BSA Flow Software Installation and User's Guide - CSI

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PDA receiving optics PDA Particle/Medium For now, select 1D Optics even if your optical system is 2D or 3D. Later on, when you are familiar with the software, you can revert to the Dantec Device Configuration utility and configure according to your equipment. Type or select from the drop down lists the appropriate beam parameters of your system. Click OK if you are using a LDA system and skip the PDA receiving optics part or click on PDA Receiver if you have a PDA system. For the PDA, select the PDA Receiver from the Optics properties. This opens the following window: Select the receiver type and type or select the appropriate parameter values. Further details are given in chapter 5.4 and 5.5. Slit width is available for 112mm DualPDA and 112mm FiberPDA optics. Window type is only available with FiberPDA and 112mm FiberPDA probes. To configure the Window type, please refer to chapter 5.5. Click on PDA Particle/Medium from the Optics properties and type or select the parameters of the following window. The default setting is water droplets in air. 4-36 BSA Flow Software: The user interface
Click on OK. Note For fully opaque and reflecting particles, the refractive index has to be set to 2 and the scattering mode set to reflection. It is possible to add new particle and new medium type in the particle/medium library: 1. Press Add button 2. Select Insert as Particle or Insert as Medium 3. Type a particle or medium name 4. Click on OK. The following window appears: 5. Enter refractive index, specific gravity, kinematic viscosity of the particles or medium. Note that specific gravity and kinematic viscosity are only for documentation purpose. 6. Click on OK. The particle and medium properties are now added in the library and can be selected by their name. BSA Flow Software: The user interface 4-37
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BSA Flow Software Version 4.10 Inst
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1. General 1.1 Table of Contents 1.
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5.5 Optical Calibrated LDA System p
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7.2.1 Basic principles of phase Dop
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1.2 Dantec Dynamics Licence Agreeme
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1.3 Laser safety All equipment usin
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2. Introduction Congratulations wit
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2.1.9 Analog Monitor Option 2.1.10
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2.3.4 Trouble shooting 2.3.5 On-lin
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3. Installation 3.1 General 3.1.1 P
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Directory structure CPU usage will
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3.2.2 Installation as administrator
Page 25 and 26: You have the possibility to define
Page 27 and 28: Click Next and select the add-ons y
Page 29 and 30: Peer-to-peer connection Processor s
Page 31 and 32: Click on the Download tab to get th
Page 33 and 34: The BSA processor will restart. Thi
Page 35 and 36: • If the Game controller needs to
Page 37 and 38: Figure 3-2 National Instruments Mea
Page 39 and 40: 3.7 Third party traverse system To
Page 41 and 42: 4. The user interface 4.1 Layout Me
Page 43 and 44: 4. If the mouse pointer was in the
Page 45 and 46: 4.3 Project explorer shortcuts to t
Page 47 and 48: Figure 4-5 Dialog for adding object
Page 49 and 50: Using Templates To make a Template,
Page 51 and 52: 4.6 The tool bar Figure 4-6 the pro
Page 53 and 54: Save As... Figure 4-10 the File men
Page 55 and 56: Figure 4-11 Save As compressed proj
Page 57 and 58: Figure 4-14 the Properties - Summar
Page 59 and 60: Figure 4-18 The Select Position dia
Page 61 and 62: Options With the Options you get a
Page 63 and 64: When Enable error logging is checke
Page 65 and 66: The fourth format, Significant Digi
Page 67 and 68: The PDA Optical Configuration objec
Page 69 and 70: 4.7.7 Help menu Figure 4-34 The Hel
Page 71 and 72: 4.9 Message window • by clicking
Page 73 and 74: PM and Bragg cell connections Warni
Page 75: LDA and PDA transmitting optics The
Page 79 and 80: In the third step, the software con
Page 81 and 82: Lightweight Traverse with handbox C
Page 83 and 84: 57G15 Traverse interface Third part
Page 85 and 86: • right-click the Traverse Server
Page 87 and 88: 4. This brings up the following dia
Page 89 and 90: To change a setting, click in the V
Page 91 and 92: Figure 4-39 System monitor in auto-
Page 93 and 94: 14. You have now completed data acq
Page 95 and 96: 4. Check the Show System Monitor wh
Page 97 and 98: . 8. LDA 1 properties are specific
Page 99 and 100: 11. To monitor the Doppler signals,
Page 101 and 102: The axes will automatically rescale
Page 103 and 104: Click Acquire. If a complete new re
Page 105 and 106: Define the positions that you want
Page 107 and 108: Select the type of the files to ope
Page 109 and 110: 5. Project explorer objects 5.1 Sta
Page 111 and 112: Browse to the file you wish to impo
Page 113 and 114: For each column, the data type must
Page 115 and 116: 5.3.1 Output properties Figure 5-4
Page 117 and 118: Figure 5-7 The Custom… dialog und
Page 119 and 120: Figure 5-8 BSA F/P 30: processor pr
Page 121 and 122: Max. acquisition time: The maximum
Page 123 and 124: Normal user interface Advanced user
Page 125 and 126: Figure 5-11 The Bragg cell connecto
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LDA 1, 2, . properties: Range and g
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5.3.4 System monitor It frequently
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Scope: Burst spectrum display Recor
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Overlaid Graphs: used to show the b
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Uncheck the Use default bindings bo
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The calibration data are stored in
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5.6.1 PDA beam system The Beam syst
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Figure 5-24: Fringe direction setti
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5.6.4 Medium properties Medium name
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Software max. limit in mm.: Self ex
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The default address of the National
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Traverse coordinates of a datum poi
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5.7.8 Traverse Mesh generator If yo
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Regions Figure 5-39 Motion pattern,
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Warning Please observe strict secur
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5.9 Export Figure 5-40 Data-sources
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If multiple positions are exported
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5.9.3 Selected columns 5.9.4 Binary
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Data C Headers Programming Examples
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char filename[256] = {0}; strcpy(fi
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Range means that the filter will ap
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5.11.1 Data Properties Note that th
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Figure 5-54. Size histogram (left)
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Figure 5-57. Velocity distribution
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Figure 5-58 list output of 1D PDA d
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The next selection in the context m
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5.13.2 Objects under Merge object A
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N−1 Mean u ∑ ηiui = i= 0 N−1
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Cross-moments The property Cross-mo
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The calculation of ε fails if Umea
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Figure 5-71 General properties of t
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An alternative geometry of a 3D LDA
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Figure 5-75: FiberPDA phase plot. A
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5.16.3 Display properties The defau
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The output quantities of the diamet
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6. Options and Add-ons This chapter
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6.1 Advanced Graphics Add-on The ma
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Figure 6-2 The Tools-Options-Output
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Figure 6-5 Scale properties for 2D
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Property group ‘Display’ Also t
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6.1.3 2D Plot [m/s] 36 34 32 The 2D
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6.1.4 2D Histogram For off-line use
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Configuring the 2D Histogram The co
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Configuring the 3D Plot Figure 6-21
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Figure 6-23 “Interpolate bin” s
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Property group ‘Data’ Figure 6-
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Coordinate shown on Intercepts the
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LDA1-Mean [m/ s] -2,00 -3,00 -4,00
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Figure 6-32 Properties of the Vecto
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Figure 6-33 shows a velocity vector
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6.1.9 Exporting plots Copying a plo
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6.2 Synchronisation Option 6.2.1 In
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Pin Signal Pin Signal 1 Out 1 14 Gr
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6.2.5 Sync. Output Signals properti
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Outputs Figure 6-40 Differential sy
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Figure 6-42 Cyclic phenomena in the
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Cycle length The property Cycle len
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It allows to define the number of b
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Note It is not possible to have 0 a
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Figure 6-47: Output data from the c
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performed prior to phase sorting yo
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Figure 6-51 Properties of the spect
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Blocking Using the FFT-approach to
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1,2 1,0 0,8 0,6 0,4 0,2 Weight fact
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Output from the Spectrum object The
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6.4.2 Advanced Spectrum object Load
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To evaluate the new algorithm, comp
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6.4.3 Correlation object Conclusion
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20 16 12 8 4 0 0.0 0.2 0.4 0.6 0.8
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Time The first column of the output
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The Protocol Figure 6-67: Generic t
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How to Use the Initialisation Strin
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Figure 6-69: Traverse File option i
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Properties Output from MATLAB engin
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Result window Script Hides and disp
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6.6.2 Calculation object from to
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Tip To combine calculated data and
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max var. max of all arguments sum v
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6.7.3 Software set-up Once A/D-hard
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Figure 6-76 BSA F/P application win
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6.7.7 Analog input specifications J
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6.8.1 Installation 6.8.2 Hardware c
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Figure 6-85 BSA F/P application win
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6.9.1 Required hardware 6.9.2 Calib
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2. Select Parameter Input 3. The fo
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B. Select Advanced Curve fitting an
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6.10 Mobile system Monitor option T
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7. Reference guide 7.1 Theory of La
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Doppler effect d0 R(z) Figure 7-1 L
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es e2 e1 U Figure 7-3 Scattering of
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Measuring volume proportional to pa
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Laser fI Beam splitter As indicated
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7.1.6 Frequency shift • Reduce th
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As long as the particle velocity do
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7.1.7 Signals The primary result of
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7.1.8 Seeding Seeding as flow field
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150 90 180 0 180 0 180 0 210 120 24
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7.2 Theory of Phase Doppler Anemome
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D is the particle diameter. βi is
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For reflection (Equation 7-16) The
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Figure 7-21: The effect of changing
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This is the principle of the spheri
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The trajectory effect The slit effe
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Figure 7-28:The DualPDA as a combin
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Figure 7-31: Reflection and refract
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Characteristic scattering angles At
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⎛ ϕ ⎞ ϕ2 = 4arcsin⎜ ⎟ −
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Figure 7-36: The critical angle con
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Using side scatter (reflected light
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Mask Front Lens Eye-piece Spatial f
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Alignment of the eyepiece The focus
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This is often not necessary in 1D a
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For both orientations of polarizati
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Figure 7-46. The effect of changing
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Table of characteristic angles Defi
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n rel ϕ c1 ϕ b0 ϕ c2 ϕ b2 ϕ r2
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Choice of wavelength Choice of mask
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Choice of wavelength and focal leng
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Choice of polarization Choice of sc
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Focal length Transmitter (FiberFlow
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Polarization ring Fixing screw Push
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Aperture plates The particle size r
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Tighten the cable securely at each
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Disconnect the receiving fiber V1 f
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Step by step procedure Phase-Dopple
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Lower half: The lower half of the b
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Recommended acceptance angles of th
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7.7.4 Air bubble in freon Character
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7.7.6 Bubble of air in diesel oil C
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7.7.8 Glass sphere in water Charact
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7.7.10 Latex sphere in water Charac
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Blocking increases calculation spee
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In this particular example we get:
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7.9 Moments (one-time statistics) 7
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1 = N Mean D mean ui (7-31) N ∑
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Software implementation Updating me
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u v 2 2 = = ∑ ∑ tU tV 2 2 − 2
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(histogram properties). ni is the n
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volume is calculated for the class
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D30 The volume mean diameter is cal
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Three further factors are however i
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d e ln 2 max 2 V do ∗ Vt = ( 7-48
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Diameter bins The number of diamete
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Trajectory dependent detection area
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Corrected particle Max d e ( Di ) C
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Integral time-scale τI Definition
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The mean values of u(t) and v(t) ar
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Low pass filtering & Step noise Obv
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fc ≡ t 1 2 ∆ If the true signal
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Estimator bias Estimator variance S
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-again S’(f) is used to distingui
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Zero padding Often the sampling per
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As an example the Hanning window is
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The Explorer window will now look s
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8.2.2 Peer-to-Peer Configuration Co
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. High Voltage or Figure 8-3: Calib
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Invalid particles in the corners Th
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Gaussain beam effect The following
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To check for connection, right-clic
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