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The Effect of Different Curing Methods on Tack-Free Curing

By Amelia Davenport, Mike Idacavage and Neil Cramer

Colorado Photopolymer Solutions








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From coatings to biomedical implants to photolithographically controlled materials, photopolymerization has dramatic advantages. It can be utilized for in situ cure materials at whatever time, location and three-dimensional pattern desired. It is one of the most energy-efficient processes known and can be used as a 100% solvent-free process. One drawback that must be overcome in most photopolymerization applications is the severe inhibition of these polymerizations by the ubiquitous presence of oxygen. As such, different UV-curable formulations must be optimized to contain an appropriate initiator package and cure with a UV source to overcome oxygen inhibition, which adds cost and development time.

The advent of LED has enabled less expensive lights with increased operating lifetimes and improved energy efficiency. However, rather than covering a broad spectrum of wavelengths, LEDs emit in narrow bands of light. The narrow wavelength emission spectrum of LED lights will inevitably influence both curing rates and oxygen inhibition. An alternate form of curing, electron beam (EB) has some distinct advantages over UV curing but also is known to exhibit problems resulting from oxygen inhibition. In this study, we evaluate the use of broadband mercury, 385 nm LED, and electron beam curing across a range of different acrylic formulations. The different methods of curing are compared by examining their effect on oxygen inhibition, cure speed and material properties.

No matter the type of irradiation source, oxygen inhibits the cure of acrylates by diffusing into the coating and creating radicals that react much more slowly than other radicals, thereby inhibiting the polymerization. This process is shown in Figure 1. When the rate of oxygen diffusing into the coating is greater than the rate of initiation, oxygen inhibition can’t be overcome. When the rate of initiation is greater than the flux of oxygen into the system, tack-free curing can be achieved, provided exposure times are long enough (Equation 1).

Parameters that influence the flux of oxygen are the polymerization rate, viscosity of the resin and cross-link density of the formulation. Parameters that influence the rate of initiation are the irradiation intensity, the photoinitiator concentration and the overlap of the emission and absorption spectrums, respectively. Figure 2 shows the emission of a typical “H” bulb and the absorption of CPK.

Numerous routes to overcome oxygen inhibition are commonly utilized, including high irradiation intensity, high photoinitiator concentration, nitrogen purging and chemical additives, such as thiol monomers. Generally, the routes to overcome oxygen inhibition with typical high intensity mercury broadband UV lamps are well established. With LED curing gaining prevalence throughout the UV curing industry, examining the effectiveness of these known routes to overcome oxygen inhibition and comparing to broadband UV is important to understand. In this work, we compare methods to overcome oxygen inhibition using a typical broadband mercury irradiation source as well as a 385 nm LED light. We also evaluate curing with electron beam irradiation.

Materials and testing

Monomers utilized in this study include epoxy diacrylate (PE230), polyester triacrylate (PS3220), urethane diacrylate (PU2100), tripropylene glycol diacrylate (TPGDA) and isobornyl acrylate (IBOA). CPS 1020 and CPS 1040 are proprietary thiol-ene based formulations. The photoinitiators utilized were 1-hydroxycyclohexyl-phenyl ketone (CPK/Omnirad 481) and 2,4,6-trimethylbenzoyl-diphenyl phosphine oxide (Omnirad TPO).

Coating: Substrates are coated with an ~125 µm layer of formulation using a wire wound drawdown bar.

Curing: Formulations were cured on a conveyor system using a Heraeus F300 light with 300 W/inch H bulb or a 25 W 385 nm LED. Formulations that took more than one pass are denoted as 9x2 or 9x3 for two (or three passes) at 9 fpm.

Tack-free determination: A fresh latex glove is pressed against the surface of the polymer with moderate pressure. If the polymer is marred in any way, the surface is tacky. If there is no surface marring, and no residue is observed on the glove, then the surface is considered tack free.

Results and discussion

A study of the effect of photoinitiator concentration is shown in Table 1 for the epoxy diacrylate system mixed 50/50 with TPGDA. Here, the results show a significant increase in the maximum belt speed that can achieve tack-free curing when the photoinitiator concentration is increased from 4 to 6 wt.%. Beyond 6 wt.% photoinitiator, tack-free curing is achieved with the maximum belt speed of 155 fpm. When cured with the LED light, tack free curing was not achievable in the system with 4 wt.% photoinitiator. The results show a significant decrease in cure time when the photoinitiator concentration is increased from 6 to 8 wt.%.

A comparison of tack-free curing with a typical epoxy diacrylate, polyester triacrylate and urethane diacrylate was performed. Each of the acrylates was cured with 1, 2 and 4 wt.% photoinitiator. The results shown in Table 2 indicated no significant difference in curing performance across these materials, despite the various viscosities and cross-link densities. Experiments were performed with broadband UV irradiation using a UV photoinitiator (CPK). Experiments were also performed with the 385 nm LED as well as with TPO as the photoinitiator. Belt speeds for tack-free curing ranged from 70 to 150 fpm with 2 and 4 wt.% photoinitiator for UV broadband irradiation. Using TPO and a 385 nm LED system, belt speeds for tack-free curing ranged from 9 to 20 fpm using 2 and 4 wt.% photoinitiator.

The high viscosity trifunctional acrylate was able to achieve tack-free cure with 1 wt.% photoinitiator when cured continuously for 60s. Curing was also performed with a 405 nm LED system, similar in power to the 385 nm LED. Minimal differences were observed between curing performance with the 385 and 405 nm LEDs.

The pure acrylate systems were compared to different thiol-ene based formulations. As seen in Table 3, the thiol-ene based formulations all cured tack-free with 1 wt.% photoinitiator and with belt speeds at 130 fpm, whereas the acrylate systems (Table 2) which are much thicker, cured at a maximum belt speed of only 20 fpm with 1 wt.% photoinitiator in all cases. At 4 wt.% photoinitiator, the thiol-ene systems achieved tack-free curing at belt speeds of greater than 155 fpm (155 fpm is the maximum belt speed for the system utilized in this study), compared to belt speeds ranging from 135 to 155 fpm for the diacrylate systems. Using 4 wt.% TPO as the photoinitiator and the 385 nm LED, the thiol-ene systems exhibited tack-free curing with belt speeds of 100 to 155 fpm.

A thiol was added to the acrylate formulations with CPK as the photoinitiator and cured using the UV broadband bulb. The belt speeds needed for tack-free cure increased dramatically with the addition. The comparison can be seen in Table 4. Cure speeds originally near 10 fpm increased to 80 to 90 fpm. Using 1 wt.% TPO and a 385 nm LED system, systems that originally couldn’t reach tack-free cure were then able to cure tack free at slow belt speeds.

The epoxy diacrylate system was evaluated as a 50/50 mixture with two different diluents – TPGDA and IBOA (Table 5). TPGDA is a low viscosity diacrylate that results in a significant drop in viscosity, but maintains high modulus and cross-link density. IBOA is a low-viscosity monoacrylate that results in a significant drop in viscosity, maintains high modulus, but results in significantly reduced cross-link density. Final viscosities after the diluent were approximately 500 cPs. The results show that tack-free curing is most difficult to achieve in the system diluted with IBOA, and less difficult with TPGDA. Due to the reduced viscosity, the system diluted with TPGDA showed more difficulty achieving tack-free curing than the base system with higher viscosity. When cured with the LED light, only the epoxy diacrylate system was able to achieve tack-free curing.

Electron beam curing also was evaluated for the urethane diacrylate system in bulk and diluted 50/50 with TPGDA and IBOA (Table 6). Electrons are accelerated through a thin foil window, impinging on a moving web at atmospheric pressure. The accelerated electrons will ionize most organic materials, with this ionization leading to the formation of free radicals, which initiate polymerization of the coating without the need for added photoinitiators in radical cured systems. The EB parameters are typically set by selecting the total dose of energy delivered to the sample and the belt speed. The current is then adjusted as needed to deliver the total dose with the given belt speed.

When curing with EB, the resins are typically purged with nitrogen to remove the presence of oxygen. EB curing has not been studied nearly as much as UV curing. Though the initiation mechanism to generate radicals is different, the fundamental polymerization kinetics should follow the same principles.

For EB curing, decreasing viscosity had no effect on curing, as seen in Table 6. Viscosities were decreased to approximately 3,400 cPs). This is contrary to UV cured systems under ambient conditions, where the effects of oxygen inhibition are more pronounced in systems with lower viscosity. Decreasing cross-linking reduces cure speed. This result is similar to UV cured systems. Polymerizations were also performed without a nitrogen blanket. Here it was found that the typical diacrylate systems were not able to achieve tack-free curing. However, the CPS 1040 thiol-ene system was readily able to achieve tack-free curing without the aid of a nitrogen blanket.

Conclusions

Several typical acrylate systems were cured with both UV broadband Mercury irradiation sources as well as LED systems. The results indicated that curing with broadband sources was more rapid than curing with LEDs. The LED systems emit significantly less energy than the broadband sources, so the reduced cure speed is not necessarily a result of reduced initiation efficiency. It was demonstrated that reducing viscosity and cross-link density both increase the effects of oxygen inhibition and increase the curing time required to achieve tack-free surfaces.

The use of thiol-ene based formulations was shown to significantly increase cure speed with both UV broadband and LED systems. In fact, the use of thiol-ene systems resulted in cure speeds with LED systems that were equivalent to those achieved in acrylate systems with UV broadband. An initiator optimization study was performed and indicated that, upon achieving a certain threshold initiation rate, cure times decreased dramatically. Systems cured with EB showed the same fundamental cure characteristics as UV cured systems.

The authors would like to address a few points about how each route influences the bulk properties of the cured coating. Increasing the photoinitiator concentration will increase the rate of termination, which will lead to a decrease in the cross-link density of the polymer which, in turn, could make the material more brittle or soften the coating because of the shorter chains. While increasing the photoinitiator concentration will improve the cure at the air interface, the bulk of the material may not receive enough energy to cure well, due to the strong absorption of the photoinitiator. The worst cases may exhibit an uncured portion in contact with the substrate. Balancing the speed of cure, cure depth and material properties can be quite challenging.

Colorado Photopolymer Solutions (CPS) was founded in 2005 by a team of photo polymerization experts. The mission of CPS is to provide high-quality materials and technology development in all areas of photo polymerization. CPS specializes in custom formulation and materials development, consulting, characterization and manufacturing. For more information, visit www.cpspolymers.com.