{"id":9646,"date":"2026-08-20T20:24:53","date_gmt":"2026-08-20T12:24:53","guid":{"rendered":"https:\/\/www.ledtestsystem.com\/?p=9646"},"modified":"2026-08-20T20:24:53","modified_gmt":"2026-08-20T12:24:53","slug":"lisun-lumen-tester-precision-photometric-measurement-solutions-for-led","status":"publish","type":"post","link":"https:\/\/ledtestsystem.com\/de\/blogs\/lisun-lumen-tester-precision-photometric-measurement-solutions-for-led\/","title":{"rendered":"LISUN Lumen Tester: Precision Photometric Measurement Solutions for LED"},"content":{"rendered":"

LISUN<\/a> Lumen Tester: Precision Photometric Measurement Solutions for LED<\/strong>
\nAn In-depth Analysis of the LPCE-2\/LPCE-3 Ulbrichtsche Kugel<\/a> and Spectroradiometer System for Solid-State Lighting Metrology<\/em><\/p>\n

Introduction to Photometric Metrology in Solid-State Lighting<\/strong>
\nThe rapid proliferation of light-emitting diode (LED) technology across general illumination, automotive headlamps, aviation beacons, and medical devices necessitates robust, traceable measurement infrastructure. Unlike incandescent sources, LEDs exhibit narrow spectral bands, high luminous efficacy variability, and temperature-dependent flux output, rendering conventional photometric heads with CIE spectral correction insufficient for accurate lumen determination. The LISUN Lumen Tester, specifically realized in the LPCE-2<\/strong> Und LPCE-3<\/strong> Integrating Sphere and Spectroradiometer Systems, addresses these challenges by offering absolute photometric, radiometric, and colorimetric characterization based on spectral measurement principles. This article details the instrumental architecture, operational physics, industrial applications, and compliance advantages of the LPCE series, underscoring its role as a definitive solution in precision photometry for LED and OLED sources.<\/p>\n

Unique Subheading 1: Operational Fundamentals of the Integrating Sphere-Spectroradiometer Coupling<\/strong>
\nThe core of the LISUN Lumen Tester lies in the synchronous operation of a high-reflectance Integrationskugel<\/a> and a array-based spectroradiometer. The integrating sphere, available in diameters of 0.3 m, 0.5 m, 1.0 m, 1.5 m, and 2.0 m for the LPCE-2, and 0.3 m to 1.0 m for the LPCE-3, homogenizes the spatial emission from the Device Under Test (DUT). The interior coating, composed of barium sulfate (BaSO\u2084) or PTFE-based material, exhibits a diffuse reflectance greater than 97% across the 380 nm to 780 nm visible range. This ensures the photometric flux incident on the sphere wall achieves a Lambertian distribution, effectively eliminating directional artifacts caused by LED die orientation or secondary optics.<\/p>\n

The spectroradiometer, typically a Czerny-Turner or crossed-CT design with a back-illuminated CCD or CMOS detector, captures the spectral power distribution (SPD) from the sphere\u2019s port. The total luminous flux (\u03a6v) is subsequently derived through numerical integration of the SPD weighted by the CIE 1924 photopic luminosity function (V(\u03bb)). The LPCE-3 model distinguishes itself by incorporating a faster grating scanning mechanism and a higher dynamic range (up to 66000:1), enabling measurements of high-lumen LED modules without external attenuators, whereas the LPCE-2 includes a built-in DC\/AC power supply and a programmable constant-current source for precise DUT drive control.<\/p>\n

Unique Subheading 2: Spectral and Spatial Error Mitigation in High-Reflectance Cavities<\/strong>
\nA critical deficiency in conventional integrating sphere systems is the self-absorption effect\u2014a phenomenon where the DUT and auxiliary fixtures absorb a fraction of the reflected light, leading to underestimated flux readings. The LISUN LPCE-2 and LPCE-3 systems incorporate a spectral correction algorithm<\/strong> based on the auxiliary lamp method. A stabilized tungsten-halogen reference lamp is mounted inside the sphere; its SPD is measured before and after DUT placement. The ratio of these two measurements yields a wavelength-dependent correction factor (k(\u03bb)), which is applied to the DUT spectrum. This compensates not only for self-absorption but also for particulate surface degradation of the sphere coating over time.<\/p>\n

Moreover, spatial non-uniformity of the sphere\u2019s radiance is addressed by orienting the DUT towards the sphere center with a 4\u03c0 or 2\u03c0 geometry, depending on the luminous flux testing standard (e.g., CIE 84, LM-79-08, or IES LM-78). The system\u2019s baffle design and port-to-sphere diameter ratio (maintained below 0.1) minimize the direct illumination of the detector port by the DUT, restricting the detector field-of-view solely to diffuse reflections. For goniophotometric correlation, the LPCE-3 offers an optional external goniometer interface, allowing simultaneous measurement of luminous intensity distribution and total flux, thus validating the sphere results against the absolute integrating method.<\/p>\n

Unique Subheading 3: Wavelength Calibration and Spectral Resolution Compliance for CIE Standards<\/strong>
\nAccurate lumen determination is contingent on the spectroradiometer\u2019s wavelength accuracy and bandwidth. The LPCE-2 and LPCE-3 systems are factory-aligned using low-pressure mercury-argon (Hg-Ar) and argon (Ar) atomic emission lines, yielding a wavelength accuracy of \u00b10.2 nm and a wavelength repeatability of \u00b10.05 nm. The spectral bandwidth (FWHM) is configurable between 0.5 nm and 5 nm via slit width adjustment. This satisfies the CIE 127 and CIE 13.3 requirements for color rendering index (CRI) and chromaticity coordinate calculation. For chromaticity, the system computes x, y, u’, v’ CIE coordinates directly from the SPD, but also outputs correlated color temperature (CCT) using the Robertson method and the CIE 13.3-1995 CRI R\u2081\u2013R\u2081\u2085 indices.<\/p>\n

An integral feature is the wavelength-dependent calibration traceable to the National Institute of Metrology (NIM) via a standard lamp. The calibration coefficients are stored in a non-volatile memory within the spectroradiometer, permitting field recalibration by the user using an optional spectral irradiance standard. This is particularly crucial for photovoltaic and aerospace sectors where spectral mismatch factors (e.g., AM1.5G reference spectra) require rigorously calibrated irradiance data rather than relative photometric output.<\/p>\n

Unique Subheading 4: Integrating Sphere Size and Geometry Selection for Diverse Luminous Flux Ranges<\/strong>
\nThe selection between LPCE-2 and LPCE-3 depends on the DUT\u2019s physical dimensions and luminous flux magnitude. Strict adherence to the \u201c20% rule\u201d\u2014the DUT\u2019s projected area should not exceed 20% of the sphere\u2019s port area\u2014is recommended to maintain measurement accuracy within \u00b11%. The table below summarizes the recommended configurations:<\/p>\n\n\n\n\n\n\n\n\n
Kugeldurchmesser<\/th>\nTypical DUT Flux Range<\/th>\nDominant Application<\/th>\nRecommended Model<\/th>\n<\/tr>\n<\/thead>\n
0.3 m<\/td>\n1 \u2013 2,000 lm<\/td>\nSmall LED packages, SMD components, automotive interior lamps<\/td>\nLPCE-3<\/td>\n<\/tr>\n
0.5 m<\/td>\n10 \u2013 20,000 lm<\/td>\nDownlights, LED tubes, AR\/VR display backlights<\/td>\nLPCE-2 \/ LPCE-3<\/td>\n<\/tr>\n
1.0 m<\/td>\n100 \u2013 100,000 lm<\/td>\nHigh-bay fixtures, streetlights, stadium projectors<\/td>\nLPCE-2<\/td>\n<\/tr>\n
1.5 m \u2013 2.0 m<\/td>\n> 50,000 lm<\/td>\nMarine searchlights, aviation runway lights, gigawatt-class medical phototherapy units<\/td>\nLPCE-2 + Auxiliary Lamp<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

The LPCE-2 includes a switchable integrating sphere<\/strong> design, where the upper hemisphere can be lifted via an electric hoist for large DUT placement, simplifying logistics in manufacturing lines. Conversely, the LPCE-3 eschews this mechanical complexity, instead offering a miniature fiber-optic feedthrough<\/strong> that couples to a second external spectroradiometer, enabling multi-spectral detection for dual-lamp or redundancy measurements.<\/p>\n

Unique Subheading 5: Electrical and Environmental Parameter Control for Reproducible LED Measurements<\/strong>
\nLED luminous flux is intrinsically sensitive to junction temperature (Tj) and forward current (If). The LISUN LPCE-2 integrates a programmable DC power source (0-300V, 0-5A for the high-current variant) with a constant-current mode accuracy of \u00b10.1%. The instrument performs a single-pulse measurement<\/strong> technique: a current pulse with a width of 20 ms is applied, and the SPD is captured within the pulse duration, minimizing the junction temperature rise to less than 2\u00b0C above ambient. This accords with the IES LM-85-14 methodology for electrical and photometric measurements of high-power LEDs.<\/p>\n

For thermal steady-state analysis, the LPCE-3 offers an external temperature probe interface, recording the case temperature (Tc) and heat sink temperature (Tcase) concurrently with the spectral scan. This permits the derivation of the luminous flux derating curve (\u0394\u03a6v\/\u0394Tj), critical for automotive lighting applications where operating temperatures range from -40\u00b0C to 105\u00b0C. Additionally, the system\u2019s internal enclosure is purged with dry nitrogen when operating in high-humidity industrial environments, preventing moisture absorption in the sphere coating and consequent drift in the near-infrared spectral response.<\/p>\n

Unique Subheading 6: Compliance with LM-79-08, CIE 84, and IES LM-78 for Absolute Photometry<\/strong>
\nRegulatory acceptance of a lumen tester hinges on its adherence to established measurement standards. The LISUN LPCE-2\/LPCE-3 systems are designed to comply with the following norms:<\/p>\n

    \n
  • IES LM-79-08<\/strong>: Approved method for the electrical and photometric measurements of solid-state lighting products. The system supports the required 4\u03c0 (sphere) or 2\u03c0 (rod) geometry, constant-current or constant-voltage operation, and ambient temperature monitoring of 25\u00b0C \u00b1 1\u00b0C.<\/li>\n
  • CIE 84-1989<\/strong>: Measurement of luminous flux, which stipulates the use of an integrating sphere photometer with a spectral mismatch correction factor (f1′ \u2264 3%). The LISUN spectroradiometer achieves an f1′ of 1.5% due to its superior stray light suppression (\u2264 0.04% @ 380 nm).<\/li>\n
  • IES LM-78-02<\/strong>: Total flux measurement of electric lamps\u2014this provision is relevant for legacy testing of halogen or fluorescent sources, which the system also accommodates via its wide spectral range (200 nm \u2013 1100 nm with the optional UV\/VIS extension).<\/li>\n<\/ul>\n

    The LISUN software suite performs automated calculations for Lichtausbeute (lm\/W)<\/strong>, luminous flux<\/strong>, PPF (Photosynthetic Photon Flux)<\/strong> for horticultural lighting, and energy efficiency index (EEI)<\/strong>. It generates a test report in PDF or Excel format that includes all original spectral data, ensuring full traceability for ISO 17025 accreditation audits.<\/p>\n

    Unique Subheading 7: Application-Specific Configurations in Automotive, Aerospace, and Display Sectors<\/strong>
    \nThe versatility of the LPCE-2\/LPCE-3 extends beyond conventional indoor lighting. In Pr\u00fcfung der Fahrzeugbeleuchtung<\/strong>, the system supports pulsed measurements of LED light sources used in adaptive driving beams (ADB). The high temporal resolution of the spectroradiometer (integration time down to 1 ms) allows the capture of flicker and transient luminescence characteristics, which are mandated by the UN\/ECE R112 and R149 regulations. For Beleuchtung f\u00fcr Luft- und Raumfahrt<\/strong>, the sphere system may be equipped with a specialized port for measuring chromaticity coordinates of cockpit backlight panels and runway edge lights in accordance with SAE AS25050. The system\u2019s ability to measure scotopic\/photopic lumens (S\/P ratio)<\/strong> is directly applicable to night-vision imaging system (NVIS) compatibility testing.<\/p>\n

    In Pr\u00fcfung von Anzeigeger\u00e4ten<\/strong>, the LPCE-3\u2019s narrow bandwidth (0.5 nm FWHM) distinguishes near-spectral emissions of OLED microdisplays, ensuring accurate white point calibration for AR\/VR headsets. The inclusion of a 2 nm spectral scanning step<\/strong> for rapid production-line measurements enables a throughput of up to 1,000 units per hour when integrated with robotic handling. For the Photovoltaikindustrie<\/strong>, the system\u2019s dual-role as an irradiance meter (via a cosine-corrected diffuser) allows it to measure the spectral mismatch coefficient (MM) between simulated sunlight and AM1.5G reference, correcting the short-circuit current (Isc) of solar cells during efficiency testing.<\/p>\n

    Unique Subheading 8: Data Acquisition, Software Integration, and Real-Time Luminous Flux Monitoring<\/strong>
    \nThe LISUN LSG-3000 and LSR-3000 software interfaces provide a dedicated digital control layer for the lumen tester. The software supports multi-threaded data logging<\/strong>, capturing up to 100 data points per second from the spectroradiometer\u2019s 16-bit ADC. A proprietary auto-ranging algorithm<\/strong> dynamically adjusts the integration time and number of accumulations to prevent saturation at high luminance levels while preserving linearity at low flux values (down to 0.1 lm). The instrument computes the total spectral radiant flux (W\/nm)<\/strong> and the luminous flux (lm)<\/strong> in accordance with the CIE system, while also outputting the color rendering index (Ra)<\/strong> across all eight standard test color samples (TCS1-TCS8).<\/p>\n

    F\u00fcr urban lighting design and smart-city deployment<\/strong>, the software exports a spatial flux map<\/strong> when coupled with the optional goniometer. This map, combined with the sphere-derived total flux, enables the calculation of utilance<\/strong>\u2014the ratio of luminous flux received on the working plane to the total flux emitted by the luminaire. For B\u00fchnen- und Studiobeleuchtung<\/strong>, the tester profiles the spectral output of moving-head LED fixtures under various dimming curves, evaluating color consistency (\u0394uv) across dimming levels, which is pivotal for color-mixing accuracy in entertainment environments.<\/p>\n

    FAQ-Abschnitt<\/strong>
    \nQ1: How does the LISUN LPCE-2 compensate for the absorption of light by the LED fixture under test?<\/strong>
    \nA1: The LPCE-2 employs an auxiliary reference lamp method. A stabilized tungsten-halogen lamp with a known SPD is operated inside the sphere; the system measures the sphere\u2019s spectral response with the DUT present and absent. The ratio of these measurements generates a wavelength-dependent correction matrix (k(\u03bb)), which multiplies the raw DUT spectrum. This corrects not only for self-absorption but also for any geometric obstruction caused by the DUT\u2019s housing or heat sink.<\/p>\n

    Q2: Is the LPCE-3 suitable for measuring the absolute luminous flux of high-power LED arrays exceeding 50,000 lumens?<\/strong>
    \nA2: Yes, but with caveats. The LPCE-3\u2019s standard configuration with a 0.5 m sphere is tailored for flux up to 20,000 lm. For flux ratings above this, we recommend the LPCE-2 with a 1.5 m or 2.0 m sphere and the high-sensitivity detector mode, which reduces the incident irradiance at the detector port. Alternatively, the LPCE-3 can be equipped with an external neutral density attenuator (ND2 to ND4) to prevent detector saturation, albeit with a slight sacrifice in signal-to-noise ratio.<\/p>\n

    Q3: What is the minimum spectral resolution required to calculate the CRI Ra with an accuracy of \u00b11%?<\/strong>
    \nA3: The CIE 13.3 method calculates CRI based on the average of eight specific chromaticity differences. To resolve these differences accurately, a spectral bandwidth of 2 nm or smaller is recommended. The LPCE-2 and LPCE-3 are factory configured with a 1.0 nm FWHM, yielding an uncertainty in Ra of less than \u00b10.3% for standard white LEDs. For narrow-band phosphor-converted LEDs (e.g., with a red emission peak at 630 nm), a 0.5 nm bandwidth is essential to avoid smearing of spectral features.<\/p>\n

    Q4: Can the system perform measurements in a 2\u03c0 (hemispherical) geometry for directional light sources?<\/strong>
    \nA4: Yes. Both LPCE-2 and LPCE-3 offer an optional 2\u03c0 adapter\u2014a masking plate that covers one hemisphere of the sphere. This configuration is critical for measuring luminous flux of downlights, truncheon lamps, and other single-direction emission sources, where a 4\u03c0 measurement would overestimate flux due to back-reflections. The system automatically recalculates the calibration factor when switching between 4\u03c0 and 2\u03c0 modes.<\/p>\n

    Q5: How does the instrument maintain calibration stability in harsh industrial environments with varying temperature and humidity?<\/strong>
    \nA5: The spectroradiometer core is thermally stabilized via a Peltier element, maintaining the detector temperature at 10\u00b0C \u00b1 0.1\u00b0C regardless of ambient variations (15\u00b0C to 35\u00b0C). The sphere enclosure is sealed with O-ring gaskets, and a desiccant cartridge is included for humidity control. The system\u2019s calibration coefficients are stored in non-volatile memory and are automatically recalled upon power-up. LISUN recommends a full recalibration interval of 12 months, though the internal drift monitoring function (using the auxiliary lamp) alerts the user when the deviation exceeds 1% of the initial value.<\/p>","protected":false},"excerpt":{"rendered":"

    LISUN Lumen Tester: Precision Photometric Measurement Solutions for LED An In-depth Analysis of the LPCE-2\/LPCE-3 Integrating Sphere and Spectroradiometer System for Solid-State Lighting Metrology Introduction to Photometric Metrology in Solid-State Lighting The rapid proliferation of light-emitting diode (LED) technology across general illumination, automotive headlamps, aviation beacons, and medical devices necessitates robust, traceable measurement infrastructure. Unlike […]<\/p>\n","protected":false},"author":1,"featured_media":3432,"comment_status":"closed","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[1069],"class_list":["post-9646","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-blogs","tag-lumen-tester"],"_links":{"self":[{"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/posts\/9646","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/comments?post=9646"}],"version-history":[{"count":1,"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/posts\/9646\/revisions"}],"predecessor-version":[{"id":9647,"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/posts\/9646\/revisions\/9647"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/media\/3432"}],"wp:attachment":[{"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/media?parent=9646"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/categories?post=9646"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/ledtestsystem.com\/de\/wp-json\/wp\/v2\/tags?post=9646"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}