In the process scale-up of photochemical synthesis, traditional batch reactors often face two major physical bottlenecks: first, limited light transmission leads to uneven distribution, where local overexposure easily causes side reactions and prolongs reaction cycles; second, low heat and mass transfer efficiency in large volumes, where heat accumulation tends to reduce product selectivity. Therefore, obtaining accurate and reproducible continuous flow process data before pilot scale has become the primary challenge for researchers and engineers.
To address the core pain points of uneven illumination, limited heat and mass transfer, and difficult process scale-up, PerfectLight has launched the PLR DPCT-O50 Small Coiled-Tube Photoreactor, specifically designed for bench-scale exploration and process optimization. Based on millimeter-scale tubular continuous flow design, this device aims to provide highly uniform illumination conditions, as well as precisely controllable flow field and heat transfer environment for reaction systems.

As the "massless reagent" of photochemical reactions, the uniformity of photon distribution directly affects the conversion rate and selectivity of reactions.
The PLR DPCT-O50 adopts a double-sided LED light source with opposite irradiation design, delivering an effective illumination area of 200×200 mm. According to the Beer-Lambert Law, unilateral illumination causes exponential light intensity attenuation when penetrating the reaction solution. In contrast, double-sided opposite irradiation effectively compensates for the radial "dark zones" caused by one-sided illumination through symmetric superposition of light fields. This design provides high optical power density while significantly flattening the radial light intensity gradient of the fluid inside the tubes.

For reaction systems extremely sensitive to "light exposure dose", the device features a 2D planar spiral coiled tube (mosquito-coil-shaped) configuration, with advantages in the following aspects:
The device is equipped with a standard chiller, controlling the operating temperature of the reaction tubing within a wide range of -20 to 80°C.
The light source has an electrical power of up to 300 W (rated electrical power, with a power adjustment range of 10% to 100%). Customized electrical power specifications are also available, with an upper limit expandable to 1 kW. While the light source outputs high-intensity photons, the water cooling system rapidly dissipates waste heat generated by non-radiative transitions of LEDs and heat converted from light energy absorbed by the reaction system. Through an independent efficient heat exchange mechanism, it achieves effective "decoupling" of photon flux and system temperature, ensuring constant temperature of core reaction materials and thus guaranteeing high reproducibility of experimental data.
The main body adopts a square bracket design. This industrial structure not only occupies a small footprint but also facilitates subsequent multi-station series connection and process scale-up expansion.
| Feature | Specification |
|---|---|
| Reaction Tube | 1/4 in × 1/8 in (OD × ID), FEP/PFA (other millimeter-scale diameters available) |
| Liquid Holding Capacity | Approx. 50 mL, double-layer staggered coiling (other capacities available) |
| Operating Range | 0 ~ 1 MPa, -20 ~ 80 °C |
| Optical Window | Effective area approx. 200 mm, quartz optical window |
| Light Source Wavelength | 450 nm, compatible with other wavelengths (255 ~ 760 nm) |
| Light Source Power | 300 W (rated electrical power, 10 ~ 100%), other powers available, up to 1 kW |
Applicable Systems: Homogeneous liquid phase systems, gas-liquid / liquid-liquid two-phase systems.
Typical Applications: