NOTICE DATED NOVEMBER, 1999:
United States National Weather Service (NWS) upper-air stations using the Sippican, Incorporated VIZ-B2 radiosonde will implement additional coefficients in the algorithm used to compute relative humidity (RH). NWS supported stations in the Caribbean using this radiosonde will also implement these coefficients. The new coefficients improve the accuracy of RH measurements at high and low RH. Starting about October 15, 1999, NWS stations using the VIZ-B2 radiosonde began phasing over to radiosondes with the new coefficients. This activity will be completed by about December 1, 1999.
NWS UPPER-AIR STATIONS
IMPLEMENTING
NEW COEFFICIENTS FOR COMPUTING RELATIVE HUMIDITY
|
INTERNATIONAL INDEX NUMBER |
STATION |
||
|
Contiguous United States |
|||
|
72365 |
Albuquerque, NM |
||
|
72764 |
Bismarck, ND |
||
|
72250 |
Brownsville, TX |
||
|
72712 |
Caribou, ME |
||
|
72251 |
Corpus Christi, TX |
||
|
72261 |
Del Rio, TX |
||
|
72387 |
Desert Rock, NV |
||
|
72451 |
Dodge City, KS |
||
|
72582 |
Elko, NV |
||
|
72768 |
Glasgow, MT |
||
|
72776 |
Great Falls, MT |
||
|
72645 |
Green Bay, WI |
||
|
72235 |
Jackson, MS |
||
|
72201 |
Key West, FL |
||
|
72597 |
Medford, OR |
||
|
72327 |
Nashville, TN |
||
|
72493 |
Oakland, CA |
||
|
72520 |
Pittsburgh, PA |
||
|
72797 |
Quillayute, WA |
||
|
72694 |
Salem, OR |
||
|
72293 |
San Diego, CA |
||
|
78526 |
San Juan, PR |
||
|
72786 |
Spokane, WA |
||
|
Alaska |
|||
|
70398 |
Annette |
||
|
70026 |
Barrow |
||
|
70308 |
St. Paul Island |
||
|
Carribean |
|||
|
78583 |
Belize City, Belize |
||
|
78954 |
Barbados |
||
|
78384 |
Grand Cayman |
||
|
Pacific Islands |
|||
|
91217 |
Guam, Mariana Is. |
||
|
91285 |
Hilo, HI |
||
|
91376 |
Majuro, Marshall Is. |
Sippican
Carbon Hygristor Data Processing using H1 and H2
Introduction
The
Sippican, Inc., VIZ-B2 radiosonde employs three coefficients to process the relative humidity (RH)
sensor (i.e., carbon hygristor) data.
The three calibration factors are: lock-in, H1, and H2.
These factors provide the original primary calibration setting (lock-in),
a new “H1” calibration coefficient to the high end of the RH range (values
> 33% RH), and a new “H2” calibration coefficient to the low end of the
RH range (values< 33% RH). The
processing algorithm uses these calibration factors to provide RH output that
best matches the sensor calibration data. The
factors are required to adjust for process and material fluctuations built into
the final sensor.
Processing
The first of the three calibration factors is the lock-in value. The lock-in is the sensor’s electrical resistance at 33% RH and 25O C. This is the original calibration factor (used for many years) and is the most fundamental of the factors supplied. For any hygristor, the lock-in is established based on the original resistance read at cut-in (cut-in is the process of bringing the sensor resistance into predetermined range during production by physically cutting the conductive surface to adjust the resistance), and calibration data from a sample of hygristors from the same lot, run in a precision RH calibration chamber. The use of the lock-in factor without the incorporation of the additional factors provides a good average response algorithm. However the algorithm does not provide the most accurate response for all sensors produced.
The H1 factor is a value used to remove bias at high RH (values > 33%) found in the calibration data. There is no change from the nominal curve at the high RH end for sensors with H1 set to a value of one. Hygristors with resistance versus RH higher than normal above 33% RH incorporate a lower H1 factor (less than 1.0) to accurately calculate RH. Inversely, a higher H1 factor (greater than 1.0) is used to accurately calculate RH when the resistance versus RH curve above 33% RH has a lower resistance than normal. The effect of H1 is weighted, with no effect at 33% RH and maximum effect at 100% RH (see equation 1).
The H2 factor is a ratio number used to remove any bias at low RH (values < 33%) found in the calibration data. There is no change from the nominal curve at low RH end for sensors with H2 set to one. Hygristors with resistance higher than the norm below 33% RH incorporate a higher H2 factor (greater than 1.0) to most accurately calculate RH. Inversely, a lower H2 factor (less than 1.0) is used to accurately calculate the RH when the resistance vs. RH curve below 33% RH has a lower resistance than the norm. The effect of H2 is weighted, with no effect at 33% RH and maximum effect at 0% RH (see equation 1).
H1 and H2 are optimized by averaging the absolute error of all 25oC and –10oC calibration data points for a given lot and then minimizing that average.
Examples
For B2 radiosondes with H1 and H2 factors optimized at H1=0.9 and H2=0.9 the accuracy improvement over the non-optimized algorithm (H1 and H2=1) is +2.64% RH at 10 % RH and –2.48% RH at 90% RH.
For B2 radiosondes with H1 and H2 factors optimized at H1=1.1 and H2=1.1 the accuracy improvement over the non-optimized algorithm (H1 and H2=1) is –2.77% RH at 10% RH and +2.39% RH at 90% RH.
Conclusion
Sippican, Inc., has developed these algorithms and the related procedures to obtain the required calibration factors from RH chamber testing. Chamber tests have shown that the RH calculations are improved by implementing the H1 and H2 calibration factors.
The most important variable used in the resistance-to-RH algorithm is the ratio of sensor resistance, Rs, to sensor lock-in resistance, Rlock-in,
Ratio = Rs / Rlock-in.
Rlock-in is the sensor resistance at +25°C and at a RH with respect to water of 33%. Rlock-in is specific to each sensor and is “locked in” during the manufacturing process to have a nominal value around 10 KΩ. Rs has a relatively small dependence on the temperature, and historically it has been found that at 33% RH the response of the sensor to changes in temperature is particularly small. This is the reason why it is the 33% RH that is “locked in”. We therefore characterize the overall behavior of the sensor resistance using the value of Ratio instead of Rs.
The main function in the resistance-to-RH algorithm is a family of curves (the quantity raised to the kth power in Equation No. 1 below), with one member of the family for every temperature. Each member describes the response of the sensor to RH at a particular temperature. The following two equations have been found to accurately match this family of curves and so are used to convert sensor resistance into relative RH for all temperatures.
Equation No.1
6
RH = A -
k=0
where,
RH = calculated percent relative humidity with respect to water
A = A1, H * g(T) * ln(Ratio) ≥ -0.2
= A2, H * g(T) * ln(Ratio) < -0.2
B = 69
Dk = D1k, H * g(T) * ln(Ratio) ≥ -0.2
= D2k, H * g(T) * ln(Ratio) < -0.2
g(T) = a function of temperature given in Equation No. 2; this function specifies the member of the family for curves at temperature T
H = H1, Ratio ≥ 1 (constant in the calibration data with VIZ system software)
= H2, Ratio < 1 (constant in the calibration data)
T =
temperature in degrees C
Equation No. 2
g( T ) = Σ
Ck * Tk
k=0
where,
Ck = a set of six calibration constants, each assuming one value when
Ratio ≥ 1 and another when Ratio < 1
T = temperature in degrees C.
The sensor response to RH at +25°C is particularly well documented and this curve is especially important. The H and Dk coefficients in Equation No. 1 are fitted to experimental data on this +25°C curve. Because the g in Equation No. 2 equals 1.00 when T =+25°C, Equation No. 1 reduces to this best-fit curve at that temperature. The Ck’s in Equation No. 2 are best-fit coefficients to experimental data at temperatures other than at +25°C.
The carbon-based RH sensor response can be accurately matched using the following coefficients in Equation No. 1.:
H * g(t) * ln(Ratio) > -0.2
H * g(t) * ln(Ratio) <
-0.2
D1
= 7.290E-01 D1 = 7.290E-01
D2
= -5.580E-02 D2 =-5.580E-02
D3
= 7.480E-03 D3 = 7.480E-03
D4
= 1.010E-02 D4 = 1.010E-02
D5
= 0.0 D5 = 0.0
D6
= 0.0 D6 = 0.0
A = 1.02E+02
A = 1.02E+-2
B = 69
B = 69
Equation No. 2A
Equation No. 2B
Rs > R33 (Ratio >1) Rs < R33 (Ratio < 1)
C0 =
7.885E-01 C0 = 9.243E-01
C1
= 9.286E-03 C1 = 3.059E-03
C2
= -2.462E-05 C2 = -1.188E-06
C3
= -3.368E-07 C3 = 0.0
C4
= 0.0 C4 = 0.0
C5
= 0.0 C5 = 0.0
NOTICE DATED DECEMBER, 1998:
The code group on cloud information will be found between the 31313 and 51515 groups in the Part B or "TTBB" message and will be encoded as follows:
41414 NhCLhCMCH
Where,
Nh = Amount of all CL cloud present or, if no CL is present, the amount of all CM cloud present in eighths of cloud cover. Code figures 0 through 9 and / are used to define cloud types as defined by a code table.
CL = Type of low cloud present.
h = Height above surface of the lowest cloud seen as defined by a code table.
CM = Type of mid-level cloud present.
CH = Type of high-cloud present.
Reference: WMO No. 306 Manual on Codes, Vol 1.1, Sections A and B.
Back to the Upper-air Observations Main Page