High Accuracy CMM Measurements at NIST by John Stoup National Institute of Standards and Technology, USA 2007 CMM Users Meeting - Mexico October 22, 2007 Today‟s Discussion We will describe the equipment and processes used at NIST for making world class CMM Measurements. • Describe what is needed to make the best possible measurements. • Outline some techniques used to assess the CMM environment‟s thermal performance. • Discuss optimizing probe performance. • Present machine performance using gauge data. • Uncertainty calculations. • Special measurement setup designs. Repeatability vs. Time 1.050 1.000 0.950 High Quality Industrial CMM in Good Lab 1000 millimeter dimension repeatability data 0.900 0.800 Cost of improvement increases substantially as you attempt to drop these lines closer together 0.750 0.700 0.650 0.600 0.500 0.450 0.400 0.350 0.300 Thermal issues dominate $ $ $$ $$$$ $$$$$$$$ 0.550 Short term repeatability Standard Deviation (micrometers) 0.850 $ $ $$ $$$$ $$$$$$$$ 0.250 0.200 0.150 0.100 0.050 0.000 5 minutes 5 days 5 years 25 millimeter dimension repeatability data Mostly machine related issues Probe limited performance Repeatability vs. Time 0.850 0.800 0.750 High quality CMM in very good laboratory Standard Deviation (micrometers) 0.700 0.650 0.600 0.550 0.500 0.450 NIST PMM in very good lab 19.9˚ - 20.1˚C operating range 0.400 0.350 0.300 0.250 0.200 NIST Moore M48 CMM 0.150 0.100 Probe limited performance 0.050 0.000 5 minutes 5 days 5 years What do we need to make very high accuracy CMM Measurements? • Extreme high quality lab space. - gradient control most important. • CMM capable of exceptional positioning repeatability. - error mapping will take care of the rest. • Probe with exceptional gauging repeatability. • Data collection techniques. - redundancy. - test for stability during long data collection runs. • Operators that strive for the highest accuracy result. The NIST Advanced Measurement Laboratory • Large laboratory spaces. • Airflow at the rate of 300 air changes/hour in CMM space. • 20.00 ºC 0.01 ºC temperature stability. • Improved power quality and mechanical reliability. NIST M48 CMM in AML laboratory • Reflected room lights. • Thermally controlled floor. • Vibration isolation. • Laser scales. • All heating sources outside of room. • Granite table added. • 4 mm/s top speed! M48 Motion Mechanisms • Roller bearing twin V-ways. • Lead screw driven. • All operation in oil baths. Average Temperature (°C ) AML Thermal Performance – short term 20.01 20.008 20.006 20.004 20.002 20 19.998 19.996 19.994 19.992 19.99 19.988 19.986 19.984 19.982 19.98 0 2 4 6 8 10 12 14 16 18 20 22 24 26 28 30 32 34 36 38 40 42 44 46 48 Hours AML Thermal Performance – long term 20.015 Average Temperature ( °C) 20.010 20.005 20.000 19.995 19.990 19.985 19.980 19.975 19.970 19.965 19.960 792 768 744 720 696 672 648 624 600 576 552 528 504 480 456 432 408 384 360 336 312 288 264 240 216 192 168 144 120 96 72 48 24 0 Hours Thermal Gradient Testing • We need to find out if the moving parts of the CMM maintain a constant temperature during operation. • We need the temperature in the measuring volume of the machine to be stable during operation. Therefore, we must • „Tune‟ the room to optimize these two requirements. • Both axes – carriage and table motions. Temperature sensor locations on M48 carriage Right Side Metal Sensor #5 & #6 Air sensor #1 Left Side Air sensor #2 Metal Sensor #7 & #8 Air sensor #3 Air sensor #4 Metal Sensor #9 & #10 Metal Sensor #11 & #12 RAM Camera Thermistor difference data Thermistor data - side to side differences 0.08 0.06 0.04 Temperature Scale (deg C) 0.02 0 A3-A4 A1-A2 M5-M6 M7-M8 M9-M10 M11-M12 -0.02 -0.04 -0.06 -0.08 -0.1 -0.12 -0.14 Time Tuning the Room Thermistor data - side to side differences after airflow adjustments 0.03 0.02 0.01 0 Temperature scale ( °C ) • Remove gradients from around machine by removing some ceiling tiles. • Increased turbulent airflow with better air mixing around the machine. • Differences reduced by ~80% -0.01 -0.02 -0.03 -0.04 -0.05 -0.06 A3-A4 A1-A2 M5-M6 M11-M12 M7-M8 M9-M10 -0.07 -0.08 -0.09 -0.1 Time Error Mapping Effort 0 Error (tenth microradians) • Error mapping the M48 takes about 2 months. • Performed redundantly over time to watch warmup behavior. • External laser used to measure all rotational errors directly. • Full 21 component map at 25mm intervals. Y Axis Roll Map, Ryy exisiting map -5 no warmup -10 1 hr warmup -15 2 hr warmup -20 3 hr warmup -25 -30 -35 -40 -45 -50 0 50 100 150 200 250 300 350 400 450 500 Table position (mm) 550 600 650 700 750 800 850 CMM Probing – repeatability is key • NIST uses a currently unavailable probe design. • Stylus geometries mapped for optimum correction. • Stem lengths kept as short as possible. • Probe trigger design is important for dirt detection. Do what it takes to get probe repeatability! • Room airflow creates vibrations in the probe. • A cover is required for highly repeatable results. • X axis repeatability ~ 9 nm. • Y axis repeatability ~ 13 nm. • Z axis repeatability ~ 7 nm. Average Puck Repeatability – 1m Step Gage Average Repeatability Standard Deviation - Step Gage Measurements 0.000040 Move to AML July 2004 0.000036 Standard Deviation (mm) 0.000032 In Old Laboratory Environment In AML 0.000028 0.000024 0.000020 0.000016 0.000012 0.000008 0.000004 0.000000 10/01 2/02 10/06 6/02 7/02 2/03 5/03 11/03 1/04 6/04 12/04 5/05 12/05 4/06 9/06 9/06 Step Gage Data – AML Comparison Long Term Repeatability - Step Gage Data all combined history vs. AML data 0.000120 AML Puck Side A 0.000110 AML Puck Side B 0.000100 History Puck Side A History Puck Side B 0.000090 Prior History Average Linear Fit 0.000080 0.000070 0.000060 0.000050 0.000040 0.000030 0.000020 0.000010 Position (mm) 96 0 10 00 10 40 92 0 88 0 84 0 80 0 76 0 72 0 68 0 64 0 60 0 56 0 52 0 48 0 44 0 40 0 36 0 32 0 28 0 24 0 20 0 16 0 12 0 80 40 0.000000 0 Sigma (mm) AML Average Linear Fit ~ 3 Day Length-Based Repeatability Comparison – NIST M48 CMM • Prior environment results: • AML current results: ulb = 0.035 + 0.022 L µm ulb = 0.019 + 0.015 L µm ** A 45% improvement in performance with a better room! This term is independent of error sources such as gage instability, inaccuracy of the CMM error map, fixturing effects, thermal gradient induced errors, and thermometer calibration. But it does include CMM positioning, probing effects, error map stability and thermal stability of the machine space. Table Setups Designed for Long Operation • Measurements of ring and large plug gauges. • Long gauge blocks, step gauges and end standards. • Grid plates and scales. • 30 % of artifacts we measure belong to NIST! M48 CMM Uncertainty Components Uncertainty Source • • • • • • • • • • • • Standard Deviations μm ppm Machine Positioning Uncertainty Temperature difference in beam paths during calibration Laser Frequency Difference Measurement Reproducibility (probe effects are here) Edlén Equation Index of Refraction – Air Temperature Index of Refraction - Air Pressure Index of Refraction – Humidity Artifact Temperature Measurement Accuracy (4mK) Coefficient of Thermal Expansion (1ppm/˚C)( 0.05˚C) Contact Deformation Gage Surface Geometry 0.04 0.04 0.002 0.004 0.01 0.02 0.04 0.03 0.01 0.04 0.03 0.05 0.05 NIST M48 CMM Typical Uncertainty Statements • For 1D measurements: Uc (k=2) = 0.11 + 0.2L µm (L is in meters) • For 2D measurements: Uc (k=2) = 0.13 + 0.2L µm (L is in meters) Special Setups and Arrangements: Silicon Spheres • Required for even lower uncertainties. • Designed to reduce or eliminate some uncertainty components. • Have achieved task specific expanded uncertainties (k = 2) of about 0.03 micrometers. Special Setups and Arrangements: Double Corner Cube • In one case, we created better than a class 1000 cleanroom environment around the machine. • Designed for a 3D feature measurement in a critical component of a NASA space interferometer to be launched in the near future. Other Special Arrangements Conclusions • The NIST M48 CMM has state of the art performance. • Everything is compromised or designed for the sake of accuracy and repeatability. • For the highest accuracy you must have all the required elements as discussed earlier. AND • We are always making incremental improvements in its performance. • Measurand definition becoming important due to surface imperfections of even the best of artifacts. • We may become “probe-limited” soon.
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