')(myInputData, myParams, divIDtoLoadDesigner);
With the designer, at any time 'myParams.draftpivotconfig' contains the draft configuration.
Creating the configuration JSON
Option 1: Use the Designer
Use of the designer is recommended as the quickest way to construct the JSON object correctly and to obtain the view you want. Use the full
jrbAnalytics example to upload your own data. Or copy this and all dependent files to a local directory. Change the 'myTable' variable to use your data set. The examples tabs will stop working, but the designer will not. Then click on the 'Show used Parameters' to see the JSON paramters used, which can be cut and pasted.
Option 2: Construct by hand
Pass a JSON Object in this format:
{
pivotconfig: pivotConfigObject
}
where
pivotConfigObject is a JSON object that contains items as follows.
| dataNames | ['field name 1', 'field name 2'] | Optional but usually needed. Array of column names that contain the data being pivoted. Usually numeric, but not always. Order of names used to determines order of output columns. |
| columnNames | ['field name 1', 'field name 2'] | Optional. Array of column names to use to populate the column headers. Usually text, but not always. Order determines hierarchy, or how data is nested. |
| rowNames | ['field name 1', 'field name 2'] | Optional. Array of column names to use to populate the row headers. Usually text, but not always. Order determines hierarchy, or how data is nested. |
| pivotFn | string of function name | Optional. Examples are 'Sum' or 'Count', 'List', 'Unique List', 'Max', 'Min', 'Mean', 'mode', 'Median', 'Product', Variance', 'StdDev' also available. 'None', invalid values or not providing this parameter result in the same none operation on the pivoted data array. You can add your own functions with the following simple extension. See start of jrbPivot.js for existing examples:
jA.extendGlobalObject('model.pivotfunctions', {
SumPlusOne: function(arrin) { return math.sum(arrin) + 1; }, //note math.js function here
CountMinusOne: function(arrin) { return arrin.length - 1; }, //note math.js function here
myFunctionName: function(arrin) { --insert calculation then -- return result; }, //modify as needed
});
|
| pivotEmpty | any value | Optional. What to use for pivoted cells that contain no data. If not set, 'undefined' will be used. A 0 or '' may be more useful. |
| cleandata | boolean, true or false | Optional but highly recommended.Interpreted as false if missing. When set, the pivot function excludes null, undefined or empty strings ('') in the input data from being pivoted. So for example this pivoted data [1, 4, '', '', 3] contains 5 items and fails to sum without cleadata set, whereas when set the data reduces to [1, 4, 3] contains 3 items and will sum. |
| options | options object | See below. Optional but needed for more useful pivoting actions. This object defines more specific filter, sort, data collation functions, and row and column summary and sub-summary functions (e.g. 'Sum' for totals and sub-totals). |
options object
a JSON Object in this format:
{
'field name': {
'action': {
'sub-action': subActionValue,
//..additional sub actions
},
//..additional actions
},
//additional field names
}
where
- 'field name' is one of the field (or column) names of the input data, OR one of '__rowTotals', '__colTotals' that are used to add overall summary rows or columns (grand totals for example).
- 'action' is one of the following: 'filter', 'msort', 'sort', 'summary', 'summarytype'. Not every action is relevant to every 'field name' as follows:
- 'filter' applies to anything except '__rowTotals' and '__colTotals'.
- 'msort', 'sort', 'summary' applies to all row and column field names. I.e. 'field name' must appear in rowNames or columnNames above.
- Additionally 'summary' applies to '__rowTotals', '__colTotals'. These are the only actions permitted for these 'field names'.
- 'summarytype' applies to data field names only. I.e. 'field name' must appear in dataNames above.
- 'sub-action' is one of the following: 'in', 'sort', 'msort', 'topOrleft', 'rightOrbottom'. 'sub-action' is related to 'action' as follows:
- 'in' - use with 'filter' action only. 'subActionValue' is an array of values to be included in the pivot.
- 'msort' - use with 'msort' action only. 'subActionValue' is an array of field values to set sort order. Over-ridden if sort is set.
- 'sort' - use with 'sort' action only. 'subActionValue' is an array with one string that defines the sort action. See below.
- 'topOrleft', 'rightOrbottom' - use with 'summary'. 'subActionValue' is an array of pivot function names (same used used in pivotFn above) with 'Summary' an additional value that is also permitted. This defines the functions and the order to use to create row or column summary lines (e.g. 'Sum' for a sub-total). Using 'Summary' as a function name means that the function used will be the same as that used by the data field names (and is recommended else results can get confusing). If not obvious 'topOrleft' means summary rows displayed above or summary columns displayed to the left the respective data set. 'rightOrbottom' means summary rows displayed below or summary columns displayed to the right the respective data set.
- 'summarytype' - use with 'summarytype' action only. 'subActionValue' is an array of pivot function names (same used used in pivotFn above) to use on the collated data in each cell in the order specified in the array. Overrides the 'pivotFn' default.
Note in the output of the pivot designer, you'll also see a 'summary_sort' or 'summarytype_sort' 'action'. You can ignore these. Used by the designer UI only to remember sort actions.
Sort Strings
for the 'sort' action and subaction, a string is parsed to determine how data rows or columns should be sorted. The string is the same as that used in the sort dropdowns in the designer and has the following format:
[order] + ' - ' + [Column name] + [' ('+function+')']
[order] is simply one of 'Descending' or 'Ascending'. The column name must be that of a data column name OR be the same as 'field name' under which the 'sort' action is placed. The function in brackets is only used with data column names and must match one of the functions being used.


Uninformed Search Techniques
Informed Search Techniques
Generating solutions from observed data
- Set of Goals
- Set of Objects
- Set of Operations
All valid states using operations on objects
- Search for solution in problem space
- Example: DFS, BFS,...
Actions: PICKUP, PUTDOWN, FORWARD, BACKWARD, LEFT, RIGHT
Condition-1: Only top ring can be moved at a time
Condition-2: Smaller ring cannot be below the large one
- Direct Graph
- Start from Initial State
- Use operations
- Check Goal State
- Blind Search
- Only Problem Defintion
- No idea if one non-goal state is better than other
- Visit all the nodes in a a certain order for pre-defined goal
- No cleverness
- No guarantee of reaching goal state
Less Ineffective than Informed Search
- Proceed level by level down the tree
- Start from root node and explore all the children, left to right
- If no solution found, expand the first(leftmost) child, then second at same depth,...
- Place start node at the end of queue
- Examine the node at the front of queue, then
Queue
Complete? Yes! Always reaches GOAL
Time? O(b^d):: Number of nodes generated
Space? O(b^d):: Keeps every node in the memory
Optimal? Yes! except deeper solutions
Branching Factor=b and goal found at depth=d
Space is more problem than time.
- Proceed down a single branch at a time
- Expand root node, then leftmost child of the root, then leftmost child of that node,..
Stack (LIFO)
Complete? No! Fails in infinite depth :: A-B-C-A
Time? O(b^m):: Maximum depth
Space? O(b*m):: Linear Space
Optimal? NO! except deeper solutions
Can go to wrong branch and may take very long time to find solution
- Optimized DFS
- Perform DFS but only at a specified depth L
- The path length is at max L
Complete? No! Solution may be beyond depth level
Time? O(b^L):: Maximum depth
Space? O(b*L):: Linear Space
Optimal? NO!
- Domain Specific Information
- Heuristic Function h(n) : Goodness of a node n
h(n) = estimated cost of minimal cost path from n to goal state
- Uses evaluation function f(n) to select a node for expansion
- Node with lowest evaluation function is expanded first
Use an evaluation function for each node -> desirability
- Greedy Best First Search
- A* Search
- tries to get as close as it can to the goal
- expands the node that appears closest to the goal
- Uses only heuristic function
Evaluation function h(n) = estimate of cost from n to closest goal
Example: hsld(n) = straight-line distance from n to goal
f(n) = h(n)
h(n) = 0 for goal state
Complete? NO! Can get stuck in loops
Time? O(b^m):: depends on good heuristic
Space? O(b^m):: Keeps all nodes in memory
Optimal? NO!
evaluation function f(n) = g(n) + h(n)
g(n) = cost so far to reach n
estimated cost from n to goal
Complete? YES!
Time? Exponential
Space? Keeps all nodes in memory
Optimal? YES!
Competitive Environments in which the agents goals are in conflict
- Often known as games
- Initial State
- A successor function
- A terminal test
- A Utility function
Opposition between agent's Utility functions
- depth first search with limited depth
- Static evaluation function for all leaf nodes
- assume opponent will make the best move possible
- Optimized MiniMax
- Instead of expanding nodes, we try to infer based on node values
- Depends on the order on how nodes are expanded
Alpha -> value of best choice so far for MAX (highest value)
Beta -> value of best choice so far for MIN (lowest value)
Each node keeps track of [alpha, beta]
Alpha -> -INF
Beta -> +INF
Research


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Fig. 1
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Nature of projected Arctic amplification. Surface temperatur ... |
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Fig. 2
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Ensemble mean and standard deviation of Arctic climate chang ... |
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Fig. 3
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Seasonality of partial temperature contributions. Seasonal c ... |
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Fig. 4
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Spatial variablity of partial temperature contributions. Ens ... |
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Fig. 5
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Relationship between regional warming pattern and individual ... |
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Fig. 6
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Local and remote Arctic amplification processes. The local a ... |
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Fig. 7
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Energy transfer and Arctic amplification. a Correlation betw ... |
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Fig. 8
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Dispersal of energy from sea ice retreat regions to the broa ... |
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Fig. 9
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Implications of changes in ocean mixed layer depth. Relation ... |


This is a Demo of a MVC application, using Spring boot framework. This application is connected to a PostgreSQL database by a JDBC driver. These two components are hosted on Heroku.
Here is the list of used tools :
Get List of Users : Link
Create a User : Link
Authors :
PROUVOST Chloé
VIOZELANGE Quentin


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"Great old castles full of dreams, Transcending all the mystical sins, Buried deep under meadows green, It was defeat never seen." - Srijanak De
Thanks for visiting my webpage.


|
Standard Reference Data Program |
Data Gateway |
Chemistry WebBook |
|
NIST subscription sites provide data under the NIST Standard Reference Data Program, but require an annual fee to access. The purpose of the fee is to recover costs associated with the development of data collections included in such sites. Your institution may already be a subscriber. Follow the links above to find out more about the data in these sites and their terms of usage.
Go To: Top, Constants of diatomic molecules, References, Notes / Error Report
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data evaluated as indicated in comments:
HL - E.P. Hunter and S.G. Lias
L - S.G. Lias
Data compiled as indicated in comments:
LLK - S.G. Lias, R.D. Levin, and S.A. Kafafi
RDSH - H.M. Rosenstock, K. Draxl, B.W. Steiner, and J.T. Herron
| Quantity | Value | Units | Method | Reference | Comment |
|---|---|---|---|---|---|
| IE (evaluated) | 11.49 ± 0.20 | eV | N/A | N/A | L |
| Quantity | Value | Units | Method | Reference | Comment |
| Proton affinity (review) | 777.8 | kJ/mol | N/A | Hunter and Lias, 1998 | at O; HL |
| Proton affinity (review) | 533. | kJ/mol | N/A | Hunter and Lias, 1998 | at Si; HL |
| Quantity | Value | Units | Method | Reference | Comment |
| Gas basicity | 750.4 | kJ/mol | N/A | Hunter and Lias, 1998 | at O; HL |
| Gas basicity | 500.5 | kJ/mol | N/A | Hunter and Lias, 1998 | at Si; HL |
| IE (eV) | Method | Reference | Comment |
|---|---|---|---|
| 11.3 ± 0.2 | EI | Nakagawa, Asano, et al., 1981 | LLK |
| 11.43 | EVAL | Huber and Herzberg, 1979 | LLK |
| 10.2 ± 0.5 | EI | Thompson, 1973 | LLK |
| 11.3 ± 0.3 | EI | Stearns and Kohl, 1973 | LLK |
| 11.3 ± 0.5 | EI | Muenow, 1973 | LLK |
| 11.5 ± 0.3 | EI | Hildenbrand, 1972 | LLK |
| 11.58 ± 0.10 | EI | Hildenbrand, 1971 | LLK |
| 11.6 ± 0.2 | EI | Hildenbrand and Murad, 1969 | RDSH |
| ~11.67 | S | Hildenbrand and Murad, 1969 | RDSH |
Go To: Top, Gas phase ion energetics data, References, Notes / Error Report
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Data compiled by: K.P. Huber and G. Herzberg
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Theoretical potential curves and spectroscopic constants for the ground and several valence excited states Heil and Schaefer, 1972 Oddershede and Elander, 1976. | ||||||||||||
| P 1Σ+ (5pσ) | 82019 | [1121.5] Z | [0.692] | 1 | [1.547] | P ← X 2 R | 81960.3 Z | |||||
| missing citation | ||||||||||||
| O 1Π | [82208.1] | [0.556] | 3 | [1.726] | O ← X R | 81588.8 Z | ||||||
| Lagerqvist, Renhorn, et al., 1973 | ||||||||||||
| N 1Π | (81232) | [(1024)] | [0.635] | 4 | [1.615] | N ← X R | 81124.8 Z | |||||
| Lagerqvist, Renhorn, et al., 1973 | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| M 1Π | 81203 | [833] | [0.640] | 5 | [1.609] | M ← X 2 R | 81000.5 Z | |||||
| Lagerqvist, Renhorn, et al., 1973 | ||||||||||||
| L 1Σ+ (5sσ) | 80783 | [1102.2] Z | [0.701] | 6 | [1.537] | L ← X 2 R | 80715.3 Z | |||||
| missing citation | ||||||||||||
| K 1Σ+ | 78369 | [905.8] Z | i | [0.615] | 7 | [1.641] | K ← X 2 R | 78202.6 Z | ||||
| Lagerqvist, Renhorn, et al., 1973 | ||||||||||||
| J 1Π (4pπ) | 76381 | [1146] | [0.6983] | 8 | [1.5402] | J ← X 2 R | 76334.3 Z | |||||
| missing citation | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| h 3Πi | (70790) 9 | (431) 9 | ~0.589 B1 | ~1.677 r1 | ||||||||
| Lagerqvist and Renhorn, 1974 | ||||||||||||
| I 1Π | (70510) | [878.9] Z | 10 | [0.614] 10 | [1.643] | I ← X R | 70333.7 Z | |||||
| Lagerqvist, Renhorn, et al., 1973 | ||||||||||||
| H 1Σ+ (4pσ) | 69727 | [1109.25] Z | 0.7146 | 0.0094 11 | 1.5225 | H ← X 2 R | 69662.26 Z | |||||
| missing citation; missing citation | ||||||||||||
| G 1Π | (69670) | [862.88] Z | 10 | [0.6292] | 10 | [1.2E-6] | [1.6226] | G ← X R | 69483.06 Z | |||
| missing citation | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| F 1Σ+ (4sσ) | 68532.0 | 1120.00 12 Z | 7.345 12 | [0.6938] | 13 | [1.5452] | F ← X 2 R | 68470.90 Z | ||||
| missing citation; missing citation | ||||||||||||
| Many unidentified emission bands in the region 21800 - 31500 cm-1. | ||||||||||||
| g 3Σ+ (4sσ) | [68091.4] | [0.71588] | [1.42E-6] | [1.52116] | g → b V | 33567.95 Z | ||||||
| missing citation | ||||||||||||
| 33639.01 Z | ||||||||||||
| 33711.59 Z | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| f 3Πi | 59283.1 | 488.4 14 | 3.4 | 0.586 14 | 0.0145 | 3E-6 | 1.681 | f → b R | 25146.6 H | |||
| missing citation; Bredohl, Cornet, et al., 1975; Shanker, Linton, et al., 1976 | ||||||||||||
| 59260.8 | 488.4 14 | 3.4 | 0.586 14 | 0.0145 | 3E-6 | 1.681 | f → b R | 25051.7 H | ||||
| missing citation; Bredohl, Cornet, et al., 1975; Shanker, Linton, et al., 1976 | ||||||||||||
| 59236.8 | 488.4 14 | 3.4 | 0.586 14 | 0.0145 | 3E-6 | 1.681 | f → b R | 24956.7 H | ||||
| missing citation; Bredohl, Cornet, et al., 1975; Shanker, Linton, et al., 1976 | ||||||||||||
| c 3Σ(+) | 57551.3 | 949.10 H | 17.30 | 0.6841 15 | 0.0079 | 1.7E-6 | 1.5561 | c → b VR | 23498.05 Z | |||
| missing citation; Singh, Bredohl, et al., 1974; Shanker, Linton, et al., 1976 | ||||||||||||
| 23569.11 Z | ||||||||||||
| 23641.69 Z | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| E 1Σ+ | 52860.9 | 675.52 Z | 4.204 | 0.54727 16 | 0.00555 | 0.000022 | 1.434E-6 | 0.018E-6 | 1.73978 | E ↔ X 17 18 R | 52578.31 Z | |
| missing citation; Barrow and Stone, 1975; missing citation | ||||||||||||
| A 1Π | 42835.4 | 852.8 Z | 6.43 19 | .0238 19 | 0.6307 20 21 | 0.00660 | 1.43E-6 | 1.6206 | A ↔ X 22 23 R | 42640.71 Z | ||
| missing citation; Singh, Upadhya, et al., 1969; missing citation; missing citation; missing citation; missing citation | ||||||||||||
| D 1Δ | 38823 24 | 730 | 3.9 | 0.5538 21 | 0.00516 | 1.729 | ||||||
| C 1Σ- | 38624 24 | 740 | 4.27 | 0.5555 21 | (0.0052) | 1.727 | ||||||
| e 3Σ- | 38309 24 | 748 | 4.19 | 0.5563 | 0.00515 | 1.726 | ||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| d 3Δr | 36487 24 25 | 767 | 4.1 | 0.5631 | (0.0052) | 1.715 | ||||||
| b 3Π2 | 34018.5 | 1013.8 (Z) | 7.57 | [0.68920] 26 | 0.00440 | [2.22E-6] | 1.5624 | b → X R | 33904.20 Z | |||
| Bredohl, Cornet, et al., 1974; Hager, Wilson, et al., 1974; Hager, Harris, et al., 1975; Linton and Capelle, 1977 | ||||||||||||
| b 3Π1 | 33947.4 27 | 1013.8 (Z) | 7.57 | [0.67607] ]26 21 | 0.00440 | [1.25E-6] | 1.5624 | b → X R | 33833.14 Z | |||
| Bredohl, Cornet, et al., 1974; Hager, Wilson, et al., 1974; Hager, Harris, et al., 1975; Linton and Capelle, 1977 | ||||||||||||
| b 3Π0 | 33874.8 | 1013.8 (Z) | 7.57 | [0.66386] 26 | 0.00440 | [0.50E-6] | 1.5624 | b → X R | 33760.56 Z | |||
| Bredohl, Cornet, et al., 1974; Hager, Wilson, et al., 1974; Hager, Harris, et al., 1975; Linton and Capelle, 1977 | ||||||||||||
| State | Te | ωe | ωexe | ωeye | Be | αe | γe | De | βe | re | Trans. | ν00 |
| a 3Σ+ | (33630) | (790) 28 | (4.1) 28 | (0.57) 28 21 | (0.0052) 28 | (1.70) 28 | a → X R | 33409 H | ||||
| Hager, Wilson, et al., 1974; Hager, Harris, et al., 1975; Linton and Capelle, 1977 | ||||||||||||
| X 1Σ+ | 0 | 1241.557 Z | 5.966 29 | 0.0054557 | 0.7267512 21 | 0.0050377 30 | 2.35E-6 30 | 0.980E-6 | 1.509739 31 | |||
| Hedelund and Lambert, 1972; Beer, Lambert, et al., 1974 | ||||||||||||
| Rotation sp. 32 | ||||||||||||
| Torring, 1968; Honerjager and Tischer, 1974; Lovas and Krupenie, 1974; Manson, Clark, et al., 1977 | ||||||||||||
| Mol. beam rf el. reson. 33 | ||||||||||||
| Raymonda, Muenter, et al., 1970; Davis and Muenter, 1974 |
| 1 | Only v=0 and 1 observed; B1 = 0.703. Both levels are perturbed. |
| 2 | Corresponding data for Si18O and confirmation of the vibrational numbering Lagerqvist and Renhorn, 1974, 2. |
| 3 | Only one strongly perturbed level observed, vibrational numbering uncertain. |
| 4 | v=1 diffuse. Vibrational numbering doubtful. |
| 5 | Of the two observed levels only v=0 has been partially analyzed. |
| 6 | v=0 strongly perturbed. Only fragments of the 1-0 band observed, B1 = 0.67. The 2-0 band 1207 (82850 cm-1) has very broad lines. |
| 7 | Higher ΔG and Bv values (v ≤ 5) are irregular. |
| 8 | v=0 strongly perturbed; v=1 observed but not analyzed. |
| 9 | v=1 observed in a perturbation of H 1Σ+ (v=1); A1 ~ -36. Slightly different constants are given by Renhorn, 1976: Te = 70826, A1= -33.2, we = 414, B1 = 0.5763. |
| 10 | The G and I states interact strongly. Higher ΔG and Bv values are irregular. The vibrational assignments of Lagerqvist, Renhorn, et al., 1973 have been revised by Lagerqvist and Renhorn, 1974, 2 to account for isotope shifts; the vibrational numbering of the I state is still in doubt, see Renhorn, 1976. The linewidth in bands labelled G-X [according to the new assignments of Lagerqvist and Renhorn, 1974, 2] increases with v'. G(v=3) is perturbed by a 3Σ+ state (probably v=4 of g 3Σ+) having B = 0.687, Tv = 71937 cm-1. |
| 11 | v=1 perturbed by h 3Πi (v=1), see 9. |
| 12 | These constants represent only v=0, 1, 2. There are vibrational perturbations for higher v which may also affect the lower levels. |
| 13 | B1 = 0.6888, B2 = 0.6785. |
| 14 | Approximate constants from a partial analysis of the 1-0, 3-0, 4-0 bands Cornet and Dubois, 1972, Bredohl, Cornet, et al., 1975; vibrational constants confirmed by Shanker, Linton, et al., 1976. The v=0 level is perturbed Bredohl, Cornet, et al., 1975; according to Verma and Shanker, 1976 the 3Π1 component interacts strongly with A 1Π(v=23). Verma and Shanker, 1976 give constants which differ considerably from those of Bredohl, Cornet, et al., 1975. |
| 15 | Spin splitting constants for v=1: λ= 0.298, γ = -0.002 Nagaraj and Verma, 1970. |
| 16 | RKR potential curve Lakshman, Rao, et al., 1976; notice that the total energies of the potential curves calculated by Lakshman, Rao, et al., 1976 are unreliable since the Te values used by them are, in fact, T00 values. |
| 17 | Radiative lifetime τ(v=1...7) = 10.5 ns Elander and Smith, 1973. These authors have calculated Franck-Condon factors and f values for bands of the v'=0 progression and have determined the r dependence of the transition moment. |
| 18 | A new emission system reported by Bredohl, Cornet, et al., 1973 has been shown Barrow and Stone, 1975 to be part of the E →X system with high v' and v"; see also Shanker, Linton, et al., 1976. |
| 19 | Field, Lagerqvist, et al., 1976 |
| 20 | The A 1Π state is extensively perturbed by levels of d 3Δ, e 3Σ-, C 1Σ-, D 1Δ; see Field, Lagerqvist, et al., 1976 who give a very detailed analysis of these perturbations for 28Si16O and 28Si18O. Selective enhancement of perturbed and corresponding "extra" lines in emission under fast pumping conditions Bredohl, Remy, et al., 1976. |
| 21 | RKR potential energy curves for the eight lowest states Field, Lagerqvist, et al., 1976; see also Nair, Singh, et al., 1965, Lakshman, Rao, et al., 1976 and 16 concerning the results of Lakshman, Rao, et al., 1976. |
| 22 | Radiative lifetime τ = 9.6 ns [phase-shift method Smith and Liszt, 1972] corresponding to fel = 0.13; see also Czernichowski and Zyrnicki, 1970. Considerably smaller f values have been derived by Main, Morsell, et al., 1968, Rusin, 1970; for a summary of reported f values see Oddershede and Elander, 1976 whose theoretical calculations predict τ = 32 ns. |
| 23 | Franck-Condon factors Nicholls, 1962, Liszt and Smith, 1972, Renhorn, 1976. Isotope shifts for 29Si16O and 30Si16O Podkorytova, 1975, Shanker, Linton, et al., 1976. |
| 24 | All constants for these states derived from perturbations in A 1Π Lagerqvist and Uhler, 1953, Field, Lagerqvist, et al., 1976. |
| 25 | A = +8. There is a strong spin-orbit interaction between 3Δ2 and 1Δ2 which causes a large asymmetry in the spin splitting of d 3Δ Field, Lagerqvist, et al., 1976. |
| 26 | Effective B0 values Singh, Bredohl, et al., 1974; using instead sums of Δ2F(J) for the three components Nagaraj and Verma, 1970 obtain B0 = 0.67668 Nagaraj and Verma, 1970. Λ-type doubling in 3Π0 and 3Π1 Singh, Bredohl, et al., 1974. |
| 27 | A0 = +73.19, A1= +73.02 Nagaraj and Verma, 1970. |
| 28 | Predicted constants Field, Lagerqvist, et al., 1976; see also Heil and Schaefer, 1972, Oddershede and Elander, 1976. Only v'=0 has been observed in chemiluminescence. From partially resolved rotational structure Linton and Capelle, 1977 derive B0 ~ 0.59. |
| 29 | These are the constants of Barrow and Stone, 1975, Field, Lagerqvist, et al., 1976 which are very similar to the old constants of Lagerqvist and Uhler, 1953 and the more recent ones of Beer, Lambert, et al., 1974 (rotation -vibration spectra); see also Cornet, 1971, Bosser, Lebreton, et al., 1972. |
| 30 | Manson, Clark, et al., 1977 |
| 31 | Rot.-vibr. Sp. 36 |
| 32 | Several microwave lines have been observed in interstellar space and some extended stellar atmospheres, see e.g. Kaifu, Buhl, et al., 1975, Buhl, Snyder, et al., 1975. Maser action is prevalent. |
| 33 | μel(v) = 3.0882 + 0.0197(v+1/2) D for v≤3 Raymonda, Muenter, et al., 1970; for gJ factors (-0.1536 μN for v=0) and other magnetic proper ties see Davis and Muenter, 1974, also Honerjager and Tischer, 1974. |
| 34 | Average of several thermochenical determinations; see the summary in the Appendix of Hildenbrand and Murad, 1974, also Coppens, Smoes, et al., 1967, Nagai, Niwa, et al., 1973. |
| 35 | Average of the values obtained on the assumption that F, L, ... and H,P, ... are the first members of two Rydberg series converging to X 2Σ+ of SiO+ Lagerqvist, Renhorn, et al., 1973, Lagerqvist and Renhorn, 1974, 2. The electron impact appearance potential is 11.58 eV Hildenbrand and Murad, 1969, Hildenbrand, 1971. |
| 36 | Observed in late-type stars Beer, Lambert, et al., 1974, Singh, 1975. |
Go To: Top, Gas phase ion energetics data, Constants of diatomic molecules, Notes / Error Report
Data compilation copyright by the U.S. Secretary of Commerce on behalf of the U.S.A. All rights reserved.
Hunter and Lias, 1998
Hunter, E.P.; Lias, S.G.,
Evaluated Gas Phase Basicities and Proton Affinities of Molecules: An Update,
J. Phys. Chem. Ref. Data, 1998, 27, 3, 413-656. [doi:10.1063/1.556018]
[all data]
Nakagawa, Asano, et al., 1981
Nakagawa, H.; Asano, M.; Kubo, K.,
Mass spectrometric study of the vaporization of lithium metasilicate,
J. Nucl. Mater., 1981, 102, 292. [all data]
Huber and Herzberg, 1979
Huber, K.P.; Herzberg, G.,
Molecular Spectra and Molecular Structure. IV. Constants of Diatomic Molecules,, Van Nostrand Reinhold Co., 1979, ,1. [all data]
Thompson, 1973
Thompson, K.R.,
Mass spectrometric determination of the atomization energies of AlSiO(g) and Al2O(g),
High Temp. Sci., 1973, 5, 62. [all data]
Stearns and Kohl, 1973
Stearns, C.A.; Kohl, F.J.,
Mass spectrometric determination of the dissociation energies of gaseous Al2, AlSi, and AlSiO,
High Temp. Sci., 1973, 5, 113. [all data]
Muenow, 1973
Muenow, D.W.,
Mass spectrometric evidence for the gaseous silicon oxide nitride molecule and its heat of atomizaton,
J. Phys. Chem., 1973, 77, 970. [all data]
Hildenbrand, 1972
Hildenbrand, D.L.,
The gaseous equilibrium Ge + SiO = GeO + Si and the dissociation energy of SiO,
High Temp. Sci., 1972, 4, 244. [all data]
Hildenbrand, 1971
Hildenbrand, D.L.,
First ionization potentials of the molecules BF, SiO and GeO,
Intern. J. Mass Spectrom. Ion Phys., 1971, 7, 255. [all data]
Hildenbrand and Murad, 1969
Hildenbrand, D.L.; Murad, E.,
Dissociation energy and ionization potential of silicon monoxide,
J. Chem. Phys., 1969, 51, 807. [all data]
Heil and Schaefer, 1972
Heil, T.G.; Schaefer, H.F., III,
Potential curves for the valence-excited states of silicon monoxide. A theoretical study,
J. Chem. Phys., 1972, 56, 958. [all data]
Oddershede and Elander, 1976
Oddershede, J.; Elander, N.,
Spectroscopic constants and radiative lifetimes for valence-excited bound states in SiO,
J. Chem. Phys., 1976, 65, 3495. [all data]
Lagerqvist, Renhorn, et al., 1973
Lagerqvist, A.; Renhorn, I.; Elander, N.,
The spectrum of SiO in the vacuum ultraviolet region,
J. Mol. Spectrosc., 1973, 46, 285. [all data]
Lagerqvist and Renhorn, 1974
Lagerqvist, A.; Renhorn, I.,
A singlet-triplet perturbation in the band spectrum of SiO,
Acta Phys. Acad. Sci. Hung., 1974, 35, 155. [all data]
Bredohl, Cornet, et al., 1975
Bredohl, H.; Cornet, R.; Dubois, I.,
A correction to the vibrational numbering of the c3Πi-a3Πr transition of SiO,
J. Phys. B:, 1975, 8, 16. [all data]
Shanker, Linton, et al., 1976
Shanker, R.; Linton, C.; Verma, R.D.,
The chemiluminescent flame spectrum of SiO,
J. Mol. Spectrosc., 1976, 60, 197. [all data]
Singh, Bredohl, et al., 1974
Singh, M.; Bredohl, H.; Remy, F.; Dubois, I.,
The d3Σ-a3Πr transition of SiO,
Can. J. Phys., 1974, 52, 569. [all data]
Barrow and Stone, 1975
Barrow, R.F.; Stone, T.J.,
The identification of a new band system associated with gaseous silicon monoxide,
J. Phys. B:, 1975, 8, 13. [all data]
Singh, Upadhya, et al., 1969
Singh, J.; Upadhya, K.N.; Nair, K.P.R.,
On the ultraviolet band system of silicon monoxide,
Indian J. Phys., 1969, 43, 665. [all data]
Bredohl, Cornet, et al., 1974
Bredohl, H.; Cornet, R.; Dubois, I.; Remy, F.,
The a3Πr-X1Σ+ transition of SiO,
J. Phys. B:, 1974, 7, 66. [all data]
Hager, Wilson, et al., 1974
Hager, G.; Wilson, L.E.; Hadley, S.G.,
Reactions of atomic silicon and germanium with nitrous oxide to produce electronically excited silicon monoxide and germanium monoxide,
Chem. Phys. Lett., 1974, 27, 439. [all data]
Hager, Harris, et al., 1975
Hager, G.; Harris, R.; Hadley, S.G.,
The a3Σ+ → X1Σ+ and b3Π → X1Σ+ band systems of SiO and the a3Σ+ → X1Σ+ band system of GeO observed in chemiluminescence,
J. Chem. Phys., 1975, 63, 2810. [all data]
Linton and Capelle, 1977
Linton, C.; Capelle, G.A.,
Chemiluminescence of Si + N2O flames,
J. Mol. Spectrosc., 1977, 66, 62. [all data]
Hedelund and Lambert, 1972
Hedelund, J.; Lambert, D.L.,
Transition probabilities for the vibration-rotation bands of silicon monoxide,
Astrophys. Lett., 1972, 11, 71. [all data]
Beer, Lambert, et al., 1974
Beer, R.; Lambert, D.L.; Sneden, C.,
The silicon monoxide radical and the atmosphere of α orionis,
Publ. Astron. Soc. Pac., 1974, 86, 806. [all data]
Torring, 1968
Torring, T.,
Das Mikrowellenrotationsspektrum des SiO,
Z. Naturforsch. A, 1968, 23, 777. [all data]
Honerjager and Tischer, 1974
Honerjager, R.; Tischer, R.,
gJ-Faktor der Molekeln SiO und PbTe und Anisotropie der Magnetisierbarkeit von SiO,
Z. Naturforsch. A, 1974, 29, 1695. [all data]
Lovas and Krupenie, 1974
Lovas, F.J.; Krupenie, P.H.,
Microwave spectra of molecules of astrophysical interest. VII. Carbon monoxide, carbon monosulfide, and silicon monoxide,
J. Phys. Chem. Ref. Data, 1974, 3, 245. [all data]
Manson, Clark, et al., 1977
Manson, E.L., Jr.; Clark, W.W.; de Lucia, F.C.; Gordy, W.,
Millimeter spectrum and molecular constants of silicon monoxide,
Phys. Rev. A: Gen. Phys., 1977, 15, 223. [all data]
Raymonda, Muenter, et al., 1970
Raymonda, J.W.; Muenter, J.S.; Klemperer, W.A.,
Electric dipole moment of SiO and GeO,
J. Chem. Phys., 1970, 52, 3458. [all data]
Davis and Muenter, 1974
Davis, R.E.; Muenter, J.S.,
Magnetic properties of silicon and germanium monoxide,
J. Chem. Phys., 1974, 61, 2940. [all data]
Lagerqvist and Renhorn, 1974, 2
Lagerqvist, A.; Renhorn, I.,
The spectrum of silicon monoxide (oxygen-18) in the vacuum ultraviolet region,
J. Mol. Spectrosc., 1974, 19, 157. [all data]
Renhorn, 1976
Renhorn,
Dissertation, Stockholm, 1976, 1. [all data]
Cornet and Dubois, 1972
Cornet, R.; Dubois, I.,
New electronic transitions of SiO,
Can. J. Phys., 1972, 50, 630. [all data]
Verma and Shanker, 1976
Verma, R.D.; Shanker, R.,
Deperturbation study of the 0-1 band of the d3Πi-b3Πr transition of the SiO molecule,
J. Mol. Spectrosc., 1976, 63, 553. [all data]
Nagaraj and Verma, 1970
Nagaraj, S.; Verma, R.D.,
A 3Σ-3Π transition of the SiO molecule,
Can. J. Phys., 1970, 48, 1436. [all data]
Lakshman, Rao, et al., 1976
Lakshman, S.V.J.; Rao, T.V.R.; Naidu, G.T.,
The true potential energy curves for different states of SiO and SiS molecules,
Pramana, 1976, 7, 369. [all data]
Elander and Smith, 1973
Elander, N.; Smith, W.H.,
Radiative lifetimes and band oscillator strengths for metal oxides. II. SiO E 1Σ+-X1Σ+,
Astrophys. J., 1973, 184, 311. [all data]
Bredohl, Cornet, et al., 1973
Bredohl, H.; Cornet, R.; Dubois, I.; Remy, F.,
A new spectrum associated with silicon monoxide,
Can. J. Phys., 1973, 51, 2332. [all data]
Field, Lagerqvist, et al., 1976
Field, R.W.; Lagerqvist, A.; Renhorn, I.,
The low lying electronic states of SiO,
Phys. Scr., 1976, 14, 298-319. [all data]
Bredohl, Remy, et al., 1976
Bredohl, H.; Remy, F.; Cornet, R.,
Perturbations in the A1Π state of SiO,
J. Phys. B:, 1976, 9, 2307. [all data]
Nair, Singh, et al., 1965
Nair, K.P.R.; Singh, R.B.; Rai, D.K.,
Potential-energy curves and dissociation energies of oxides and sulfides of group IV A elements,
J. Chem. Phys., 1965, 43, 3570. [all data]
Smith and Liszt, 1972
Smith, W.H.; Liszt, H.S.,
Radiative lifetimes and absolute oscillator strengths for the SiO A1Π-X1Σ+ transition,
J. Quant. Spectrosc. Radiat. Transfer, 1972, 12, 505. [all data]
Czernichowski and Zyrnicki, 1970
Czernichowski, A.; Zyrnicki, W.,
Determination of the band oscillator strengths (0,1) and (0,2) for the A1Π-X1Σ+ system in the SiO molecule,
Acta Phys. Pol., 1970, 37, 865. [all data]
Main, Morsell, et al., 1968
Main, R.P.; Morsell, A.L.; Hooker, W.J.,
Measurement of the oscillator strength of the SiO (A1Π - X1Σ+) band system,
J. Quant. Spectrosc. Radiat. Transfer, 1968, 8, 1527. [all data]
Rusin, 1970
Rusin, A.D.,
Excitation of the SiO spectrum by an explosion in a spherical bomb,
Moscow Univ. Chem. Bull. Engl. Transl., 1970, 25, 11, In original 397. [all data]
Nicholls, 1962
Nicholls, R.W.,
Franck-Condon factors to high vibrational quantum numbers II: SiO, MgO, SrO, AlO, VO, NO,
J. Res. Nat. Bur. Stand. Sect. A, 1962, 66, 227. [all data]
Liszt and Smith, 1972
Liszt, H.S.; Smith, W.H.,
RKR Franck-Condon factors for blue and ultraviolet transitions of some molecules of astrophysical interest and some comments on the interstellar abundance of CH, CH+, and SiH,
J. Quant. Spectrosc. Radiat. Transfer, 1972, 12, 947. [all data]
Podkorytova, 1975
Podkorytova, N.S.,
Analysis and isotropic effect for Si28O and Si29O molecules,
Opt. Spectrosc. Engl. Transl., 1975, 38, 637, In original 1103. [all data]
Lagerqvist and Uhler, 1953
Lagerqvist, A.; Uhler, U.,
The ultra-violet band-system of silicon monoxide,
Ark. Fys., 1953, 6, 95. [all data]
Cornet, 1971
Cornet, R.,
Constantes vibrationnelles et energies de dissociation des etats X1Σ+ et A1Π de SiO,
Bull. Cl. Sci. Acad. R. Belg., 1971, 57, 1069. [all data]
Bosser, Lebreton, et al., 1972
Bosser, G.; Lebreton, J.; Marsigny, L.,
Nouvelles bandes du systeme A1Π→X1Σ+ de SiO,
C.R. Acad. Sci. Paris, Ser. C, 1972, 275, 531. [all data]
Kaifu, Buhl, et al., 1975
Kaifu, N.; Buhl, D.; Snyder, L.E.,
Vibrationally excited SiO: a new type of maser source in the millimeter wavelength region,
Astrophys. J., 1975, 195, 359. [all data]
Buhl, Snyder, et al., 1975
Buhl, D.; Snyder, L.E.; Lovas, F.J.; Johnson, D.R.,
Is there a maser in the silicon monoxide ground state,
Astrophys. J., 1975, 201, 29. [all data]
Hildenbrand and Murad, 1974
Hildenbrand, D.L.; Murad, E.,
Mass spectrometric studies of gaseous ThO and ThO2,
J. Chem. Phys., 1974, 61, 1232. [all data]
Coppens, Smoes, et al., 1967
Coppens, P.; Smoes, S.; Drowart, J.,
Mass spectrometric determination of the dissociation energies of the molecules GeS, ScS, YS, LaS, and CeS,
Trans. Faraday Soc., 1967, 63, 2140. [all data]
Nagai, Niwa, et al., 1973
Nagai, S.I.; Niwa, K.; Shinmei, M.; Yokokawa, T.,
Knudsen effusion study of silica,
J. Chem. Soc. Faraday Trans. 1, 1973, 69, 1628. [all data]
Singh, 1975
Singh, P.D.,
The silicon monoxide radical in M stars - the fundamental rotation-vibration band of SiO,
Astron. Astrophys., 1975, 44, 411. [all data]
Go To: Top, Gas phase ion energetics data, Constants of diatomic molecules, References
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Send your homework as a single ZIP archive with your files, or send a link to your GitHub repo. Try to keep line lengths below 80 characters.
Let p=(x,y) be a point in a plane.
Define the following functions using lambda:
(a) a test if p is in unit (filled) circle,
(b) a test if the coordinates of p are positive,
(c) a sorting key (y decreasing, x increasing),
(d) a sorting key (the sum |x|+|y|).
Using tests: list(filter((lambda p: ...), point_list)) Using sorting keys: point_list.sort(key=lambda p: ...)
Reversing a part of a list in place, reverse_range(L, left, right), the right index is included. Write iterative and recursive versions.
# Example. L = [0, 1, 2, 3, 4, 5, 6, 7, 8, 9] reverse_range(L, 3, 6) # index 6 is included! print(L) # [0, 1, 2, 6, 5, 4, 3, 7, 8, 9] # the list L changed # The numbers outside the range are intact.
Create the following infinite generators:
(a) iter_even(), producing even numbers (0, 2, 4, ...),
(b) iter_odd(), producing odd numbers (1, 3, 5, ...),
(c) iter_power(k), producing powers of k (1, k, k*k, k*k*k, ...).


class Resque::Worker
Public Class Methods
# File lib/resque_manager/overrides/resque/worker.rb, line 224 def self.start(options) ips = options[:hosts] application_path = options[:application_path] queues = options[:queues] if Rails.env =~ /development|test/ Thread.new(application_path, queues) { |application_path, queue| system("cd #{application_path || '.'} && bundle exec #{ResqueManager.resque_worker_rake || 'rake'} RAILS_ENV=#{Rails.env} QUEUE=#{queue} resque:work") } else Thread.new(ips, application_path, queues) { |ip_list, application_path, queue| system("cd #{Rails.root} && #{ResqueManager.resque_worker_cap || 'bundle exec cap'} #{Rails.env} resque:work host=#{ip_list} application_path=#{application_path} queue=#{queue}") } end end
logic for mappged_mget changed where it returns keys with nil values in latest redis gem.
# File lib/resque_manager/overrides/resque/worker.rb, line 206 def self.working names = all return [] unless names.any? names.map! { |name| "worker:#{name}" } Resque.redis.mapped_mget(*names).map do |key, value| find key.sub("worker:", '') unless value.nil? end.compact end
Public Instance Methods
# File lib/resque_manager/overrides/resque/worker.rb, line 148 def all_workers_in_pid_working workers_in_pid.select { |w| (hash = w.processing) && !hash.empty? } end
# File lib/resque_manager/overrides/resque/worker.rb, line 259 def continue if Rails.env =~ /development|test/ system("kill -CONT #{self.pid}") else system("cd #{Rails.root} && #{ResqueManager.resque_worker_cap || 'bundle exec cap'} #{Rails.env} resque:continue_worker pid=#{self.pid} host=#{self.ip}") end end
# File lib/resque_manager/overrides/resque/worker.rb, line 48 def ip to_s.split(':').first[/\b(?:\d{1,3}\.){3}\d{1,3}\b/] end
# File lib/resque_manager/overrides/resque/worker.rb, line 10 def local_ip @@local_ip ||= UDPSocket.open { |s| s.connect('google.com', 1); s.addr.last } end
# File lib/resque_manager/overrides/resque/worker.rb, line 220 def overview_message job['overview_message'] end
# File lib/resque_manager/overrides/resque/worker.rb, line 215 def overview_message=(message) data = encode(job.merge('overview_message' => message)) Resque.redis.set("worker:#{self}", data) end
# File lib/resque_manager/overrides/resque/worker.rb, line 36 def path to_s.split(':').fourth end
# File lib/resque_manager/overrides/resque/worker.rb, line 251 def pause if Rails.env =~ /development|test/ system("kill -USR2 #{self.pid}") else system("cd #{Rails.root} && #{ResqueManager.resque_worker_cap || 'bundle exec cap'} resque:pause_worker pid=#{self.pid} host=#{self.ip}") end end
When the worker gets the -USR2 signal, #to_s may give a different value for the thread and queue portion
# File lib/resque_manager/overrides/resque/worker.rb, line 23 def pause_key key = to_s.split(':') "worker:#{key.first}:#{key.second}:all_workers:paused" end
Stop processing jobs after the current one has completed (if we're currently running one).
OVERRIDE to set a redis key so UI knows it's paused too
# File lib/resque_manager/overrides/resque/worker.rb, line 100 def pause_processing_with_pause_key pause_processing_without_pause_key Resque.redis.set(pause_key, Time.now.to_s) end
# File lib/resque_manager/overrides/resque/worker.rb, line 87 def paused Resque.redis.get pause_key end
are we paused? OVERRIDE so UI can tell if we're paused
# File lib/resque_manager/overrides/resque/worker.rb, line 93 def paused? @paused || paused.present? end
# File lib/resque_manager/overrides/resque/worker.rb, line 28 def pid to_s.split(':').second end
Looks for any workers which should be running on this server and, if they're not, removes them from Redis.
This is a form of garbage collection. If a server is killed by a hard shutdown, power failure, or something else beyond our control, the Resque workers will not die gracefully and therefore will leave stale state information in Redis.
By checking the current Redis state against the actual environment, we can determine if Redis is old and clean it up a bit.
# File lib/resque_manager/overrides/resque/worker.rb, line 127 def prune_dead_workers Worker.all.each do |worker| host, pid, thread, path, queues = worker.id.split(':') next unless host.include?(hostname) next if worker_pids.include?(pid) log! "Pruning dead worker: #{worker}" worker.unregister_worker end end
# File lib/resque_manager/overrides/resque/worker.rb, line 40 def queue to_s.split(':').fifth end
OVERRIDE for multithreaded workers
# File lib/resque_manager/overrides/resque/worker.rb, line 57 def queues Thread.current[:queues] == "*" ? Resque.queues.sort : Thread.current[:queues].split(',') end
# File lib/resque_manager/overrides/resque/worker.rb, line 52 def queues_in_pid workers_in_pid.collect { |w| w.queue }.compact end
# File lib/resque_manager/overrides/resque/worker.rb, line 236 def quit if Rails.env =~ /development|test/ if RUBY_PLATFORM =~ /java/ #jruby doesn't trap the -QUIT signal #-TERM gracefully kills the main pid and does a -9 on the child if there is one. #Since jruby doesn't fork a child, the main worker is gracefully killed. system("kill -TERM #{self.pid}") else system("kill -QUIT #{self.pid}") end else system("cd #{Rails.root} && #{ResqueManager.resque_worker_cap || 'bundle exec cap'} #{Rails.env} resque:quit_worker pid=#{self.pid} host=#{self.ip} application_path=#{self.path}") end end
override so we can synchronize the client on the reconnect for multithreaded workers.
# File lib/resque_manager/overrides/resque/worker.rb, line 187 def reconnect tries = 0 begin redis.synchronize do |client| client.reconnect end rescue Redis::BaseConnectionError if (tries += 1) <= 3 log "Error reconnecting to Redis; retrying" sleep(tries) retry else log "Error reconnecting to Redis; quitting" raise end end end
# File lib/resque_manager/overrides/resque/worker.rb, line 267 def restart queues = self.queues_in_pid.join('#') quit self.class.start(hosts: self.ip, queues: queues, application_path: self.path) end
Schedule this worker for shutdown. Will finish processing the current job.
OVERRIDE for multithreaded workers
# File lib/resque_manager/overrides/resque/worker.rb, line 80 def shutdown_with_multithreading Thread.list.each { |t| t[:shutdown] = true } shutdown_without_multithreading end
# File lib/resque_manager/overrides/resque/worker.rb, line 180 def shutdown_with_multithreading? shutdown_without_multithreading? || Thread.current[:shutdown] end
Runs all the methods needed when a worker begins its lifecycle.
OVERRIDE for multithreaded workers
# File lib/resque_manager/overrides/resque/worker.rb, line 63 def startup enable_gc_optimizations if Thread.current == Thread.main register_signal_handlers prune_dead_workers end run_hook :before_first_fork register_worker # Fix buffering so we can `rake resque:work > resque.log` and # get output from the child in there. $stdout.sync = true end
# File lib/resque_manager/overrides/resque/worker.rb, line 32 def thread to_s.split(':').third end
The string representation is the same as the id for this worker instance. Can be used with `Worker.find`.
# File lib/resque_manager/overrides/resque/worker.rb, line 16 def to_s @to_s || "#{hostname}(#{local_ip}):#{Process.pid}:#{Thread.current.object_id}:#{Thread.current[:path]}:#{Thread.current[:queues]}" end
Start processing jobs again after a pause
OVERRIDE to set remove redis key so UI knows it's unpaused too
Would prefer to call super but get no superclass method error
# File lib/resque_manager/overrides/resque/worker.rb, line 110 def unpause_processing_with_pause_key unpause_processing_without_pause_key Resque.redis.del(pause_key) end
Unregisters ourself as a worker. Useful when shutting down. OVERRIDE to also remove the pause key Would prefer to call super but get no superclass method error
# File lib/resque_manager/overrides/resque/worker.rb, line 140 def unregister_worker_with_pause(exception = nil) unregister_worker_without_pause(exception) Resque.redis.del(pause_key) end
This is the main workhorse method. Called on a Worker instance, it begins the worker life cycle. The following events occur during a worker's life cycle: 1. Startup: Signals are registered, dead workers are pruned, and this worker is registered. 2. Work loop: Jobs are pulled from a queue and processed. 3. Teardown: This worker is unregistered. Can be passed an integer representing the polling frequency. The default is 5 seconds, but for a semi-active site you may want to use a smaller value. Also accepts a block which will be passed the job as soon as it has completed processing. Useful for testing.
OVERRIDE for multithreaded workers
# File lib/resque_manager/overrides/resque/worker.rb, line 169 def work_with_multithreading(interval = 5.0, &block) work_without_multithreading(interval, &block) loop do #hang onto the process until all threads are done break if all_workers_in_pid_working.blank? sleep interval.to_i end end
# File lib/resque_manager/overrides/resque/worker.rb, line 44 def workers_in_pid Array(Resque.redis.smembers(:workers)).select { |id| id =~ /\(#{ip}\):#{pid}/ }.map { |id| Resque::Worker.find(id) }.compact end


VENUS BEAUTY INSTITUTE A film review by Norm Schrager Copyright 2000 filmcritic.com filmcritic.com
A movie that centers around the workplace can end up feeling like a sitcom. You have a couple of principal characters whose lives are examined, and a small cast of others that are thrown in to add pizazz to the storytelling. This may work in a well-written 22-minute TV show, but in Venus Beauty Institute it results in a film that eventually loses its focus, trying to rely on passion that just ain't that passionate.
Pity poor Angèle (Nathalie Baye). She toils away at the titular French beauty salon during the day, and looks for quick sexual encounters at night. In her 40s, she feels too burned by the loves in her past to get hurt again, and instead finds her happiness in hunting down men with whom to have trysts. Early in the film, she quickly approaches a stranger in a cafeteria, tactlessly luring him away from dinner so they can do it in his car. We get the feeling that she wants more -- a funny opening sequence where she gets dumped helps -- but she's too headstrong for that.
Angèle won't commit, and neither does Venus Beauty Institute. Writer/director Tonie Marshall has the right idea for two-thirds of the movie, putting nearly all her efforts to crafting Angèle, diving into what could be a complex character. We see her public side at the salon as well as her private life, and Marshall surrounds her with a circle of people in both, including an engaged, scruffy-looking guy who falls instantly in love at the sight of her (what is it with the French and leading men that look like Gerard Depardieu?!). We get to see her new relationship with him as well as her friends, acquaintances, and customers at the salon.
But once Marshall starts spending more time with others, we lose interest. With the time invested in Angèle, we don't really care to see the supporting characters from the salon outside of that setting. With its pink and peach color design in the midst of bustling Paris, the shop provides a creative contrast to the rest of the movie, and some of the film's best and quirkiest scenes are right there -- maybe the story should've never left that set. But when Marshall decides that we need to know more about Angèle's buddies, the movie and the salon lose their flavor.
As Angèle, veteran French actress Baye (The Man Who Loved Women) brings out as much of this complex character as possible, and was nominated for France's César Award (the movie won four, including Best French Film). Bearing a resemblance to Kathy Baker, she shows a life of weariness and street smarts on her face, looking like she was once a stunning beauty who now needs to remind herself of that. Baye delivers Angèle's aggressive come-ons and facial mannerisms with a matter-of-fact attitude that shows off real natural talent.
But as lively as she makes Angèle, Baye can't hold up the finale of the movie on her own. The final act makes Venus Beauty Institute too long, as Marshall stretches the story beyond a comfortable length, and throws in some stupid, predictable plot points. Thinking that this would be great for say, a Sunday afternoon video rental, I was proven wrong by the movie's finale. And the final shot, meant to come off as magical and romantic, is too contrived just like, well, many sitcoms.

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THREE COLORS: WHITE A film review by Bryant Frazer Copyright 1995 Bryant Frazer
Bookended as it is by BLUE and RED, the second film in Kieslowski's liberty/equality/fraternity trilogy is a welcome relief from the sometimes tragic sensibility of the other two films. WHITE is about post-Communist Poland. It is about the tricks that hold up our own quests for "equality" (is there really such a thing outside of mathematics?). But most of all, it's a love story.
Of course, all three of the films are love stories in a way; but BLUE is a love story that ends as the film begins, and RED is a love story once removed. WHITE is a story about stubborn love, a sort of co-dependent relationship that endures despite the best efforts of both lovers. Zbigniew Zamachowski plays Karol Karol, the impotent hairdresser who is abandoned in Paris by wife Julie Delpy. Unable to support himself, the spurned lover eventually returns to his native Poland, smuggling himself in inside a friend's suitcase. Seething with resentment, he makes a fortune in his newly capitalist homeland, and then sets off on an elaborate plan to revenge himself on his wife. Kieslowski makes some wry observations about the nature of capitalism and the lust for "easy money." Karol doesn't simply want to make himself the financial equal of his wife; he wants to become "more equal" than she is. That being the case, it's not enough for him simply to make a fortune. He wants to humiliate her, as well.
He manages that, but the circumstances are an idiosyncratic delight. WHITE isn't lofty enough to avoid an occasional detour into sober, existential territory, but the side trips add a little weight to the story, which is at heart a marriage farce. The sublime Zamachowski pulls his best Chaplin routine here, and it pays off charmingly. It's no surprise that Delpy is radiant, and plays the ice queen well (my favorite shot of Delpy is still her cameo in RED, where all three films touch briefly). In most ways, this film is the least of the trilogy -- WHITE is so conciliatory toward its audience that it threatens to float away. But at the end, it's anchored by a Chaplinesque moment of revelation that justifies our attention and respect, and this film's solid place in Kieslowski's admirable trilogy.
-- DEEP FOCUS: Archived Reviews by Bryant Frazer http://www.panix.com/~bfrazer/flicker/
The review above was posted to the
rec.arts.movies.reviews newsgroup (de.rec.film.kritiken for German reviews).
The Internet Movie Database accepts no responsibility for the contents of the
review and has no editorial control. Unless stated otherwise, the copyright
belongs to the author.
Please direct comments/criticisms of the review to relevant newsgroups.
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We have detected different licenses in package.json and other licenses files (LICENSE, LICENSE.MD etc). This probably means that there is an inconsistency in the choice of the license (or a file not updated yet with the right license).
This flag has not been created to detect multiple licenses / conformance rules.
Example: ISC OR GPL-2.0-with-GCC-exception.
Under the hood we use conformance to parse licenses !


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A programmer and Developer
A full stack web and app developer,Windows Systems Administrator, Network Engineer.
Ordered and received inventory
Maintained Automated Supply Sysytems
Operated, configured and troubleshot unit level computers
Fixed networks issues on unit level computers
Fixed level one and two on unit level computers daily
Utilized Microsoft SPSS statistical software to track and analyze data
Designed and built statistical analysis models on large data sets using Teradata.
Troubleshot customer network issues remotely through emails
configured and troubleshot computers and print issues
Provided first level contact and conveyed resolutions to customer issues
system Administration


關於 v5
版本
v5.6.0 "Kristen"
授權
目前使用: Unlicense/MIT
This project uses dual license, Unlicense, MIT.
===================================================================
This is free and unencumbered software released into the public domain.
Anyone is free to copy, modify, publish, use, compile, sell, or
distribute this software, either in source code form or as a compiled
binary, for any purpose, commercial or non-commercial, and by any
means.
In jurisdictions that recognize copyright laws, the author or authors
of this software dedicate any and all copyright interest in the
software to the public domain. We make this dedication for the benefit
of the public at large and to the detriment of our heirs and
successors. We intend this dedication to be an overt act of
relinquishment in perpetuity of all present and future rights to this
software under copyright law.

IN NO EVENT SHALL THE AUTHORS BE LIABLE FOR ANY CLAIM, DAMAGES OR
OTHER LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE,
ARISING FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR
OTHER DEALINGS IN THE SOFTWARE.
For more information, please refer to http://unlicense.org/
===================================================================
Copyright (C) 2020 NCT skyouo
Permission is hereby granted, free of charge, to any person obtaining a copy of
this software and associated documentation files (the "Software"), to deal in
the Software without restriction, including without limitation the rights to use,
copy, modify, merge, publish, distribute, sublicense, and/or sell copies of the
Software, and to permit persons to whom the Software is furnished to do so,
subject to the following conditions:
The above copyright notice and this permission notice shall be included in all
copies or substantial portions of the Software.
 IN NO EVENT SHALL THE AUTHORS OR
COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER LIABILITY, WHETHER
IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM, OUT OF OR IN
CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE SOFTWARE.
===================================================================


---
layout: default
title: Help
permalink: /help/
---
Help Documentation
Russ here!
Sorry, but there isn't any documentation yet. The program is in a very beta stage. Just send me any questions you have directly.
TODO
- write up tutorial
- individual use
- race comittee
- regatta manager
- people should have an idea of best practices when they operate this program
- think about workflow
- how would a sailing academy use this program over a season


by Jack Porter on November 20, 2018
by Rita Zhang on November 7, 2018
by Jacob Levy on September 19, 2018
by Michael Culbertson on September 18, 2018


The test below will allow for any number of decimal places, samples, and Likert categories. If your value is a percent convert it to a decimal. Note that the sample size determines how many decimal places you can check. With a sample size of 1-99 you can check two decimal places. With a sample size of 100-999 you can check three decimal places.
See this help page for rounding issues.


DROP DATABASE
Drops a database.
Syntax
DROP DATABASE database_name
Parameters
- database_name
-
Name of the database to be dropped. You can't drop the dev, padb_harvest, template0, or template1 databases, and you can't drop the current database.
To drop an external database, drop the external schema. For more information, see DROP SCHEMA.
Examples
The following example drops a database named TICKIT_TEST:
drop database tickit_test;


 Take a peek at the new “Ongoing Work Dashboard:”
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Engineering will be more responsive to issue comments
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these now pipe into our HipChat
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JIRA comments are the place to have any formal discussion
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let’s say you have a discussion on the phone regarding a ticket and a decision is reached. make sure one someone in that discussion records the output on the appropriate work item or it functionally never happened!
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if you’d like a comment to NOT pipe into HipChat, put #nohipchat in the body of the comment to prevent this
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iOS engineer(s) beginning to work directly with West for great justice!
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greater unity between engineering and marketing/design
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more insight into what’s coming down the pipe leading to a smoother implementation phase
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Goals:
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increased transparency regarding engineering operations
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more clarity about what’s being built and by whom
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Close to the Metal
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Intense rework of the API based on feedback coming out of the Denver Demo and our desire to future proof the existing infrastructure and data model so that we can be responsive (to Product/Marketing) in the upcoming sprints
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Core decisions and architecture regarding the Blinker in-house client layer
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administration panels - what they ought to do and how we secure them
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Takeaways:
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we’re now firmly on the road to a 1.0!
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The road ahead:
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West assets incoming end of this week
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Next sprint (starting 2/3/14) we will be implementing these assets for iOS and responsive web
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Goals:
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implement first set of features
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refine the handoff and collaboration process (Engineering - West)
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“point person” introductions and working relationships
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translation of assets and user stories into product requirements & engineering deliverables
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