Engineers new to UV curing often use "UV power" and "UV dose" interchangeably, as if they describe the same thing with different words. They do not. The confusion between these two parameters is a direct route to under-cured adhesive, inconsistent bond performance, and the frustrating inability to reproduce a process from one production run to the next. Understanding exactly what each term means — and where each one matters in the curing process — resolves most process setup problems before they start. UV Power: A Property of the Lamp UV power, expressed in milliwatts (mW) or watts (W), is the total radiant output of the curing lamp — the rate at which the lamp emits UV energy. It is a property of the light source itself, measured at the lamp's output aperture or at a reference point defined by the manufacturer. UV power tells you how much energy the lamp is producing, but it says nothing about how that energy is distributed over the cure surface or how much of it actually reaches the adhesive. A lamp with 10 W of UV output illuminating a 10 cm² area delivers very different irradiance than the same lamp focused onto a 1 cm² spot. The power is the same in both cases; the intensity at the cure surface is not. Irradiance: Power per Unit Area The parameter that describes UV intensity at the cure surface is irradiance — expressed in mW/cm². Irradiance is derived from the lamp's UV power and the area over which that power is distributed: Irradiance (mW/cm²) = UV Power (mW) ÷ Cure Area (cm²) In practice, irradiance is measured directly at the cure surface with a calibrated radiometer rather than calculated from lamp power, because optical losses in the light guide, reflections at optic surfaces, and beam divergence all reduce the fraction of lamp power that arrives at the substrate. Irradiance is the parameter that adhesive manufacturers specify as a requirement — because it is the quantity experienced by the adhesive, not the quantity emitted by the lamp. UV Dose: Energy Delivered Over Time UV dose, expressed in mJ/cm², is the total UV energy received by the cure surface over the full exposure period. It is calculated as: UV Dose (mJ/cm²) = Irradiance (mW/cm²) × Exposure Time (seconds) Dose accumulates as long as the lamp is on. A lamp delivering 2,000 mW/cm² for 1 second deposits 2,000 mJ/cm² of dose. The same lamp running for 2 seconds deposits 4,000 mJ/cm². Dose is the total photochemical work done on the adhesive — the cumulative photon exposure that drives polymerization to completion. Adhesive manufacturers specify a required dose range for each product. Below the minimum dose, polymerization is incomplete and the bond will not achieve its specified mechanical properties. Above the maximum dose, some formulations show no further improvement; others may exhibit degradation from over-exposure. The Relationship Between Power, Irradiance, and Dose These three parameters form a chain: the lamp's power determines the available UV output; the optical system converts…

On a circuit board where components are spaced 1.5 mm apart, or in a camera module where a lens must be bonded without UV reaching the image sensor 2 mm away, the spatial precision of a UV curing system is not a refinement — it is a hard requirement. UV LED spot lamps are specifically designed to meet this requirement, and the combination of optical engineering, delivery system design, and process control that enables pinpoint curing accuracy is worth understanding in detail. Defining Curing Accuracy Curing accuracy in a UV spot lamp context means the ability to deliver a defined dose of UV light to a specific, bounded area while minimizing UV exposure to adjacent regions. Two spatial parameters define this performance: spot size at the work surface and spot uniformity within that area. A spot lamp that delivers high irradiance to the center of a 5 mm diameter circle but drops to 10% at the edges produces an inconsistent cure across the bondline. A spot lamp that delivers uniform irradiance across a 3 mm diameter circle but also illuminates 15 mm of surrounding substrate is not spatially accurate for a tight-clearance application. The Optical Delivery System The foundation of spatial accuracy in a UV spot lamp is the light guide and cure head optics. Light travels from the LED array through a liquid or fiber optic guide and exits at the cure head. The angular distribution of that exit beam is determined by the guide's numerical aperture — a parameter describing the range of angles over which light exits the distal face. A cure head without focusing optics produces a diverging beam: the spot size at the work surface increases with working distance, and the irradiance decreases as the beam spreads. This diverging behavior limits spatial accuracy at longer working distances. Most UV spot lamp cure heads include a focusing lens or a collimating lens to reshape this output. A focusing lens converges the beam to a smaller diameter at a defined focal distance, producing higher irradiance in a smaller area. A collimating lens produces a more parallel beam that maintains a consistent diameter over a useful working distance range. Both approaches improve spatial accuracy compared to an unfocused light guide exit. Apertures and Field-Limiting Accessories Where geometry allows, a physical aperture — essentially a plate with a precision hole — mounted at the cure head can further restrict the illuminated area. Light passing through the aperture reaches the substrate; light outside the aperture boundary is blocked. Apertures are particularly effective when curing adhesive in a via or port where the surrounding substrate must remain UV-free. Aperture accessories for UV spot lamp cure heads are available in standard diameters and can be custom-fabricated for demanding applications. The selection of aperture size must account for the spot size at the working distance: an aperture smaller than the beam diameter wastes UV power; an aperture larger than the desired cure area provides no spatial restriction. Working Distance and Its Effect on…

When a UV LED spot lamp system is delivered to the assembly floor, one of the key hardware decisions the purchasing engineer has already made — sometimes without fully realizing its implications — is the type of light guide. Whether that guide contains an optical fluid or a bundle of silica fibers affects UV throughput, mechanical durability, long-term maintenance costs, and compatibility with the wavelength being used. Both technologies work; which one is right depends on the specific demands of the application. How Each Technology Transports UV Light A liquid light guide uses a flexible polymer or glass tube filled with a purified optical fluid — often a matching-index oil or synthetic fluid — surrounded by a jacket with a lower refractive index. Light entering the guide at the proximal face undergoes total internal reflection at the fluid-jacket boundary and propagates to the distal output face with low loss per unit length. A fiber optic light guide is a bundle of thin glass or fused silica fibers, each individually guiding light by internal reflection at the core-cladding boundary. The bundle is jacketed for mechanical protection. Fused silica is the preferred fiber material for UV applications because it maintains high transmission at wavelengths from 200 nm through the visible range, with low solarization susceptibility. Both technologies rely on the same physics, but the practical differences between them are significant across several dimensions. UV Transmission Efficiency Liquid guides, when filled with a properly matched optical fluid, transmit very efficiently at UV wavelengths between 365 nm and 405 nm. In high-quality designs, transmission losses per meter of guide length are low, and the coupling efficiency at the proximal face can exceed that of fiber bundles because the continuous fluid-filled core captures a larger fraction of the input cone than a fiber bundle's packing fraction allows. Fiber bundles have inherent packing fraction losses — the gaps between individual fibers at the input face do not accept light. A typical round fiber bundle may have a packing fraction of 70–80%, meaning up to 30% of the input face area contributes no light transport. This reduces the effective numerical aperture of the bundle and limits maximum optical throughput compared to a liquid guide of equivalent diameter. For applications that require maximum irradiance at the cure surface, liquid guides generally deliver more UV power to the target. Solarization Resistance Both guide types undergo some degree of UV-induced degradation (solarization) over time. High-intensity UV radiation causes cumulative absorption changes in the guiding material, gradually reducing throughput. Fused silica fiber bundles have inherently low solarization at 365–405 nm due to the material's high purity and resistance to UV-induced color center formation. Well-specified silica fiber guides can maintain high transmission through many thousands of hours of UV exposure. Liquid guides are more variable in solarization resistance. Standard optical fluids show gradual UV-induced degradation; higher-purity fluids or UV-stabilized formulations extend service life. Some liquid guide designs allow the optical fluid to be replaced, resetting transmission performance without replacing the entire guide…

A UV LED spot lamp without a light guide is essentially a powerful light source with no way to deliver that light where it is needed. The light guide is the component that bridges the lamp head — where the LED array and thermal management hardware live — and the cure point on the assembly. Understanding what a light guide is, how it works, and what limits its performance is essential for anyone specifying or operating a UV spot curing system. The Function of a Light Guide In a UV LED spot lamp system, the LED array is typically housed in a separate controller or lamp head unit. This unit contains the electronics, thermal management hardware, and optical components necessary to drive the LEDs at stable output levels. Routing this entire assembly to every cure point in a production cell is impractical, particularly in tight spaces or automated systems where the cure head must move. A light guide solves this problem by transporting the UV light from the LED array to a handheld or fixture-mounted cure head using internal reflection. Light enters the guide at one end — the proximal end, connected to the lamp housing — travels through the guide with minimal loss, and exits at the distal end — the cure head — where it illuminates the adhesive. The lamp head itself does not need to move; the flexible guide delivers the UV output to wherever the cure head is positioned. How Light Is Transported Light guides exploit the physical principle of total internal reflection. When a light ray traveling through a medium with a high refractive index strikes the boundary with a lower-refractive-index medium at an angle beyond the critical angle, the ray is reflected back into the guide rather than transmitted out. In a well-designed light guide, this reflection occurs at every point along the guide's interior walls, and light travels from input to output with relatively low loss per unit length. The angle within which light can enter the guide and still undergo total internal reflection defines the guide's numerical aperture (NA). Light entering at steeper angles — beyond the NA — is not efficiently coupled and is lost as heat in the guide walls. This makes the coupling optics between the LED array and the proximal face of the guide a critical efficiency factor: how much of the LED's raw output falls within the guide's acceptance cone determines how much usable UV power reaches the cure surface. Liquid-Filled Light Guides One common light guide construction uses a flexible tube filled with a transparent liquid — typically a high-purity optical fluid. The liquid provides the high-refractive-index core, and a lower-index jacket or tube wall defines the boundary for total internal reflection. Liquid guides transmit UV efficiently across a wide wavelength range, including the deep UV below 365 nm that solid fiber optics struggle to pass without absorption. They are flexible and can be routed around obstacles in tight assembly cells. Their main limitations are mechanical…

The transition from mercury arc lamps to UV LEDs in manufacturing environments is not as simple as swapping one lamp for another. The adhesive chemistry — specifically the photoinitiators embedded in the resin — was often designed around the spectral output of mercury arc lamps, and understanding how that chemistry responds differently to LED output is what separates a successful lamp migration from a process that produces unreliable bonds and unexplained failures. The Spectral Mismatch Problem Mercury arc lamps emit a broad spectrum of ultraviolet and visible light, with pronounced emission peaks at 254 nm, 303 nm, 313 nm, 334 nm, 365 nm, 405 nm, 436 nm, and other wavelengths. Traditional UV photoinitiators were formulated to absorb across this spectrum, often with broad absorption bands covering 300–400 nm. A single photoinitiator molecule in a mercury lamp adhesive might absorb meaningfully at 313, 334, and 365 nm simultaneously. UV LEDs emit at a single narrow peak, typically 10–20 nm wide at half-maximum. A 365 nm LED produces almost no output at 313 nm or 405 nm. A 395 nm LED produces almost no output at 365 nm. When a mercury-lamp adhesive is exposed to a UV LED, only the portion of the photoinitiator's absorption band that overlaps with the LED's narrow emission contributes to cure. The rest of the absorption spectrum is effectively wasted. Common Mercury-Era Photoinitiators and Their LED Compatibility Benzophenone and benzophenone derivatives are classic free-radical photoinitiators that absorb primarily in the 280–330 nm range. They are poorly suited to UV LED curing at 365 nm and beyond because their absorption drops steeply above 330 nm. Formulations relying on benzophenone as the primary photoinitiator may not cure adequately under any commercially available UV LED. Irgacure 651 (DMPA) has absorption primarily below 350 nm, with meaningful response out to about 365 nm. This photoinitiator performs reasonably under 365 nm LED lamps but shows declining efficiency at 385 nm and above. Adhesives formulated with DMPA as the primary initiator may require significantly higher dose under longer-wavelength LEDs. Irgacure 184 (hydroxy-cyclohexyl-phenyl-ketone) is a widely used alpha-hydroxy ketone photoinitiator with good absorption in the 300–370 nm range. It functions reasonably under 365 nm LED illumination and is often used in LED-compatible formulations, though its efficiency decreases at 385 nm and higher. Irgacure 819 (bisacylphosphine oxide, BAPO) is a photoinitiator specifically designed to absorb into the 370–420 nm range, making it well suited to UV LED curing systems operating at 385–405 nm. Its broader absorption spectrum and high molar absorption coefficient at longer wavelengths make it a frequent choice in adhesives reformulated for LED compatibility. Irgacure TPO (diphenyl(2,4,6-trimethylbenzoyl)phosphine oxide) absorbs from approximately 350 nm to 420 nm, with good response across the typical UV LED emission range. TPO is commonly found in LED-optimized adhesive formulations and supports efficient curing at 365, 385, 395, and 405 nm. Why Reformulation Is Often Required An adhesive formulated for mercury lamp curing may contain photoinitiators that work reasonably well at 365 nm but show degraded performance at 395…

The wavelength selection in a UV LED curing system is not a preference — it is a photochemical requirement. Choose correctly and your adhesive cures completely, repeatably, and at the speed your process demands. Choose incorrectly and you may spend weeks troubleshooting what looks like a dispensing problem, a bondline geometry issue, or a mechanical failure that is actually the wrong photons hitting the wrong photoinitiators. The Basis for Selection: Photoinitiator Absorption The starting point for any wavelength selection is the adhesive's photoinitiator system. Photoinitiators are the molecules that absorb UV photons and generate the reactive species — free radicals or cations — that initiate polymerization. Each photoinitiator has a characteristic absorption spectrum: a curve showing how efficiently it absorbs light at each wavelength. For a UV LED curing lamp to work, its emission peak must fall within the absorption band of the adhesive's photoinitiator. When emission and absorption are well matched, photons are absorbed efficiently and the cure reaction proceeds quickly. When they are mismatched, most photons pass through the adhesive without triggering any photochemical reaction, regardless of how high the irradiance. Adhesive product datasheets for LED-compatible products will specify a recommended wavelength or a recommended wavelength range. That specification is the first filter in wavelength selection. 365 nm: The Mercury-Compatible Choice 365 nm was the dominant UV LED curing wavelength in the early LED adoption period, largely because it corresponds to one of the primary emission lines of mercury arc lamps (the i-line at 365 nm). Adhesives formulated for mercury lamp curing typically have photoinitiators with strong absorption in the 340–380 nm range, making 365 nm LEDs compatible without adhesive reformulation. This wavelength remains important when: - An existing process was originally qualified on a mercury lamp and the adhesive formulation has not changed - The adhesive datasheet explicitly specifies 365 nm - The application requires short-wavelength photons to activate photoinitiators in optically thin layers where higher photon energy improves reaction yield The limitation of 365 nm LEDs is lower wall-plug efficiency compared to longer wavelengths. For a given drive power, a 365 nm LED generates less optical output than a 395 nm or 405 nm LED. This can limit maximum achievable irradiance or require more aggressive thermal management to sustain output. 385 nm: The Transition Wavelength 385 nm occupies a middle position — more efficient than 365 nm in terms of LED output per watt of electrical input, and compatible with a substantial range of photoinitiators. Some adhesive manufacturers have introduced LED-optimized formulations targeting this wavelength specifically. 385 nm is a logical selection when: - The adhesive datasheet recommends 380–390 nm operation - Higher irradiance than a 365 nm system can provide is required - The application involves coatings or inks originally developed for 385 nm printing systems 395 nm: The Industrial LED Curing Workhorse 395 nm represents the point on the UV LED efficiency curve where output per watt is substantially higher than at 365 or 385 nm, and where a wide range of LED-optimized adhesive…

Pick up a UV LED spot lamp catalog from any major manufacturer and you will find the same handful of wavelength options listed across the product range: 365 nm, 385 nm, 395 nm, 405 nm. These numbers are not marketing differentiators or arbitrary specifications — they correspond to discrete emission peaks built into the LED semiconductor structure, and selecting the right wavelength for a given adhesive and application is one of the most consequential decisions in UV curing system design. Why UV LEDs Emit at Discrete Wavelengths Unlike mercury arc lamps, which produce a continuous spectrum of ultraviolet and visible output with peaks at several fixed mercury emission lines, UV LEDs are narrow-band sources. Each LED chip is fabricated from a semiconductor material with a specific bandgap energy, and the light it emits is concentrated in a narrow spectral band — typically with a full-width half-maximum of 10 to 20 nm around the peak wavelength. This narrow emission is a fundamental property of LED physics, not a design choice. The practical consequence is that the wavelength of a UV LED curing lamp must be matched to the photoinitiator chemistry in the adhesive. A photoinitiator that absorbs efficiently at 365 nm may have negligible absorption at 405 nm, and vice versa. Using the wrong wavelength produces low cure rates, incomplete polymerization, or no cure at all — regardless of how high the irradiance or how long the exposure. The Four Standard Wavelengths 365 nm sits at the boundary between UVA and UVB radiation and represents the shortest wavelength widely available in high-power UV LED curing systems. At 365 nm, photon energy is sufficient to activate a broad range of conventional photoinitiators, including Irgacure 184, Irgacure 651, and many photoinitiators used in optical adhesives. Adhesives formulated for mercury lamp curing often have their photoinitiator peak absorption centered near this wavelength, making 365 nm LEDs the natural migration path when switching from mercury to LED. The trade-off is that LED efficiency at 365 nm is lower than at longer wavelengths, which can mean lower available irradiance at a given drive power. 385 nm represents a balance point in the UV LED efficiency curve. Many LED chips achieve higher wall-plug efficiency at 385 nm than at 365 nm, enabling higher irradiance output at the cure surface. Some adhesive photoinitiators are specifically formulated to absorb in the 380–390 nm range. This wavelength is common in printing and graphics applications and is increasingly specified in industrial adhesive formulations designed for LED compatibility. 395 nm falls in a region where LED efficiency is high and cost per milliwatt of output is lower than at shorter UV wavelengths. Many UV-LED-optimized adhesive formulations target this wavelength. Some processes that previously required 365 nm can be reformulated for 395 nm operation, gaining irradiance and system efficiency without sacrificing cure performance. 405 nm is at the visible violet boundary — light at this wavelength is faintly perceptible as deep violet to the human eye. LED chips at 405 nm are highly…

Two assemblies cured under different UV LED settings can look identical when they come off the line and produce completely different bond strengths in pull testing. The explanation almost always comes back to a misunderstanding of two parameters that seem interchangeable but are not: UV intensity and UV dose. Getting these right is not an academic exercise — it is the practical foundation of any repeatable UV curing process. Defining UV Intensity UV intensity — more precisely called irradiance in radiometric terminology — is the instantaneous power of UV light arriving at the cure surface, expressed in milliwatts per square centimeter (mW/cm²). It is a rate: how fast UV energy is being delivered to the adhesive at any given moment. If a UV LED spot lamp is on and aimed at a bond joint, the irradiance at that joint is the intensity value. Irradiance is determined by the lamp's output power, the optical coupling efficiency of the delivery system, and the working distance between the cure head and the substrate. It does not depend on how long the lamp is on. A lamp operating at 3,000 mW/cm² delivers that irradiance whether it is on for 0.1 seconds or 10 seconds. Defining UV Dose UV dose — also called UV energy or fluence — is the total UV energy received by the adhesive surface over the full exposure period, expressed in millijoules per square centimeter (mJ/cm²). It is calculated as: UV Dose (mJ/cm²) = Irradiance (mW/cm²) × Time (seconds) Dose is cumulative. It accumulates as long as the lamp is on and UV light is reaching the adhesive. A lamp delivering 3,000 mW/cm² for 1 second provides a dose of 3,000 mJ/cm². A lamp delivering 1,500 mW/cm² for 2 seconds also provides 3,000 mJ/cm². Why They Behave Differently in the Curing Process The equation above might suggest that intensity and time are fully interchangeable — that any combination producing the required dose will give the same cure result. For many adhesives, that is approximately true within a moderate range. For others, it is not, and confusing the two parameters leads to real process failures. Intensity-sensitive reactions. Free-radical polymerization depends on generating reactive radical species faster than oxygen scavenging can consume them. If irradiance falls below the adhesive's threshold intensity, oxygen inhibition dominates regardless of exposure time. The adhesive surface remains tacky even after extended exposure, because the initiation rate is never high enough to overcome the inhibition mechanism. Increasing exposure time does not help. The solution is higher irradiance, not longer exposure. Dose-limited through-cure. In thick bondlines or with pigmented adhesives that limit UV penetration, the total energy reaching the interior of the adhesive layer determines how completely the deeper material polymerizes. Once the surface has cured and attenuates incoming light, additional dose delivered over a longer exposure helps drive deeper polymerization, while additional intensity primarily affects the already-saturated surface. These two mechanisms mean that a process optimized only for dose — without verifying that irradiance exceeds the material's threshold —…

When a UV LED curing system specification sheet lists a number in milliwatts per square centimeter, it is describing irradiance — and if you do not understand what that number means in the context of your process, you cannot reliably specify, qualify, or troubleshoot a UV curing system. Irradiance is not just one of several UV curing parameters; it is the parameter that governs how quickly and completely photopolymerization initiates. Irradiance Defined Irradiance is the radiant power delivered to a surface per unit area. In UV curing, it is expressed in milliwatts per square centimeter (mW/cm²) and represents the instantaneous intensity of UV energy striking the adhesive at any given moment during exposure. It is sometimes called UV intensity, though irradiance is the more precise engineering term. Irradiance is a rate measurement, not a quantity measurement. It describes how fast UV energy is being deposited on the cure surface, not how much total energy has been delivered. That distinction separates irradiance from UV dose, which is the cumulative energy (in mJ/cm²) received over the full exposure period. How Irradiance Is Generated In a UV LED spot lamp system, irradiance at the work surface is determined by four factors: the output power of the LED array, the efficiency of the optical coupling system (the light guide and focusing optics), the working distance between the cure head and the substrate, and the area over which the output is distributed. Higher LED drive current increases output power but also increases junction temperature, which reduces LED efficiency and accelerates degradation if thermal management is inadequate. Optical coupling efficiency determines how much of the LED's raw output actually reaches the cure point rather than being scattered or absorbed within the light guide. Working distance has a significant effect — as the cure head is moved farther from the substrate, the same optical power is spread over a larger area, reducing irradiance according to the inverse square law. This means that irradiance is not a fixed property of a curing lamp. It is a value that depends on how the lamp is positioned and configured in the process. Why Irradiance Matters for Polymerization The rate of free-radical initiation — the step that triggers chain polymerization — is proportional to the rate of photon absorption, which is directly proportional to irradiance. Higher irradiance generates more photoinitiator-derived radicals per unit time, which means polymerization initiates faster and proceeds more aggressively. For most UV-curable adhesive formulations, there is a minimum irradiance threshold below which the initiation rate cannot overcome inhibition effects (primarily oxygen inhibition) and the adhesive will not cure properly regardless of how long exposure continues. This threshold varies by adhesive formulation and photoinitiator concentration, but it is a hard lower bound on acceptable irradiance for a given material. Above the threshold, higher irradiance generally produces faster cure speeds and, up to a point, better through-cure as more reactive species are generated throughout the adhesive layer simultaneously. Irradiance vs. Dose: Different Roles in the Cure Irradiance and dose…

A UV-curable adhesive sitting in a dispense tip looks unremarkable — it is a clear, slightly viscous liquid that shows no indication of what it is capable of. Expose it to the right wavelength of ultraviolet light for a fraction of a second, and it transforms into a rigid, cross-linked polymer network strong enough to hold precision components in alignment for the life of the product. Understanding that transformation — from the first photon to the finished polymer — is what separates engineers who troubleshoot curing problems from those who encounter them repeatedly. The Starting Material: UV-Curable Resin UV-curable adhesives are formulated from three primary components: monomers, oligomers, and photoinitiators. Monomers are small, reactive molecules that form the building blocks of the cured polymer. Oligomers are longer pre-polymer chains that give the cured material its bulk mechanical properties — flexibility, hardness, tensile strength, and chemical resistance. Photoinitiators are the light-sensitive trigger molecules that make the entire reaction possible. In its uncured state, the resin is stable at room temperature and in the absence of UV light. The components are designed not to react with each other spontaneously; without activation, the adhesive can sit in a dispense cartridge for months without changing state. Step One: Photon Absorption When UV light from a LED curing lamp strikes the adhesive surface, individual photons penetrate the resin and are absorbed by photoinitiator molecules. The energy of a photon is inversely proportional to its wavelength — shorter wavelengths carry more energy per photon. The photoinitiators in a given adhesive formulation are selected to absorb efficiently at a specific wavelength range, matched to the output of the curing lamp. Absorption is not universal across the resin volume. Near the surface, where irradiance is highest, absorption is rapid. Deeper into the adhesive layer, the resin itself — along with already-reacted material — attenuates the incoming light. This depth-of-cure behavior is one reason that bondline thickness matters in UV curing process design. Step Two: Radical or Cation Generation Once a photoinitiator molecule absorbs a photon, it enters an electronically excited state. This excited state is short-lived and highly reactive. For free-radical photoinitiators — the most common type in UV adhesives — the excited molecule cleaves into two radical fragments. Each fragment carries an unpaired electron, making it extremely reactive with neighboring monomer molecules. Cationic photoinitiators follow a different mechanism: photon absorption generates a strong acid that initiates ring-opening polymerization of epoxy groups. Cationic systems offer advantages in oxygen-inhibited environments and continue to react after UV exposure is removed, but they behave differently from free-radical systems in terms of cure speed and temperature sensitivity. Step Three: Chain Polymerization Free radicals generated by photoinitiator cleavage attack the double bonds in monomer and oligomer molecules, adding them one at a time to a growing polymer chain. This chain-growth process is rapid — a single initiated chain can grow to thousands of repeat units in milliseconds. The reaction propagates until the radical either encounters another radical (termination) or runs out of reactive…