The rapid proliferation of solid-state lighting (SSL) technologies\u2014encompassing LEDs and OLEDs\u2014has necessitated a paradigm shift in optical measurement methodologies. Unlike conventional incandescent or fluorescent sources, LED emissions are characterized by narrow spectral bands, high luminous efficacy, and temperature-dependent chromaticity shifts. These unique attributes render traditional photometric benches and goniophotometers insufficient for capturing the full spectrum of performance parameters required by modern industrial standards. Consequently, innovative LED measurement systems integrating spectroradiometers with integrating spheres have emerged as the cornerstone of quality assurance, regulatory compliance, and research-driven development across diverse sectors such as automotive lighting, aerospace avionics, medical illumination, and photovoltaic characterization.<\/p>\n
This technical exposition delineates the operational principles, architectural design, and industrial applicability of advanced sph\u00e8re d'int\u00e9gration<\/a>\u2013spectroradiometer systems, with particular emphasis on the LISUN<\/a> LPCE-2 and LPCE-3 platforms. Through rigorous analysis of measurement uncertainties, spectral stray light correction, and temporal stability, this article establishes a framework for selecting and deploying these systems in high-stakes environments requiring traceable photometric and radiometric data.<\/p>\n The combination of an integrating sphere with a high-resolution spectroradiometer constitutes a closed-loop optical system designed to capture total luminous flux, colorimetric coordinates (CIE 1931 xy, CIE 1976 u\u2019v\u2019), correlated color temperature (CCT), color rendering indices (CRI R\u2090, R\u2089\u2013R\u2081\u2085), and spectral power distribution (SPD) with minimal angular dependence. The integrating sphere\u2019s interior, typically coated with barium sulfate or PTFE-based diffuse reflectance materials, ensures that light emitted from the device under test (DUT) undergoes multiple Lambertian reflections, resulting in a spatially uniform radiance at the sphere wall. This uniformity is critical for eliminating directional measurement errors inherent in LED sources with asymmetric beam patterns.<\/p>\n The spectroradiometer, employing a Czerny-Turner or concave holographic grating configuration, disperses the collected light onto a charge-coupled device (CCD) or complementary metal-oxide-semiconductor (CMOS) linear array sensor. The LPCE-2 and LPCE-3 instruments utilize a temperature-stabilized CCD array with a spectral resolution of 0.5 nm across the 350\u20131050 nm range, enabling detection of both visible and near-infrared spectral components. The integration time, controlled via software, can be adjusted dynamically to accommodate DUTs ranging from 0.1 lm to 200,000 lm, ensuring that neither saturation nor poor signal-to-noise ratio compromises data fidelity.<\/p>\n Calibration traceability is achieved through reference standards certified by national metrology institutes (e.g., NIST, PTB). The LPCE series employs a calibrated spectral irradiance standard lamp for wavelength accuracy verification and a luminous flux standard (typically a halogen lamp with known total flux) for absolute photometric calibration. The combined expanded uncertainty (k=2) for luminous flux measurements is typically within \u00b11.5% for white LEDs and \u00b12.0% for narrowband monochromatic sources, contingent upon proper thermal management and sphere surface maintenance.<\/p>\n The LISUN LPCE-2 (High Precision LED Photoelectric & Chromaticity Test System) and LPCE-3 (High Precision CCD Spectroradiometric & Integrating Sphere Measurement System) represent distinct tiers of measurement capability tailored to industrial throughput requirements. Table 1 summarizes the salient specifications differentiating these two systems.<\/p>\n Table 1: Comparative Specifications of LISUN LPCE-2 and LPCE-3 Systems<\/strong><\/p>\n The LPCE-3 incorporates a back-thinned CCD sensor offering enhanced quantum efficiency in the ultraviolet (350\u2013400 nm) and near-infrared (800\u20131050 nm) regions, rendering it indispensable for applications such as horticultural LED evaluation (photomorphogenic response) and solar simulator spectral matching assessment. Both systems feature an auxiliary fiber-optic input for spatially resolved radiance measurements\u2014a critical capability for automotive headlamp beam pattern analysis and display uniformity testing.<\/p>\n The accompanying software suite, LISUN-2, automates data acquisition, computes photometric and colorimetric parameters in accordance with CIE 127:2007 and IESNA LM-79-19 protocols, and generates pass\/fail criteria based on user-defined tolerance limits. Real-time graphing of SPD, chromaticity drift, and flux stability over extended burn-in periods (up to 24 hours) is supported, facilitating reliability and aging studies for LED and OLED manufacturers.<\/p>\n The versatility of the LPCE-2\/LPCE-3 systems enables deployment across a wide spectrum of industries where precise light measurement is paramount. Below, we examine sector-specific use cases, associated testing standards, and measurement challenges addressed by these systems.<\/p>\n For mass-production quality control, the LPCE-2 provides rapid (sub-second) binning of LEDs into flux and chromaticity bins according to ANSI C78.377 and IEC 60081. The system\u2019s 500 mm integrating sphere accommodates up to 10 W LEDs\u2014common in retrofit bulbs and downlights\u2014without thermal overload. OLED panels, which emit Lambertian patterns, benefit from the sphere\u2019s uniform response, enabling accurate extraction of luminance and efficacy (lm\/W) without need for goniometric correction.<\/p>\n Automotive forward-lighting systems (e.g., adaptive driving beams, matrix LEDs) require compliance with ECE R112, R123, and SAE J1383 standards. The LPCE-3\u2019s auxiliary port allows insertion of a luminance standard, enabling calibrated photometric measurements of near-field patterns. For aerospace certification (DO-160, MIL-STD-810), the system\u2019s temperature-controlled detector ensures stable readings from -40\u00b0C to +85\u00b0C ambient conditions, critical for wingtip and landing light validation.<\/p>\n In display metrology, the LPCE-3 measures emission spectra of OLED and microLED screens, computing color volume (DCI-P3, sRGB coverage) and flicker-induced temporal chromaticity shift. For photovoltaic module qualification (IEC 60904-9), the spectroradiometer assesses spectral mismatch between the test solar simulator and AM1.5G reference spectrum, enabling correction factors for certified module efficiency.<\/p>\n Research institutions developing LED-based fluorescence excitation sources or field programmable gate array (FPGA)-driven hyperspectral imagers utilize the LPCE-2\u2019s stability (drift <0.1% over 8 hours) to validate prototype designs. The software\u2019s scripting capability (Python API) allows automated iteration of hundreds of operating conditions, accelerating iterative design cycles.<\/p>\n Urban lighting consultants evaluate potential light pollution using the system\u2019s SPD data to compute scotopic\/photopic ratios and correlated color temperature uniformity across streetlight arrays. Stage lighting manufacturers\u2014such as those producing moving heads with variable CCT\u2014use the LPCE-3\u2019s TM-30 output (fidelity index Rf, gamut index Rg) to ensure skin-tone rendering accuracy under complex tunable-white spectra. Medical lighting systems (surgical luminaires, phototherapy lamps) require CRI >95 and minimal UV leakage; the LPCE-3\u2019s extended UV detection (350 nm) confirms compliance with IEC 60601-2-41.<\/p>\n Navigation lights (COLREGS-compliant) demand precise chromaticity boundaries defined by CIE S015. The LPCE-2\u2019s automated pass\/fail classification of CIE xy coordinates within 0.001 tolerance ensures each fixture meets maritime safety standards without manual goniophotometry.<\/p>\n When benchmarked against alternative measurement architectures (e.g., goniophotometers or spectral radiance meters), the integrated sphere\u2013spectroradiometer approach offers distinct advantages in speed, cost, and multiparameter extraction.<\/p>\n Throughput advantage<\/strong>: A typical goniophotometer requires 10\u201330 minutes to obtain total luminous flux via integration of angular intensity distributions. The LPCE-2\/3 achieves the same with a single 100 ms acquisition\u2014a 6000x improvement suitable for inline production lines.<\/p>\n Spectral fidelity<\/strong>: Unlike photopic-filtered illuminance meters (which exhibit up to 5% error for non-standard SPDs), the spectroradiometer captures the full SPD, enabling accurate calculation of any colorimetric quantity (e.g., chromaticity, CCT) without filter mismatch.<\/p>\n Stray light correction<\/strong>: The LPCE-3 employs a proprietary stray light subtraction algorithm based on iterative spectral convolution. Comparative testing against a reference double-monochromator system (Kontron SFM-25) demonstrated agreement within 0.3% for flux measurements of blue (450 nm) and phosphor-converted white LEDs\u2014a performance metric superior to most single-monochromator systems operating without correction.<\/p>\n Auxiliary measurement capabilities<\/strong>: Both systems support simultaneous electrical measurement (voltage, current, power) via integrated four-quadrant programmable supplies. This allows real-time efficacy (lm\/W) computation during thermal stabilization\u2014critical for detecting efficiency droop at high drive currents.<\/p>\n To achieve reliable industrial measurements, users must consider error sources unique to integrating sphere systems: self-absorption by the DUT (significant for large fixtures), sphere wall degradation over time (barium sulfate coating undergoes hygroscopic yellowing), and detector linearity deviations for low or high flux levels.<\/p>\n The LPCE-2\/3 systems incorporate an auxiliary lamp for self-absorption correction; the user measures the sphere\u2019s response to a reference lamp with and without the DUT present, computing a correction factor applied to all subsequent measurements. For high-purity white LEDs (CCT >5000 K), the self-absorption correction can amount to 2\u20133% of total flux.<\/p>\n Calibration intervals are recommended at 12 months for routine production use and 6 months for research applications. LISUN offers a calibration service utilizing a NIST-traceable 150 W quartz tungsten halogen lamp (CIE source A) and a deuterium lamp for UV validation. The calibration certificate provides expanded uncertainties (k=2) for both photometric and spectral quantities.<\/p>\n 1. Can the LPCE-2 measure luminous flux of high-power LED modules exceeding 100 W?<\/strong> 2. How does the LPCE-3\u2019s back-thinned CCD improve measurement capability for UV LEDs?<\/strong> 3. What is the procedure for validating system performance between calibrations?<\/strong> 4. Can the system measure pulsed LED signals, such as those used in pulse-width modulation (PWM) dimming?<\/strong> 5. Is the software capable of exporting data in formats compatible with statistical process control (SPC) systems?<\/strong> Introduction to High-Precision Photometric and Colorimetric Metrology for Solid-State Lighting The rapid proliferation of solid-state lighting (SSL) technologies\u2014encompassing LEDs and OLEDs\u2014has necessitated a paradigm shift in optical measurement methodologies. Unlike conventional incandescent or fluorescent sources, LED emissions are characterized by narrow spectral bands, high luminous efficacy, and temperature-dependent chromaticity shifts. These unique attributes render traditional […]<\/p>\n","protected":false},"author":1,"featured_media":3432,"comment_status":"closed","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[1187],"class_list":["post-8660","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-blogs","tag-led-measurement-machine"],"_links":{"self":[{"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/posts\/8660","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/comments?post=8660"}],"version-history":[{"count":1,"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/posts\/8660\/revisions"}],"predecessor-version":[{"id":8661,"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/posts\/8660\/revisions\/8661"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/media\/3432"}],"wp:attachment":[{"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/media?parent=8660"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/categories?post=8660"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/ledtestsystem.com\/fr\/wp-json\/wp\/v2\/tags?post=8660"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}Sph\u00e8re int\u00e9gratrice<\/a> and Spectroradiometer Synergy: Theoretical Foundations for Luminous Flux and Spectral Analysis<\/h2>\n
LISUN LPCE-2 and LPCE-3 System Specifications and Operational Architecture<\/h2>\n
\n\n
\n \nParam\u00e8tre<\/th>\n LPCE-2<\/th>\n LPCE-3<\/th>\n<\/tr>\n<\/thead>\n \n Type de d\u00e9tecteur<\/td>\n CCD Array (2048 pixels)<\/td>\n Back-thinned CCD (2048 pixels)<\/td>\n<\/tr>\n \n Gamme spectrale<\/td>\n 380\u2013800 nm<\/td>\n 350\u20131050 nm<\/td>\n<\/tr>\n \n Pr\u00e9cision de la longueur d'onde<\/td>\n \u00b10.3 nm<\/td>\n \u00b10.2 nm<\/td>\n<\/tr>\n \n Stray Light Suppression<\/td>\n <0.1% (at 635 nm)<\/td>\n <0.05% (at 635 nm)<\/td>\n<\/tr>\n \n Sphere Diameter Options<\/td>\n 300 mm, 500 mm, 1000 mm<\/td>\n 300 mm, 500 mm, 1000 mm, 2000 mm<\/td>\n<\/tr>\n \n Measurement Speed (full spectrum)<\/td>\n 10 ms\u201310 s<\/td>\n 5 ms\u20135 s<\/td>\n<\/tr>\n \n Maximum Luminous Flux Range<\/td>\n 0.1\u2013100,000 lm<\/td>\n 0.01\u2013200,000 lm<\/td>\n<\/tr>\n \n CRI Calculation<\/td>\n R\u2090, R\u2081\u2013R\u2081\u2085<\/td>\n R\u2090, R\u2081\u2013R\u2081\u2085, TM-30 (Rf, Rg)<\/td>\n<\/tr>\n \n Power Supply Integration<\/td>\n AC\/DC programmable source (0\u2013300 V, 0\u20135 A)<\/td>\n AC\/DC programmable source with pulse mode (0\u2013600 V, 0\u201310 A)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n Industrial Metrology Applications Across Thirteen Distinct Sectors<\/h2>\n
Lighting Industry and LED\/OLED Manufacturing<\/h3>\n
Automotive Lighting Testing and Aerospace\/Aviation Lighting<\/h3>\n
Display Equipment Testing and Photovoltaic Industry<\/h3>\n
Optical Instrument R&D and Scientific Research Laboratories<\/h3>\n
Urban Lighting Design, Stage\/Studio Lighting, and Medical Lighting Equipment<\/h3>\n
Marine and Navigation Lighting<\/h3>\n
Competitive Advantages and Comparative System Performance Metrics<\/h2>\n
Measurement Uncertainty Considerations and Calibration Protocols<\/h2>\n
Frequently Asked Questions Regarding LISUN LPCE-2 and LPCE-3 Systems<\/h2>\n
\nYes, provided the module\u2019s physical dimensions fit within the integrating sphere. The LPCE-2 with a 1000 mm sphere supports thermal dissipation of up to 200 W using an external heat sink connected via a thermally conductive port. Ensure that the auxiliary air-cooling fan is operational to prevent internal temperature rise above 50\u00b0C, which could corrupt measurement accuracy due to sphere coating moisture desorption.<\/p>\n
\nThe back-thinned CCD\u2019s quantum efficiency at 365 nm (common UV LED peak) is approximately 65%, compared to 35% for conventional front-illuminated CCDs. This reduces integration time by nearly half, minimizing the contribution of dark current noise and enabling detection of UV LEDs with radiant flux as low as 1 \u00b5W without external preamplification.<\/p>\n
\nUsers should perform a daily check using a calibrated reference lamp (supplied with the system) in a fixed orientation. Measure and log the CCT and total flux; historical data should fall within \u00b10.5% of the baseline for spectral parameters and \u00b11.0% for flux. Any deviation exceeding \u00b12% warrants recalibration before proceeding with production measurements.<\/p>\n
\nYes. The LPCE-3 supports a fast-integrating mode with a minimum integration time of 5 ms. For PWM frequencies above 500 Hz, the system averages multiple acquisitions to mitigate aliasing. For frequencies below 200 Hz, the pulse-mode power supply synchronizes the measurement window with the LED on-time to exclude the transient overshoot characteristic of inductive driving circuits.<\/p>\n
\nThe LISUN-2 software exports measurement files in CSV, XML, and JSON formats. Additionally, a TCP\/IP socket interface allows direct transmission of measurement data to external databases (e.g., SQL, MySQL) for real-time SPC monitoring. Custom field definitions (e.g., batch number, operator ID) can be appended to each record for traceability audits under ISO 9001.<\/p>","protected":false},"excerpt":{"rendered":"