BSA Flow Software Installation and User's Guide - CSI

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4.10.5 Data rate requirements Below are some recommendations. For a detailed description, please consult the Reference guide chapter. Mean and RMS velocity 4.10.6 Stop criterion possibilities If you are looking for average quantities such as mean and RMS velocity, the data rate is not critical, but you should acquire sufficient samples for reliable statistics. This usually means 1000 - 2000 samples per position, but depends on the flow characteristics. To avoid statistical bias, you can use the Controlled Dead Time mode, with the Dead Time interval set to at least 2 times the integral time scale of the flow. Alternatively, you can use burst mode and select Transit Time Weighting in the Moments object. Time series, spectrum and correlation functions For this type of results where the dynamics of fluctuations is investigated, the data rate should obviously be high. If you expect a dominant frequency in a spectrum, the data rate should ideally be around 2 π times the highest frequency you are looking for since the spectrum will fall off at a frequency of mean data rate/2 π. If you cannot achieve such data rate, the optical system must be optimised in terms of laser power, receiving optics aperture, and use of forward scatter if possible. Changing from backscatter to forward scatter typically increases the data rate by at least an order of magnitude. BSA Flow software includes several stop criteria to stop the acquisition: • Sample numbers to stop when the acquired sample numbers is reached (see group properties in chapter 5). • Acquisition time to stop when the acquisition time is reached (see group properties in chapter 5). • Statistical stop criteria to stop the acquisition on the confidence (see using confidence limits as stop criteria for data acquisition in chapter 5). • Cyclic phenomena stop criteria to stop the acquisition either on a number on particles per phase bin or on the cycle numbers (see Properties of the Cyclic Phenomena Object in chapter 6. Note Please note that multiple stop criteria can be made inside the same project: sample number, elapsed time, etc. The acquisition will stop based on the criterion met first. 4.11 How to add new data to a project In BSA Application, add the new positions to the position co-ordinates list, either by typing into the list, or by adding a new region, and using the Mesh Generator to define the new positions. Click the Run button. Click Run in the Data Overwrite Warning window. In the Ready to Acquire… window, select Positions, and specify the indices of the new positions: 4-62 BSA Flow Software: The user interface
Click Acquire. If a complete new region was added, choose accordingly in the above dialog box. BSA Flow Software: The user interface 4-63
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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
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You have the possibility to define
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Click Next and select the add-ons y
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Peer-to-peer connection Processor s
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Click on the Download tab to get th
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The BSA processor will restart. Thi
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• If the Game controller needs to
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Figure 3-2 National Instruments Mea
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3.7 Third party traverse system To
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4. The user interface 4.1 Layout Me
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4. If the mouse pointer was in the
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4.3 Project explorer shortcuts to t
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Figure 4-5 Dialog for adding object
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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 and 76: LDA and PDA transmitting optics The
Page 77 and 78: Click on OK. Note For fully opaque
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: The axes will automatically rescale
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
Page 127 and 128: LDA 1, 2, . properties: Range and g
Page 129 and 130: 5.3.4 System monitor It frequently
Page 131 and 132: Scope: Burst spectrum display Recor
Page 133 and 134: Overlaid Graphs: used to show the b
Page 135 and 136: Uncheck the Use default bindings bo
Page 137 and 138: The calibration data are stored in
Page 139 and 140: 5.6.1 PDA beam system The Beam syst
Page 141 and 142: Figure 5-24: Fringe direction setti
Page 143 and 144: 5.6.4 Medium properties Medium name
Page 145 and 146: Software max. limit in mm.: Self ex
Page 147 and 148: The default address of the National
Page 149 and 150: Traverse coordinates of a datum poi
Page 151 and 152: 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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