D501 and D501-RS. Microscanner D-Series IR Thermometers. no effect. no effect. no effect. no effect no effect

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Microscanner D-Series The Only Certified Accurate Surface Instruments in the World A MUST FOR ISO 9001 ISO 9002 ISO 9003 TRACEABILITY PROGRAMS Common Surface Measurement Errors D501 and D501-RS Microscanner D-Series IR Thermometers Conventional IR Point and Shoot guns and probes, including laser aimed units Conventional contact probes, thermocouples, RTDs, thermistors 1 Pre-set Emissivity errors? 2 Emissivity shift errors? 3 User adjustment errors? 4 Background reflection errors? 5 Contact errors? 6 Friction heating errors? 7 Heat sinking errors? 8 Time based errors? 51 Water Street, Watertown, MA 02172 USA 800-422-3006 617-923-9900 Fax 617-923-9911

The D-Series is an entirely different type of instrument than conventional temperature measuring devices. Designed specifically for the highest possible accuracy, it is the only infrared instrument which can be certified as to NIST-tracable accuracy on real surfaces of unknown emissivity, while completely free of contact errors and heat sinking errors of contact devices. Recessed cone traps all emitted surface radiation, and blocks out any radiation from environment. Actual measurement area is in the center, well away from the area contacted by the edge of the cone. Only a thin lip of material actually contacts the target, thus minimizing heat transfer. Reflective cone automatically corrects for emissivity variations by creating an actual blackbody at the precise location of measurement. Figure 1. Unique Automatic Emissivity Compensation System (AECS) produces accurate temperatures everywhere the infrared probe is placed, by creating its own blackbody. Effect of Emissivity on Reading for a 500 F (260 C) Target in 70 F (21 C) ambient 1. Emissivity errors The true emissivity of a surface is known only approximately. Conventional IR devices without Exergen s Automatic Emissivity Compensation System can only display an approximate temperature over their entire temperature range. The accuracy specifications given by most manufacturers are only for a black body calibration and do not hold outside laboratory conditions. Black body calibrations do not include emissivity shifts, ambient change effects on the target, and other phenomena that introduce significant errors. 550 500 450 deg F 400 350 300 1 0.8 0.6 Non-metals and Oxides 0.4 Emissivity D-Series using marker D-Series w/o marker Conventional Infrared 290 deg C 200 150 0.2 0 Clean Metals Figure 2. D-Series is accurate over a wide emissivity range, sufficient to include all non-metals. If a marker (or any other non-metal coating) is used, the D-series is accurate on clean metals as well. Conventional IR devices have considerable inaccuracy. 2. Emissivity shift errors Even if an IR gun is set to the correct emissivity to read a surface accurately at a particular temperature, it does not mean that the IR gun will read the same target correctly at other temperatures. Emissivity of virtually all surfaces changes with temperature. A common assumption for conventional IR thermometry is that emissivity is constant with changes in target surface temperature. Real materials do not have this characteristic. ε Conventional IR assumption Actual emissivity

3. User adjustment errors A setting of emissivity = 0.9 on an IR gun from one manufacturer will not necessarily match that of another IR gun from another manufacturer. There are no standards set in the industry on the precise measurement and meaning of emissivity. Also, Quality Assurance programs should not rely upon any instrument that allows users to alter the instrument settings and to let it display whatever the user wishes. 4. Background reflection errors Even if emissivity is constant (see #2), there are still errors induced by changing ambient temperatures. For example, with emissivity = 0.9, ambient reflections account for 10% of the signal that the IR gun will see. If ambient changes, the IR gun will display a different target temperature, even if the target remains at the same temperature. Effect of Ambient on Target Reading for 100 F (38 C) Target with.8 Emissivity Target T (F) 4 16 27 38 110 Conventional Infrared 106 102 98 94 D-Series 90 0 20 40 60 80 100 32 120 Ambient T (F) Figure 3. D-Series remains accurate even if the ambient temperature varies, while conventional IR devices have considerable inaccuracies. (C) 43 38 5. Contact errors Thermocouples, RTDs, thermistors and other contact devices only measure their own temperature. They do not measure surface temperature. Published Accuracy specifications are for the probes only, not the surfaces they must measure. Users must guarantee that the probes are brought to the same temperature as the surface. Can you guarantee that your probes are brought to the same temperature as the targets to be measured? 6. Friction heating errors For moving surfaces, a contact probe is prone to frictional heating. The size of the error is dependent on the roughness of the surface, the speed, the coating on the probe, and so on. It is impossible to control all the variables. 7. Heat sinking errors 500 400 300 deg F 200 100 Time Comparison Between D-Series and Contact Thermocouple for Measuring a 500 F (260 C) Surface D-Series Contact Probes Contact Error 260 200 0 0.001 0.01 0.1 1 10 100 1000 Time from start of Measurement (sec) Figure 4. D-Series measures surface temperature in a fraction of a second, while contact probes (thermocouples, RTD s, thermistors, etc.) require many minutes to acheive equilibrium. Contact probes always have a residual error due to imperfect heat transfer from the surface to probe. 150 90 deg C For most non-metals, heat sinking errors can be quite large. The heat transfer rate of the metal leads required on contact probes conducts heat faster than the target material can replace, resulting in unknown and fairly large errors. In general, the less dense the target material, the larger the heat sinking error with a contact probe. 8. Time based errors Contact temperature probes are slow. The temperature of a target can change more quickly than most probes, resulting in errors in real time measurement.

Psychrometrics, the science of measurement and control of moisture in air, is based entirely on thermodynamics of air and water: the properties and temperature. Relative humidity (RH) is one of the common parameters used to describe the psychrometric state of air in an environment, in an oven, or any area where moisture content can influence product quality or personnel comfort. The accurate and reliable measurement of RH is one of the most challenging tasks in industry, and has included devices such as chilled mirrors, lithium chloride cells, aluminum oxide sensors, capacitance polymer sensors, hair hygrometers, carbon hygristors, and a wide variety of technologies to meet the requirements. Calibration and certification has been even more difficult, due to the fact that most humidity measuring devices employ indirect methods and therefore have limited traceability. Infrared Psychrometry with the Microscanner D-Series: Measure Relative Humidity to Certified Accuracy ±0.5% RH Air Flow Thin layer of evaporating water at thermodynamic equilibrium: wet-bulb temperature Wet Porous Material A MUST FOR ISO 9001 ISO 9002 ISO 9003 TRACEABILITY PROGRAMS The Infrared Psychrometry method with the D- Series is a direct application of the thermodynamics and mathematics that defines humidity: the D-Series is capable of measuring the true wet-bulb temperature accurately, and with the dry-bulb temperature, the RH can be computed to a very high accuracy via standard psychrometric equations. The process is as follows: A porous material (filter paper is suitable) is wetted with water (purity is not important), and air from the environment flows across the surface to bring the surface to thermodynamic equilibrium with the air, i.e. to the lowest possible temperature produced by the evaporating water, which is the wet-bulb temperature.

The porous material, cooled on both sides by evaporating water, reaches wet-bulb temperature throughout the material, thus maintaining wet-bulb temperature at the surface for several seconds after the air flow stops. Since the water is opaque to infrared wavelengths, in as thin a layer as.002 in. (.05 mm), and the D-Series is able to measure the temperature with a time constant of 0.1 seconds, an accurate measurement of the wet-bulb temperature is obtained. The same procedure is employed on a non-porous material to obtain an accurate dry-bulb temperature. With the appropriate psychrometric equations, the RH is immediately calculated. Each D-Series is equipped with, as a standard accessory, an RH Kit, which includes a convenient card with the wet and dry materials, simple RH and Dewpoint calculator, and handy tube of water. Maximum accuracy for RH measurement is obtained with the D-Series models measuring 0.1 resolution. Though the absolute accuracy of the D-Series is not 0.1, the RH is most sensitive to wet-bulb depression, i.e. the difference between dry-bulb and wet-bulb temperature. In its differential mode, the D-Series is accurate to 0.1, which translates to an RH accuracy of approximately 0.5% for the normal range of RH. Also Manufactured by Exergen Industrial Division IR detector D-Series nosepiece surface at wet-bulb temperature in the field-of-view of detector IRt/c Infrared Thermocouples Low-cost, high-quality sensors for non-contact temperature measurement and control. IRt/c sensors are used by more customers worldwide for process control, factory automation and OEM applications than any other IR device in the world. The small, easy to use IRt/c sensors require no power and connect directly to standard thermocouple devices available worldwide. Over 300 models offered, covering temperature ranges from -50 to 5000F (-45 to 2760C) with up to 0.01C precision. For more information and pricing, please request a free copy of The IRt/c Book catalog from your local distributor, or Exergen. Microscanner E-Series Distributed by: Microscanner E-Series and IR.1Probe for Electrical Inspection These unique handheld instruments are used by professionals for fast, accurate scanning of electrical equipment. The Microscanner Super E with a 200:1 lens, color-coded display and optional pointing laser is the fastest and most powerful pocket-sized electrical IR scanner in the world. The IR.1Probe is a low cost electrical IR scanner for use with standard digital multimeters. Contact Exergen or your local distributor for more information. PN818103 REV.3

Specifications Model D501 D1001 D1201 D1601 Range Relative Humidity Measurement Emissivity Adjustment Calibration Requirement Linearity Error Emissivity Error Repeatability Resolution -50 to 550F 0-1000F 186-1207F 186-1600F & -45 to 287C & -18 to 540C & 86 to 653C & 86 to 871C Kit Included Kit Included No No Automatic Emissivity Compensation System None +/-1% of Reading - maximum +/-3% maximum +/-1% maximum of Difference between target temperature and instrument temperature when touching, for emissivity of 0.8 to 1.0 o +/-0.1 F & +/-0.1 o C 0.1 o F & 0.1 o C Microscanner D501& D501RS D501 Display / Update Bright LEDs at 10 times per second Response Time 80 msec approximately Field of View Minimum Spot Size Spectral Sensitivity 1:1 (53 o approximately) 1/4 inch (6.4 mm) approximately 2 to 20 microns D1001 Analog Output* 1 Mv / OF (1mV/ o C) Optional o o F/ C Conversion Yes Yes Yes Yes Remote Sensor** Instrument Operating Battery Life Available on all models; standard on D1201 and 1601 32 to 122 o F (0 to 50 o C) Approximately 5000 Readings from on 9V Alkaline Battery D1201 Dimensions Main Case: 3 3/8 X 5 X 3/4 (8.5 X 12.5 X 2cm) Weight (Remote Sensor Version) 7 oz (.2 kg) approx. 9 oz (.25 kg) approx. *Optional Analog Output - Specify AO example: Microscanner D501-AO **Remote Sensor - Specify Model RS example: Microscanner D501-RS D1601 Consult factory or distributor for special duty models with special accuracies and temperature ranges for OEM and volume applications.