apogee SI-4H1 Infrared Radiometers Owner’s Manual
- June 3, 2024
- APOGEE
Table of Contents
OWNER’S MANUAL
INFRARED RADIOMETER
Models SI-411, SI-421, SI-431, and SI-4H1
(including SS models)
APOGEE INSTRUMENTS, INC.
721 WEST 1800 NORTH, LOGAN, UTAH 84321, USA TEL:
435-792-4700 | FAX:
435-787-8268
WEB: APOGEEINSTRUMENTS.COM
DECLARATION OF CONFORMITY
EU Declaration of Conformity
This declaration of conformity is issued under the sole responsibility of
the manufacturer:
Apogee Instruments, Inc. 721 W 1800 N
Logan, Utah 84321 USA
for the following product(s):
Models: SI-411, SI-421, SI-431, SI-4H1 Type: Infrared Radiometer
The object of the declaration described above is in conformity with the relevant Union harmonization legislation:
2014/30/EU Electromagnetic Compatibility (EMC) Directive
2011/65/EU Restriction of Hazardous Substances (RoHS 2) Directive
Standards referenced during compliance assessment:
EN 61326-1:2013 Electrical equipment for measurement, control and laboratory
use EMC requirements
EN 50581:2012 Technical documentation for the assessment of electrical and
electronic products with respect to the restriction of hazardous substances
Please be advised that based on the information available to us from our raw
material suppliers, the products manufactured by us do not contain, as
intentional additives, any of the restricted materials including cadmium,
hexavalent chromium, lead, mercury, polybrominated biphenyls (PBB),
polybrominated diphenyls (PBDE).
Further note that Apogee Instruments does not specifically run any analysis on
our raw materials or end products for the presence of these substances, but
rely on the information provided to us by our material suppliers.
Signed for and on behalf of:
Apogee Instruments, May 2016
Bruce Bugbee
President
Apogee Instruments, Inc.
INTRODUCTION
All objects with a temperature above absolute zero emit electromagnetic
radiation. The wavelengths and intensity of radiation emitted are related to
the temperature of the object. Terrestrial surfaces (e.g., soil, plant
canopies, water, snow) emit radiation in the mid infrared portion of the
electromagnetic spectrum (approximately 4-50 µm).
Infrared radiometers are sensors that measure infrared radiation, which is
used to determine surface temperature without touching the surface (when using
sensors that must be in contact with the surface, it can be difficult to
maintain thermal equilibrium without altering surface temperature). Infrared
radiometers are often called infrared thermometers because temperature is the
desired quantity, even though the sensors detect radiation.
Typical applications of infrared radiometers include plant canopy temperature
measurement for use in plant water status estimation, road surface temperature
measurement for determination of icing conditions, and terrestrial surface
(soil, vegetation, water, snow) temperature measurement in energy balance
studies.
Apogee Instruments SI series infrared radiometers consist of a thermopile
detector, germanium filter, precision thermistor (for detector reference
temperature measurement), and signal processing circuitry mounted in an
anodized aluminum housing, and a cable to connect the sensor to a measurement
device. All radiometers also come with a radiation shield designed to minimize
absorbed solar radiation, but still allowing natural ventilation. The
radiation shield insulates the radiometer from rapid temperature changes and
keeps the temperature of the radiometer closer to the target temperature.
Sensors are potted solid with no internal air space and are designed for
continuous temperature measurement of terrestrial surfaces in indoor and
outdoor environments. SI-400 series sensors output a digital signal using
SDI-12 protocol version 1.3.
SENSOR MODELS
Model | Output |
---|---|
SI-400 Series | SDI-12 |
SI-100 Series | Voltage |
Sensor model number and serial number are located on a label near the pigtail leads on the sensor cable. If you need the manufacturing date of your sensor, please contact Apogee Instruments with the serial number of your sensor.
The four FOV options and associated model numbers are shown below:
SPECIFICATIONS
| SI-411| SI-421| SI-431| SI-4H1
---|---|---|---|---
Input Voltage Requirement| 5.5 to 24 V DC
Current Drain| 0.6 mA (quiescent),1.3 mA (active)
Calibration Uncertainty (-20 to 65 C),
when target and detector temperature are
within 20 C| 0.2 C| 0.2 C| 0.3 C| 0.2 C
Calibration Uncertainty (-40 to 80 C),
when target and detector temperate are
different by more than 20 C
(see Calibration Traceability below)| 0.5 C| 0.5 C| 0.6 C| 0.5 C
Measurement Repeatability| less than 0.05 C
Stability (Long-term Drift)| less than 2 % change in slope per year when
germanium filter is maintained in a
clean condition (see Maintenance and Recalibration section below)
Response Time| 0.6 s, time for detector signal to reach 95 % following a step
change; fastest data
transmission rate for SDI-12 circuitry is 1 s
Response Time| 22º half angle| 18º half angle| 14º half angle| 32º horizontal
half
angle; 13º vertical
half angle
Spectral Range| 8 to 14 µm; atmospheric window (see Spectral Response below)
Operating Environment| -45 to 80 C; 0 to 100 % relative humidity (non-
condensing)
Dimensions| 23 mm diameter; 60 mm length
Mass| 190 g (with 5m of lead wire)
Cable| 5 m of two conductor, shielded, twisted-pair wire; additional cable
available in
multiples of 5 m; santoprene rubber jacket (high water resistance, high UV
stability,
flexibility in cold conditions); pigtail lead wires
Calibration Traceability
Apogee SI series infrared radiometers are calibrated to the temperature of a
custom blackbody cone held at multiple fixed temperatures over a range of
radiometer (detector/sensor body) temperatures. The temperature of the
blackbody cone is measured with replicate precision thermistors thermally
bonded to the cone surface. The precision thermistors are calibrated for
absolute temperature measurement against a platinum resistance thermometer
(PRT) in a constant temperature bath. The PRT calibration is directly
traceable to the NIST.
Spectral Response
Spectral response of SI series infrared radiometers. Spectral response (green
line) is determined by the germanium filter and corresponds closely to the
atmospheric window of 8-14 µm, minimizing interference from atmospheric
absorption/emission bands (blue line) below 8 µm and above 14 µm. Typical
terrestrial surfaces have temperatures that yield maximum radiation emission
within the atmospheric window, as shown by the lackbody
curve for a radiator at 28 C (red line).
DEPLOYMENT AND INSTALLATION
The mounting geometry (distance from target surface, angle of orientation
relative to target surface) is determined by the desired area of surface to be
measured. The field of view extends unbroken from the sensor to the target
surface. Sensors must be carefully mounted in order to view the desired target
and avoid including unwanted surfaces/objects in the field of view, thereby
averaging unwanted temperatures with the target temperature (see Field of View
below). Once mounted, the green cap must be removed. The green cap can be used
as a protective covering for the sensor, when it is not in use.
An Apogee Instruments model AM-210 mounting bracket is recommended for
mounting the sensor to a cross arm or pole. The AM-210 allows adjustment of
the angle of the sensor with respect to the target and accommodates the
radiation shield designed for all SI series infrared radiometers.
Field of View
The field of view (FOV) is reported as the half-angle of the apex of the cone
formed by the target surface (cone base) and the detector (cone apex), as
shown below, where the target is defined as a circle from which 98 % of the
radiation detected by the radiometer is emitted.
Sensor FOV, distance to target, and sensor mounting angle in relation to the
target will determine target area.
Different mounting geometries (distance and angle combinations) produce
different target shapes and areas, as shown below.
A simple FOV calculator for determining target dimensions based on infrared radiometer model, mounting height, and mounting angle, is available on the Apogee website: http://www.apogeeinstruments.com/using-your- apogeeinstruments-infrared-radiometer/.
CABLE CONNECTORS
Apogee started offering in-line cable connectors on some bare-lead sensors in
March 2018 to simplify the process of removing sensors from weather stations
for calibration by not requiring the full cable to be uninstalled back to the
data logger.
The ruggedized M8 connectors are rated IP67, made of corrosion-resistant
marine-grade stainless-steel, and designed for extended use in harsh
environmental conditions.
Instructions
Pins and Wiring Colors: All Apogee connectors have six pins, but not all
pins are used for every sensor. There may also be unused wire colors inside
the cable. To simplify data logger connection, we remove the unused pigtail
lead colors at the data logger end of the cable.
If you ever need a replacement cable, please contact us directly to ensure
ordering the proper pigtail configuration.
Alignment: When reconnecting your sensor, arrows on the connector jacket
and an aligning notch ensure proper orientation.
Disconnection for extended periods: When disconnecting the sensor for an
extended period of time from a station, protect the remaining half of the
connector still on the station from water and dirt with electrical tape or
other method.
Tightening: Connectors are designed to be firmly finger-tightened only.
There is an o-ring inside the connector that can be overly compressed if a
wrench is used. Pay attention to thread alignment to avoid crossthreading.
When fully tightened, 1-2 threads may still be visible.
Inline cable connectors are installed 30 cm from the head (pyranometer pictured)
A reference notch inside the connector ensures proper alignment before tightening.
When sending sensors in for calibration, only send the short end of the cable and half the connector.
Finger-tighten firmly
OPERATION AND MEASUREMENT
All SI-400 series radiometers have an SDI-12 output, where target and detector
temperatures are returned in digital format. Measurement of SI-400 series
radiometers requires a measurement device with SDI-12 functionality that
includes the M or C command.
VERY IMPORTANT: Apogee changed all wiring colors of our bare-lead sensors
in March 2018 in conjunction with the release of inline cable connectors on
some sensors. To ensure proper connection to your data device, please note
your serial number or if your sensor has a stainless-steel connector 30 cm
from the sensor head then use the appropriate wiring configuration below.
Wiring for SI-400 Series with Serial Numbers range 0-3056
Wiring for SI-400 Series with Serial Numbers 3057 and above or with a cable connector
Sensor Calibration
Apogee SI series infrared radiometers are calibrated in a temperature
controlled chamber that houses a custombuilt blackbody cone (target) for the
radiation source. During calibration, infrared radiometers (detectors) are
held in a fixture at the opening of the blackbody cone, but are thermally
insulated from the cone. Detector and target temperature are controlled
independently. At each calibration set point, detectors are held at a constant
temperature while the blackbody cone is controlled at temperatures below (12
C), above (18 C), and equal to the detector temperature. The range of detector
temperatures is -15 C to 45 C (set points at 10 C increments). Data are
collected at each detector temperature set point, after detectors and target
reach constant temperatures.
All Apogee SDI-12 infrared radiometer models (SI-400 series) have sensor-
specific calibration coefficients determined during the custom calibration
process. Coefficients are programmed into the microcontroller at the factory.
Calibration data for each sensor are provided on a calibration certificate
(example shown on following page).
Calibration overview data are listed in box in upper left-hand corner, temperature errors are shown in graph, and calibration date is listed below descriptions of calibration procedure and traceability.
SDI-12 Interface
The following is a brief explanation of the serial digital interface SDI-12
protocol instructions used in Apogee SI-400 series infrared radiometers. For
questions on the implementation of this protocol, please refer to the official
version of the SDI-12 protocol: http://www.sdi-2.org/specification.php
(version 1.4, August 10, 2016).
Overview
During normal communication, the data recorder sends a packet of data to the
sensor that consists of an address and a command. Then, the sensor sends a
response. In the following descriptions, SDI-12 commands and responses are
enclosed in quotes. The SDI-12 address and the command/response terminators
are defined as follows:
Sensors come from the factory with the address of “0” for use in single sensor
systems. Addresses “1 to 9” and “A to Z”, or “a to z”, can be used for
additional sensors connected to the same SDI-12 bus.
“!” is the last character of a command instruction. In order to be compliant
with SDI-12 protocol, all commands must be terminated with a “!”. SDI-12
language supports a variety of commands. Supported commands for the Apogee
Instruments SI-400 series infrared radiometers are listed in the following
table (“a” is the sensor address. The following ASCII Characters are valid
addresses: “0-9” or “A-Z”).
Supported Commands for Apogee Instruments SI-400 Series Infrared Radiometers
Instruction Name | Instruction Syntax | Description |
---|---|---|
Send Identification Command | al! | Send Identification Information |
Measurement Command | aM! | Tells the Sensor to take a Measurement |
Measurement Command w/ Check Character | aMCI | Tells the Sensor to take a |
Measurement and return it with a Check Character
Change Address Command| aAb!| Changes the Address of the Sensor from a to b
Concurrent Measurement Command| aC!| Used to take a measurement when more than
one sensor is used on the same data line
Concurrent Measurement Command w/ Check Character| aCC!| Used to take a
measurement when more than one sensor is used on the same data line. Data is
returned with a check character.
Address Query Command| ?!| Used when the address is unknown to have the sensor
identify its address
Get Data Command| aDO!| Retrieves the data from a sensor
Make Measurement Command: M!
The make measurement command signals a measurement sequence to be
performed. Data values generated in response to this command are stored in the
sensor’s buffer for subsequent collection using “D” commands. Data will be
retained in sensor storage until another “M”, “C”, or “V” command is executed.
M commands are shown in the following examples:
Command | Response | Response to 0D0! |
---|---|---|
aM! or aM0! | a0011 |
Target temperature |
aM1! | a0012 |
Target temperature and sensor body temperature |
aM2! | a0012 |
Target millivolts and sensor body temperature |
aMC! or aMC0! | a0011 |
Target temperature w/ CRC |
aMC1! | a0012 |
Target temperature and sensor body temperature w/ CRC |
aMC2! | a0012 |
Target millivolts and sensor body temperature w/CRC |
where a is the sensor address (“0-9”, “A-Z”, “a-z”) and M is an upper-case
ASCII character.
The target temperature and sensor body temperature are separated by the sign
“+” or “-“, as in the following example (0 is the address):
Command | Sensor Response | Sensor Response when data is ready |
---|---|---|
0M! | 00011 |
0 |
0D0! | 0+23.4563 |
|
0M1! | 00012 |
0 |
0D0! | 0+23.4563+35.1236 |
|
0M2! | 00012 |
0 |
0D0! | 0+1.0+35.1236 |
where 23.4563 is target temperature, 1.0 is target millivolts, and 35.1236 is detector (sensor body) temperature.
Concurrent Measurement Command: aC!
A concurrent measurement is one which occurs while other SDI-12 sensors on the
bus are also making measurements. This command is similar to the “aM!”
command, however, the nn field has an extra digit and the sensor does not
issue a service request when it has completed the measurement. Communicating
with other sensors will NOT abort a concurrent measurement. Data values
generated in response to this command are stored in the sensor’s buffer for
subsequent collection using “D” commands. The data will be retained in the
sensor until another “M”, “C”, or “V” command is executed:
Command | Response | Response to 0D0! |
---|---|---|
aC! | a00101 |
Target temperature |
aC1! | a00102 |
Target temperature and sensor body temperature |
aC2! | a00102 |
Target millivolts and sensor body temperature |
aCC! | a00101 |
Target temperature w/ CRC |
aCC1! | a00102 |
Target temperature and sensor body temperature w/ CRC |
aCC2! | a00102 |
Target millivolts and sensor body temperature w/CRC |
where a is the sensor address (“0-9”, “A-Z”, “a-z”, “*”, “?”) and C is an
upper-case ASCII character.
For example (0 is the address):
Command | Sensor Response |
---|---|
0C! | 000101 |
0D0! | 0+23.4563 |
0C1! | 000102 |
0D0! | 0+23.4563+35.1236 |
0C2! | 000102 |
0D0! | 0+1.0+35.1236 |
where 23.4563 is target temperature, 1.0 is target millivolts, and 35.1236 is detector (sensor body) temperature.
Change Sensor Address: aAb!
The change sensor address command allows the sensor address to be changed. If
multiple SDI-12 devices are on the same bus, each device will require a unique
SDI-12 address. For example, two SDI-12 sensors with the factory address of 0
requires changing the address on one of the sensors to a non-zero value in
order for both sensors to communicate properly on the same channel:
Command | Response | Description |
---|---|---|
aAb! | b |
Change the address of the sensor |
where a is the current (old) sensor address (“0-9”, “A-Z”), A is an upper-case
ASCII character denoting the instruction for changing the address, b is the
new sensor address to be programmed (“0-9”, “A-Z”), and ! is the standard
character to execute the command. If the address change is successful, the
datalogger will respond with the new address and a
Send Identification Command: aI!
The send identification command responds with sensor vendor, model, and
version data. Any measurement data in the sensor’s buffer is not disturbed:
Command | Response | Description |
---|---|---|
aI! | a13Apogee SI-4mmvvvxx…xx |
The sensor serial number and other |
identifying values are returned
where a is the sensor address (“0-9”, “A-Z”, “a-z”, “*”, “?”), mm is a the sensor model number (11, 21, 31, or H1), vvv is a three character field specifying the sensor version number, and xx…xx is serial number.
Metadata Commands
Identify Measurement Commands
The Identify Measurement Commands can be used to view the command response
without making a measurement. The command response indicates the time it takes
to make the measurement and the number of data values that it returns. It
works with the Verification Command (aV!), Measurement Commands (aM!, aM1! …
aM9!, aMC!, aMC1! … aMC9!), and Concurrent Measurement Commands (aC!, aC1! …
aC9! , aCC!, aCC1! … aCC9!). The format of the Identify Measurement Command is
the address, the capital letter I, the measurement command, and the command
terminator (“!”), as follows:
The format of the response is the same as if the sensor is making a
measurement. For the Verification Command and Measurement Commands, the
response is atttn
3IMC2!| The Identify Measurement Command for sensor address 3, M2 command,
requesting a CRC.
---|---
30032
and two data values will be returned.
Identify Measurement Parameter Commands
The Measurement Parameter Commands can be used to retrieve information about
each data value that a command returns. The first value returned is a Standard
Hydrometeorological Exchange Format (SHEF) code. SHEF codes are published by
the National Oceanic and Atmospheric Administration (NOAA). The SHEF code
manual can be found at http://www.nws.noaa.gov/oh/hrl/shef/indexshef.htm.
The second value is the units of the parameter. Additional fields with more
information are optional.
The Measurement Parameter Commands work with the Verification Command (aV!),
Measurement Commands (aM!, aM1! … aM9!, aMC!, aMC1! … aMC9!), and Concurrent
Measurement Commands (aC!, aC1! … aC9! , aCC!, aCC1! … aCC9!).
The format of the Identify Measurement Parameter Command is the address, the
capital letter I, the measurement command, the underscore character (“_”), a
three-digit decimal number, and the command terminator (“!”). The three-digit
decimal indicates which number of measurement that the command returns,
starting with “001” and continuing to “002” and so on, up to the number of
measurements that the command returns.
The format of the response is comma delimited and terminated with a semicolon.
The first value is the address. The second value is the SHEF code. The third
value is the units. Other optional values may appear, such as a description of
the data value. The response is terminated with a Carriage Return (
a,
Identify Measurement Parameter Command example:
1IC_001!| The Identify Measurement Parameter Command for sensor address 1, C
command, data value 1.
---|---
1,RW,Watts/meter squared, incoming solar radiation;
solar radiation.
Target Temperature Measurement
SI-400 series infrared radiometers have an SDI-12 output. The following
equations and the custom calibration coefficients described in this section
are programmed into the microcontroller. Target temperature is output directly
in digital format.
The detector output from SI series radiometers follows the fundamental physics
of the Stefan-Boltzmann Law, where radiation transfer is proportional to the
fourth power of absolute temperature. A modified form of the Stefan-Boltzmann
equation is used to calibrate sensors, and subsequently, calculate target
temperature:
where TT is target temperature [K], TD is detector temperature [K], SD is the
millivolt signal from the detector, m is slope, and b is intercept. The mV
signal from the detector is linearly proportional to the energy balance
between the target and detector, analogous to energy emission being linearly
proportional to the fourth power of temperature in the Stefan-Boltzmann Law.
During the calibration process, m and b are determined at each detector
temperature set point (10 C increments across a -15 C to 45 C range) by
plotting measurements of TT4 TD4 versus mV. The derived m and b coefficients
are then plotted as function of TD and second order polynomials are fitted to
the results to produce equations that determine m and b at any TD:
Where C2, C1, and C0 are the custom calibration coefficients listed on the
calibration certificate (shown above) that comes with each SI-100 series
radiometer (there are two sets of polynomial coefficients, one set for m and
one set for b). Note that TD is converted from Kelvin to Celsius (temperature
in C equals temperature in K minus 273.15) before m and b are plotted versus
TD.
To make measurements of target temperatures, Eq. (1) is rearranged to solve
for TT [C], measured values of SD and TD are input, and predicted values of m
and b are input:
Emissivity Correction
Appropriate correction for surface emissivity is required for accurate
surface temperature measurements. The simple (and commonly made) emissivity
correction, dividing measured temperature by surface emissivity, is incorrect
because it does not account for reflected infrared radiation.
The radiation detected by an infrared radiometer includes two components: 1.
radiation directly emitted by the target surface, and 2. reflected radiation
from the background. The second component is often neglected. The magnitude of
the two components in the total radiation detected by the radiometer is
estimated using the emissivity (ε) and reflectivity (1 – ε) of the target
surface:
where E Sensor is radiance [W m-2 sr-1] detected by the radiometer, E Target
is radiance [W m-2 sr-1] emitted by the target surface, E Background is
radiance [W m-2 sr-1] emitted by the background (when the target surface is
outdoors the background is generally the sky), and is the ratio of non-
blackbody radiation emission (actual radiation emission) to blackbody
radiation emission at the same temperature (theoretical maximum for radiation
emission). Unless the target surface is a blackbody ( = 1; emits and absorbs
the theoretical maximum amount of energy based on temperature), E sensor will
include a fraction (1– ε ) of reflected radiation from the background.
Since temperature, rather than energy, is the desired quantity, Eq. (1) can be
written in terms of temperature using the Stefan-Boltzmann Law, E = T4
(relates energy being emitted by an object to the fourth power of its absolute
temperature):
where T Sensor [K] is temperature measured by the infrared radiometer
(brightness temperature), T Target [K] is actual temperature of the target
surface, T Background [K] is brightness temperature of the background (usually
the sky), and is the Stefan-Boltzmann constant (5.67 x 10-8 W m-2 K-4). The
power of 4 on the temperatures in Eq. (2) is valid for the entire blackbody
spectrum.
Rearrangement of Eq. (2) to solve for T Target yields the equation used to
calculate the actual target surface temperature (i.e., measured brightness
temperature corrected for emissivity effects):
Equations (1)-(3) assume an infinite waveband for radiation emission and constant € at all wavelengths. These assumptions are not valid because infrared radiometers do not have infinite wavebands, as most correspond to the atmospheric window of 8-14 um, and € varies with wavelength. Despite the violated assumptions, the errors for emissivity correction with Eq. (3) in environmental applications are typically negligible because a large proportion of the radiation emitted by terrestrial objects is in the 8-14 um waveband (the power of 4 in Eqs. (2) and (3) is a reasonable approximation), for most terrestrial objects does not vary significantly in the 8-14 um waveband, and the background radiation is a small fraction (1 — ε) of the measured radiation because most terrestrial surfaces have high emissivity (often between 0.9 and 1.0). To apply Eq. (3), the brightness temperature of the background (Tgackgrouna) Must be measured or estimated with reasonable accuracy. If a radiometer is used to measure background temperature, the waveband it measures should be the same as the radiometer used to measure surface brightness temperature. Although the ¢ of a fully closed plant canopy can be 0.98-0.99, the lower € of soils and other surfaces can result in substantial errors if ¢ effects are not accounted for.
MAINTENANCE AND RECALIBRATION
Blocking of the optical path between the target and detector, often due to moisture or debris on the filter, is a common cause of inaccurate measurements. The filter in SI series radiometers is inset in an aperture, but can become partially blocked in four ways:
- Dew or frost formation on the filter.
- Salt deposit accumulation on the filter, due to evaporating irrigation water or sea spray. This leaves a thin white film on the filter surface. Salt deposits can be removed with a dilute acid (e.g., vinegar). Salt deposits cannot be removed with solvents such as alcohol or acetone.
- Dust and dirt deposition in the aperture and on the filter (usually a larger problem in windy environments). Dust and dirt are best removed with deionized water, rubbing alcohol, or in extreme cases, acetone.
- Spiders/insects and/or nests in the aperture leading to the filter. If spiders/insects are a problem, repellent should be applied around the aperture entrance (not on the filter).
Clean inner threads of the aperture and the filter with a cotton swab dipped
in the appropriate solvent. Never use an abrasive material on the filter. Use
only gentle pressure when cleaning the filter with a cotton swab, to avoid
scratching the outer surface. The solvent should be allowed to do the
cleaning, not mechanical force.
It is recommended that infrared radiometers be recalibrated every two years.
See the Apogee webpage for details regarding return of sensors for
recalibration (http://www.apogeeinstruments.com/tech-support-
recalibrationrepairs/).
TROUBLESHOOTING AND CUSTOMER SUPPORT
Independent Verification of Functionality
The simplest way to check sensor functionality is the aM2! command. This
command returns detector temperature and detector voltage output. Detector
temperature should read very near room temperature. When the aperature of the
sensor is covered with aluminum foil, the voltage output should read very near
0 mV.
If the sensor does not communicate with the datalogger, use an ammeter to
check the current drain. It should be near 0.6 mA when the sensor is not
communicating and spike to approximately 1.3 mA when the sensor is
communicating. Any current drain greater than approximately 6 mA indicates a
problem with power supply to the sensors, wiring of the sensor, or sensor
electronics.
Compatible Measurement Devices (Dataloggers/Controllers/Meters)
Any datalogger or meter with SDI-12 functionality that includes the M or C
command.
An example datalogger program for Campbell Scientific dataloggers can be found
on the Apogee webpage at http://www.apogeeinstruments.com/content/Infrared-
Radiometer-Digital.CR1.
Modifying Cable Length
SDI-12 protocol limits cable length to 60 meters. For multiple sensors
connected to the same data line, the maximum is 600 meters of total cable
(e.g., ten sensors with 60 meters of cable per sensor). See Apogee webpage for
details on how to extend sensor cable length
(http://www.apogeeinstruments.com/how-to-make-aweatherproof-cable-splice/).
Signal Interference
In instances where SI-400 series radiometers are being used in close proximity
to communications (near an antenna or antenna wiring), it may be necessary to
alternate the data recording and data transmitting functions (i.e.,
measurements should not be made when data are being transmitted wirelessly).
If EMI is suspected, place a tinfoil cap over the front of the sensor and
monitor the signal voltage from the detector. The signal voltage should remain
stable at (or very near) zero.
APOGEE INSTRUMENTS, INC, | 721 WEST 1800 NORTH, LOGAN, UTAH 84321, USA
TEL: 435-792-4700 | FAX:
435-787-8268 | WEB:
APOGEEINSTRUMENTS.COM
Copyright ©2018 Apogee instruments, Inc.
References
- apogeeinstruments.com/content/Infrared-Radiometer-Digital.CR1
- How to Make a Weatherproof Cable Splice
- Recalibration and Repair | Apogee Instruments
- Office of Water Prediction
- SDI-12 Specification
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