Rhoe A. Thompson

Array nonuniformity correction: new procedures designed for difficult measurement conditions

For many types of infrared scene projectors, differences in the outputs of individual elements are one source of error in projecting a desired radiance scene. This is particularly true of resistor-array based infrared projectors. Depending on the sensor and application, the desired response uniformity may prove difficult to achieve. The properties of the sensor used to measure the projector outputs critically affect the procedures that can be used for nonuniformity correction (NUC) of the projector, as well as the final accuracy achievable by the NUC. In this paper we present a description of recent efforts to perform NUC of an infrared projector under “adverse” circumstances. For example, the NUC sensor may have some undesirable properties, including: significant random noise, large residual response nonuniformity, temporal drift in bias or gain response, vibration, and bad pixels. We present a procedure for reliably determining the output versus input response of each individual emitter of a resistor array projector. This NUC procedure has been demonstrated in several projection systems at the Kinetic Kill Vehicle Hardware-In-the-Loop Simulator (KHILS) including those within the KHILS cryogenic chamber. The NUC procedure has proven to be generally robust to various sensor artifacts.

Radiometrically calibrating spectrally coupled two-color projectors

Infrared projection systems based on resistor arrays typically produce radiometric outputs with wavelengths that range from less than 3 microns to more than 12 microns. This makes it possible to test infrared sensors with spectral responsivity anywhere in this range. Two resistor-array projectors optically folded together can stimulate the two bands of a 2-color sensor. If the wavebands of the sensor are separated well enough, it is possible to fold the projected images together with a dichroic beam combiner (perhaps also using spectral filters in front of each resistor array) so that each resistor array independently stimulates one band of the sensor. If the wavebands are independently stimulated, it is simple to perform radiometric calibrations of both projector wavebands. In some sensors, the wavebands are strongly overlapping, and driving one of the resistor arrays stimulates both bands of the unit-under-test (UUT). This “coupling” of the two bands causes errors in the radiance levels measured by the sensor, if the projector bands are calibrated one at a time. If the coupling between the bands is known, it is possible to preprocess the driving images to effectively decouple the bands. This requires performing transformations, which read both driving images (one in each of the two bands) and judiciously adjusting both projectors to give the desired radiance in both bands. With this transformation included, the projection system acts as if the bands were decoupled - varying one input radiance at a time only produces a change in the corresponding band of the sensor. This paper describes techniques that have been developed to perform radiometric calibrations of spectrally coupled, 2-color projector/sensor systems. Also presented in the paper are results of tests performed to demonstrate the performance of the calibration techniques. Possible hardware and algorithms for performing the transformation in real-time are also presented.

Procedures and recent results for two-color infrared projection

Testing of two-color imaging sensors often requires precise spatial alignment, including correction of distortion in the optical paths, beyond what can be achieved mechanically. Testing, in many cases, also demands careful radiometric calibration, which may be complicated by overlap in the spectral responses of the two sensor bands. In this paper, we describe calibration procedures used at the Air Force Research Laboratory hardware-in-the-loop (HWIL) facility at Eglin AFB, and present some results of recent two-color testing in a cryo-vacuum test chamber.

Advances in cryo-vacuum test capabilities for dual-band sensors at the kinetic kill vehicle hardware-in-the-loop simulation (KHILS) facility

The KHILS Vacuum Cold Chamber (KVACC) has formed the basis for a comprehensive test capability for newly developed dual-band infrared sensors. Since initial delivery in 1995, the KVACC chamber and its support systems have undergone a number of upgrades, maturing into a valuable test asset and technology demonstrator for missile defense systems. Many leading edge test technologies have been consolidated during the past several years, demonstrating the level of fidelity achievable in tomorrows missile test facilities. These technologies include resistive array scene projectors, sub-pixel non-linear spatial calibration and coupled two-dimensional radiometric calibration techniques, re-configurable FPGA based calibration electronics, dual-band beam-combination and collimation optics, a closed-cycle multi-chamber cryo-vacuum environment, personal computer (PC) based scene generation systems and a surrounding class-1000 clean room environment. The purpose of this paper is to describe this unique combination of technologies and the capability it represents to the hardware-in-the-loop community.

Process-based real-time scene data processor design for emitter array infrared projectors

An alternative class of infrared projector real-time nonuniformity correction processor is introduced, based on the concept that the fundamental role of the processor is to reverse each of the projector processing steps as the input DAC voltage word is converted into infrared signal radiance output. The design is developed by assessment of the sequence of processes occurring within the projector and is tested by simulation. It is shown that there is potential for high fidelity nonuniformity correction across the infrared dynamic range without the need for the introduction of curve-fitting breakpoints.

Developments at the kinetic-kill Vehicle hardware-in-the-loop Simulator (KHILS) facility

The Ballistic Missile Defense Organization (BMDO) sponsored the development of the Kinetic Kill Vehicle Hardware-in-the- Loop Simulator (KHILS) to provide a comprehensive ground test capability for end game performance evaluation of BMDO interceptor concepts. Since its inception in 1986, the KHILS facility has been on the forefront of HWIL test technology development. This development has culminated in closed-loop testing involving large format resistive element projection arrays, 3D scene rendering systems, and real-time high fidelity phenomenology codes. Each of these components has been integrated into a real-time environment that allows KHILS to perform dynamic closed-loop testing of BMDO interceptor systems or subsystems. Ongoing activities include the integration of multiple resistor arrays into both a cold chamber and flight motion simulator environment, increasing the update speed of existing arrays to 180 Hz, development of newer 200 Hz snapshot resistor arrays, design of next generation 1024 X 1024 resistor arrays, development of a 1000 Hz seeker motion stage, integration of a resistor array into an RF chamber, and development of advanced real-time plume flow-field codes. This paper describes these activities and test results of the major facility components.

Prediction methodologies for target scene generation in the Aerothermal Targets Analysis Program (ATAP)

The Air Force Research Laboratory (AFRL) Aerothermal Targets Analysis Program (ATAP) is a user-friendly, engineering-level computational tool that features integrated aerodynamics, six-degree-of-freedom (6-DoF) trajectory/motion, convective and radiative heat transfer, and thermal/material response to provide an optimal blend of accuracy and speed for design and analysis applications. ATAP is sponsored by the Kinetic Kill Vehicle Hardware-in-the-Loop Simulator (KHILS) facility at Eglin AFB, where it is used with the CHAMP (Composite Hardbody and Missile Plume) technique for rapid infrared (IR) signature and imagery predictions. ATAP capabilities include an integrated 1-D conduction model for up to 5 in-depth material layers (with options for gaps/voids with radiative heat transfer), fin modeling, several surface ablation modeling options, a materials library with over 250 materials, options for user-defined materials, selectable/definable atmosphere and earth models, multiple trajectory options, and an array of aerodynamic prediction methods. All major code modeling features have been validated with ground-test data from wind tunnels, shock tubes, and ballistics ranges, and flight-test data for both U.S. and foreign strategic and theater systems. Numerous applications include the design and analysis of interceptors, booster and shroud configurations, window environments, tactical missiles, and reentry vehicles.

Numerical quantization effects in KHILS projection systems

The Honeywell resistor arrays produce radiance outputs, which are observed to have a strong non-linear dependence on the voltage out of the digital-to-analog-converters (DACs). In order for the projection system to run in a radiometrically calibrated mode, the radiances in the image generator must be transformed with exactly the inverse of the resistor array response function before they are sent to the DACs. Representing the image values out of the image generator and the values into the DACs with quantized, digital values introduces errors in the radiance out of the resistor array. Given the functional form of the emitter array response and the number of bits used to represent the image values, these errors in the radiometric output due to the quantization effects can be calculated. This paper describes the calculations and presents results for WISP, MSSP, and the new extended range and standard range BRITE II arrays.

Correction of spatial distortions in a two-color infrared projection system

As discussed in a previous paper to this forum, optical components such as collimators that are part of many infrared projection systems can lead to significant distortions in the sensed position of projected objects versus their true position. The previous paper discussed the removal of these distortions in a single waveband through a polynomial correction process. This correction was applied during post-processing of the data from the infrared camera-under-test. This paper extends the correction technique to two-color infrared projection. The extension of the technique allows the distortions in the individual bands to be corrected, as well as providing for alignment of the two color channels at the aperture of the camera-under-test. The co-alignment of the two color channels is obtained through the application of the distortion removal function to the object position data prior to object projection.

Optimization of resistor array infrared projector temporal response

The thermal conduction and electronic drive processes that govern the temporal response of resistor array infrared projectors are reviewed. The characteristics and limitations of the voltage overdrive method that can be implemented for sharpening the temporal response are also discussed. Overdrive is shown to be a viable technique provided sufficient drive power and temperature margins are available outside of the normal dynamic range. It is shown also by analysis of overdrive measurements applied to a Honeywell GE snapshot resistor array that practical real-time overdrive processors can be designed to operate consistently with theoretical predictions.