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???S? TiO2 S? ?????? ????? G?? ??? FO???????????? ?????????S? ????SF?????O? ???O?

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Similar 2-D sonic anemometer/thermometers were mounted at the 4-, 8- and 16-m ... deviations of the velocity fluctuations in the x, y, z directions: , , and ... – PowerPoint PPT presentation

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Title: ???S? TiO2 S? ?????? ????? G?? ??? FO???????????? ?????????S? ????SF?????O? ???O?


1
FIELD EXPERIMENT MUST Short Term Scientific
Mission, COST 732
Efthimiou George1, Silvia Trini Castelli2, Tamir
Reisin3 31 March - 5 April 2008, Torino,
Italy 1Department of Engineering and Management
of Energy Resources, University of West
Macedonia, Kozani, Greece 2Institute of
Atmospheric Sciences and Climate National
Research Council, Torino, Italy 3SOREQ NRC,
Yavne, Israel
Thessaloniki 13-14 May 2008
2
Purpose of this STSM
  • Mock Urban Setting Test (MUST) is one of the most
    successful field experiment containing a rich and
    comprehensive dataset. Largely used by the
    scientific community, it includes detailed
    information about tracer concentrations and
    turbulence.
  • COST 732 WGs used mainly Wind Tunnel data
    (Bezpalcova, 2005).
  • The purpose of this STSM was to process the field
    campaigns data in order to prepare a specific
    data set to further validate CFD and non-CFD
    codes for the field experiment conditions.

3
Description of the work carried out during the
visit
  • General description of the MUST field experiment
    (buildings, equipment).
  • Examination of existing meteorological and
    concentration data sets.
  • Development of software to handle data.
  • Processing of Velocity and Concentration Time
    Series Statistics.

4
General description of the MUST field experiment
(buildings, equipment)
  • The geometry and the coordinates of the Wind
    Tunnel experiment is supposed to be the same as
    used in the Field experiment 0 degree case.
    Accordingly
  • The Shipping Containers.
  • The VIP van for the collection of wind and
    concentration data.
  • The 32-m tower near the centre of the container
    array.
  • The 6-m towers in each of the four quadrants.
  • The measurements of concentrations in the four
    sampling lines.

5
Meteorological Measurements Tracer Detection
  • Concentration Measurements
  • Ultraviolet Ion Collectors (UVIC).
  • Digital Photoionization Detection (digiPID).
  • Meteorological Measurements
  • Dugway Proving Ground (DPG) data.
  • Defense Science and Technology Laboratory (DSTL)
    data.

6
Ultraviolet Ion Collectors (UVIC)
  • These files include time series of concentration
    in ppm with time interval 0.01s.
  • There are 24 UVICS mounted
  • on the four 6-m towers
  • A, B, C, D.
  • On each of these 6-m towers,
  • 6 UVICs were deployed at the
  • following levels
  • 1, 2, 3, 4, 5 and 5.9 m.

Yee, E. and Biltoft, 2004
7
Ultraviolet Ion Collectors (UVIC)
  • There are 2 other files
  • Tip.dat (2 m above the
  • ground on the 32 m
  • tower)
  • Wake.dat (2 m above the
  • ground, 1m behind the
  • center of the building H4)

Yee, E. and Biltoft, 2004
8
Digital Photoionization Detection (digiPID)
  • These files include time series of concentration
    in ppm with time interval 0.02s.
  • There are 48 ascii files which correspond to
    horizontal and vertical profiles of
    concentration.
  • Horizontal profiles of concentration fluctuations
    were measured using 40 dPIDs which were arrayed
    along the four horizontal sampling lines that
    were parallel to and centred in the street
    canyons.
  • The concentration detectors along the four
    horizontal sampling lines were placed at a height
    of 1.6 m.

9
Digital Photoionization Detection (digiPID)
  • Vertical profiles of concentration statistics
    were characterized by 8 dPIDs deployed on the
    32-m lattice tower near the centre of the
    obstacle array at heights of 1m, 2m, 4m, 6m, 8m,
    10m, 12m, and 16m.

Yee, E. and Biltoft, 2004
10
DPG wind data
  • These files include time series of velocities and
    temperature with time interval 0.1s.
  • Measurements of the vertical profiles of the mean
    horizontal wind velocity and temperature in the
    upwind flow obtained from a 16-m telescoping
    pneumatic mast.
  • Similar 2-D sonic anemometer/thermometers were
    mounted at the 4-, 8- and 16-m levels of a 16-m
    pneumatic mast downwind of the back of the
    obstacle array.
  • Vertical profiles of mean wind speed and
    temperature were obtained from the 32-m lattice
    tower located near the center of the obstacle
    array.

11
DPG wind data
  • Also there are 4 more positions with measurements
    inside the domain.
  • V2 In front of the
  • building G5 1.15m
  • V4 Between the buildings
  • G6 and G7 1.15m
  • V3 Between the buildings
  • G6 and H6 1.15m
  • V1 2.5m Northwest of the
  • building ?6 1.15m

Yee, E. and Biltoft, 2004
12
DSTL wind data
  • These files include time series of velocities and
    temperature with time interval 0.05s.
  • There are 8 ascii files which correspond to
    velocities and temperatures at heights 2 and 6 m.
  • These data belongs to the four towers A, B, C, D.

13
Examination of existing meteorological and
concentration data sets
  • There are two main sets of data acquired during
    the trials, namely
  • The dispersion data which were obtained using 74
    high-speed photoionization detectors (48 DPIDs
    and 26 UVICs).
  • The meteorological dataset (i.e. the wind
    velocity and sonic temperature), which was
    obtained using 22 sonic anemometers (14 DPG and 8
    DSTL).

14
Examination of existing meteorological and
concentration data sets
  • We selected a first sub-set of data, collected
    during two days (25 and 26 September 2001) and
    corresponding to a neutrally stratified
    atmospheric surface layer (ASL) according to
    Monin Obukhov Length.
  • We chose the experiment that corresponds to the
    release starting at 1830 and ending at 1845 on
    25 of September 2001.

15
Development of software to handle data
  • A tailored Fortran code was written as a flexible
    tool that allows reading the time series of
    velocities, concentration and temperature, thus
    calculating mean values and variances for any
    averaging time, chosen by the user.
  • The output files, as time series and averaged
    fields can be used by the COST WGs, CFD and
    non-CFD, for numerical model simulation.

16
Processing of Velocity and Concentration Time
series - Statistics
  • The concentration time series were acquired over
    sampling times of 15 minutes for most of the
    continuous release experiments.
  • The MUST dataset authors made the following
    processing of the data
  • Because background meteorological conditions may
    change over the 15-minute sampling time duration,
    it was necessary to apply conditional sampling to
    the concentration time series.

17
Processing of Velocity and Concentration Time
series - Statistics
  • For this reason they extracted 3- to 5- minute
    period from each record of 15-minute duration
    with a minimal variation of mean wind direction.
  • Finally they used this 3- to 5- minute period as
    the standard sampling period for computation of
    the plume concentration statistics.

18
Processing of Velocity and Concentration Time
series - Statistics
  • According to the above, two periods from trial 25
    September 2001 were chosen for analysis.
  • These two periods (100-900 seconds and 300-500
    seconds) were the same both for velocities and
    concentrations and primarily based on the
    stationarity (i.e., speed and direction) of the
    wind over the period.

19
Processing of Velocity and Concentration Time
series - Statistics
Mean value -40.55o
20
Processing of Velocity and Concentration Time
series - Statistics
  • We performed the same analysis on the original
    data as carried out by the MUST data referees,
    checked and compared our results with their
    averaged data.
  • For velocities and temperatures we chose also to
    analyze a 30 minutes period and we calculated the
    statistics producing a time series of data
    averaged over one minute. For concentrations we
    performed an analogous analysis but for a period
    of 17 minutes.

21
Processing of Velocity and Concentration Time
series - Statistics
Velocities Temperatures 100-900 seconds
(183040 184400), values averaged over 800
s 300-500 seconds (183400 183720), values
averaged over 200 s 30 minutes period (181500
184500), time series of data averaged over 1
minute
22
Processing of Velocity and Concentration Time
series - Statistics
  • Velocities Temperatures
  • For each data record from each sonic anemometer,
    we computed the following quantities
  • Mean velocity in each direction , , and
    (m s-1). Note that W is not available for the
    two-axis sonic anemometers mounted on the
    pneumatic masts just upstream and downstream of
    the MUST array.
  • Mean direction
  • Velocity standard deviations of the velocity
    fluctuations in the x, y, z directions
    , , and
  • (m s-1).

23
Processing of Velocity and Concentration Time
series - Statistics
  • Velocities Temperatures
  • Turbulence kinetic energy
  • Mean temperature (K)
  • Covariances and .
  • Temperature flux in ms-1K.
  • Friction velocity

24
Processing of Velocity and Concentration Time
series - Statistics
  • Velocities Temperatures
  • Local free convection velocity scale
    where g9.8 m s-2 and z is the
    height (m) of the anemometer above the ground
    surface.
  • Monin-Obukhov length where ? 0.4 von
    Karmans constant.
  • Sensible heat flux (W
    m-2) where ?1.2 kg m-3 is density of air, and
    Cpa1005 J kg-1K-1 is specific heat capacity of
    dry air at constant pressure.

25
Processing of Velocity and Concentration Text
Files
Meteorological variables (200s)
26
Processing of Velocity and Concentration Text
Files
Meteorological variables (15 min)
27
Meteorological plots
  • Velocity U, V, W
  • Direction
  • Temperature
  • Turbulence Kinetic Energy

28
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29
?
0
30
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38
Calculation of turbulence kinetic energy in
upwind mast (consistency check)
  • Because the upwind mast consists only from 2-D
    sonic anemometer-thermometer we did not have the
    3rd component of velocity (w) and we calculate
    Turbulent Kinetic Energy in four ways
  • We calculate first the time series of the
    variances of the velocities fluctuations ,
    . Then we calculate the time series of
    turbulent kinetic energy according to the
    relation
  • and finally

39
Calculation of turbulence kinetic energy in
upwind mast
  • Like in the first way but this time we account
    also for the prime of velocity w?w? according to
    the relation
  • (Yee and Biltoft, 2004).
  • The time series of turbulent kinetic energy
    becomes

40
Calculation of turbulence kinetic energy in
upwind mast
  • In the following process we calculate the mean
    values of the standard deviations of wind
    velocity fluctuations and denoted as varu,
    varv where

41
Calculation of turbulence kinetic energy in
upwind mast
  • Like in the third way but at this time we account
    also the mean value of the prime w?w? according
    to the relation
  • (Yee and Biltoft, 2004) and the mean value
    of turbulent kinetic energy becomes

South Tower Numerical Simulation South Tower Numerical Simulation South Tower Numerical Simulation South Tower Numerical Simulation South Tower Numerical Simulation

4m 2.245630 1.935884 2.245626 1.935884
8m 2.199033 1.895721 2.199036 1.895720
16m 1.974085 1.701799 1.974081 1.701794
42
Calculation of turbulence kinetic energy -
mistakes
  • From the MUST data we noticed that turbulent
    kinetic energy in the statistics file is
    erroneously calculated as follows

South Tower MUST data South Tower MUST data

4m 0.98388
8m 0.97364
16m 0.92248
43
Calculation of turbulence kinetic energy -
mistakes
The part of the script DPGSONIC.MAT which refers
to TKE   Ubar mean U / mean x
component/ \ Vbar mean V / mean y
component/ \ Wbar mean W / mean z
component/ \ Tbar mean T / mean
temperature/ \ Abar RADTOD atan Ubar
Vbar / mean bearing (deg)/ \ Sbar
sqrtUbarUbarVbarVbar / mean wind
speed/ \ / compute deviations from mean/ \
dU U - Ubar dV V - Vbar dW
W - Wbar dT T - Tbar dA A
- Abar / compute variances/ \ U2
meandU dU V2 meandV dV W2
meandW dW T2 meandT dT
A2 meandA dA
44
Calculation of turbulence kinetic energy -
mistakes
/ compute standard deviations/ \ U1
sqrt U2 V1 sqrt V2 W1
sqrt W2 T1 sqrt T2 A1
sqrt A2 TKE 0.5sqrt
U2V2W2 / turbulent kinetic energy / \
45
Calculation of mean direction - mistakes
  • In the file explaining how to calculate the
    direction they suggest first to calculate the
    instantaneous direction and then to average these
    time series to obtain the mean value.
  • The procedure described does not output the
    values as in the file of statistics M2681829.
  • We apply the correct way to average the wind
    direction for every averaging period, we
    calculated the mean values of wind components and
    after calculate the corresponding wind direction
    on the averaged and

46
Processing of Velocity and Concentration Time
series - Statistics
Concentrations 100-900 seconds (183040
184400) , values averaged over 800 s 300-500
seconds (183400 183720) , values averaged
over 200 s 17 minutes period (182900
184600), time series of data averaged over 1
minute
47
Processing of Velocity and Concentration Time
series - Statistics
  • Concentrations
  • After the conditional sampling of concentration,
    we computed the following concentration
    statistics
  • Mean concentration (ppm).
  • Concentration standard deviation of the
    concentration fluctuation
  • Concentration fluctuation intensity

48
Processing of Velocity and Concentration Text
Files
Concentrations (200s)
49
Processing of Velocity and Concentration Text
Files
Concentrations (17 min)
50
Concentration plots
  • Mean concentration

51
Inflow wind
52
Inflow wind
53
Inflow wind
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Further discussion
  • Except from the known measurements points in COST
    there are others for which we have the data but
    we do not know their exact positions inside the
    domain.

Milliez and Carissimo, 2008
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