ADVANCED COOLING SIMULATION TECHNOLGIES FOR THE INJECTION MOLDING PROCESS Lu Chen, Clinton Kietzmann*, David Astbury*, Liang Shao Autodesk (China), 399 Pudian Road, Shanghai, China 200122 *Autodesk Australia Pty Ltd, Moldflow R&D Center, 259 -261 Colchester Road, Kilsyth Vic 3137 Abstract Cooling circuit design in plastic injection molding has become the focus for improving part quality and reducing cycle times. In order to achieve both high quality parts and low cycle times; technologies such as, rapid heat cycling, and conformal cooling are commonly used. This paper gives an extensive introduction to a 3D finite element method based solver which has been developed to simulate these molding technologies. Rapid heating and cooling cycling heats the mold surface prior to mold filling using steam, hot water or heater cartridges and cools the mold during the cooling phase with chilled water resulting in a very good surface finish without compromising the cycle time. With conformal cooling, the cooling channels follow the precise geometry of the part in the mold. This aids in creating a uniform temperature distribution across the surface of the part by targeting hot spots. Rapid heating and cooling technology combined with conformal cooling is also supported by this solver. Typical cases for these technologies are presented in the paper and discussed. Introduction Plastic injection molding is one of the most popular manufacturing processes for mass production. In order to obtain cost effective high quality parts consistently, many molders turn to simulation technology for part and mold design. Simulation technology aims to provide the analyst with accurate mold cooling or heating, filling and part warp results to guide their design decisions. Traditional injection molding design aims to maintain the mold at a constant temperature for the entire injection molding cycle. In order to achieve this, coolant is pumped through the mold cooling channels with constant inlet temperatures. Traditionally these cooling lines are comprised of a network of holes drilled through the solid mold that are plugged at various positions forcing the coolant to follow a certain path. If more cooling is required closer to the part in a certain region of the mold the traditional approach is to insert a baffle or a bubbler in this region [1]. Conformal cooling channels are made to any shape that follows the precise geometry of the part in the mold. This aids in creating a uniform temperature distribution in the part by targeting hot spots on the part surface with arbitrary shaped cooling channels in the mold. Ultimately these result in better quality parts, shortened cycle times, reduced waste and cost reductions. Traditional cooling lines are used to supply and remove coolant from this insert containing the conformal cooling channel. These conformal cooling channels replace the conventional cooling lines in the mold and no other change in the injection molding cycle is required. Conformal cooling channels are proving to be very popular when used in conjunction with the Rapid Heating and Cooling injection molding process. Rapid Heating and Cooling varies the inlet temperature of the coolant during the injection molding cycle. The aim is to have a mold cavity surface temperature close to melt temperature during the mold filling stage and to reduce the surface temperature to ejection temperature during the packing and cooling stage of the injection molding cycle. The high mold cavity surface temperature during filling results in high gloss surface finishes of plastic parts, avoiding the need for any other post molding surface enhancements such as polishing and painting. A hotter mold during filling also results in lower injection pressures, allowing the molding of parts with reduced wall thicknesses and the selection of gating locations which reduce mold cost. The hotter mold also reduces the impact of weld lines which improves the strength and aesthetics of the part. The benefits of rapid heating and cooling processes are particularly favorable when molding clear components such as lenses and flat screen television housings among other components. The use of conformal cooling channels can minimize the distance from the cooling channels to the part cavity, so allowing the mold in contact with the part to more quickly heat up and cool down during each cycle. However in order to utilize the full potential of conformal cooling it is very important that the fluid flow dynamics in the conformal cooling channel be understood. Large hollow voids in the mold working as conformal cooling channels may not be ideal for optimum heat removal during cooling or heating for Rapid Heating and Cooling. The fluid will always circulate along the path of least resistance through the conformal channel. Hence if the conformal channel has large variations in cross sectional area it is highly likely that the flow will stagnate in some pockets with very little fluid circulating through those regions. If the fluid is not circulating in a certain area of the mold poor heat transfer will result in this region of the mold. This will lead to uneven cooling or heating of the mold resulting in poor part quality. The most common heating methods considered for simulation are saturated steam, electric cartridge and pressurized hot water heating. Saturated steam is the most effective medium for heating the mold due to the release of latent heat energy when it condenses to water. The heat transfer capacity of saturated steam is much higher than that of pressurized hot water or superheated steam. Saturated steam provides most heat via latent heat release when condensing from a vapor to a liquid. Only saturated steam is considered in the work presented here. Even though saturated steam is the most effective medium for heating the mold, some molders prefer for safety reasons to use hot compressed or pressurized water to heat the mold. Simulation of heating by pressurized water is included in the work presented here. After the part has filled the molding cavity at high cavity surface temperature, the rapid heating and cooling process aims to cool the part down to ejection temperature by using conventional or conformal cooling methods. Usually chilled water is circulated through the channels for a period of time, reducing the cavity surface temperature to a temperature suitable for ejection. On certain parts such as flat screen television housings or automotive interior components where only one side of the part requires a high quality surface finish, only the fixed half of the mold is exposed to the rapid heating and cooling process. The moving half with the side of the part where surface finish is not important can rely on conventional cooling. However for lenses and other optical applications rapid heating and cooling is required in both halves of the mold. Almost all the rapid heating and cooling systems discussed use a closed loop control system where thermocouples are placed in the mold at strategic positions near the cavity to control the commencing and termination of various stages of the cycle. Rapid heating and cooling cycle The rapid heating and cooling cycle differs somewhat to a conventional injection molding cycle. With the closed loop nature of the cycle, it is possible that no two injection molding cycles are ever identical. The heating and cooling stages could turn on and off at inconsistent times during successive cycles. Our simulation of the process supports closed loop control as well as timer controlled processes where each cycle will be identical. The rapid heating and cooling cycle usually begins during the mold open stage just after the previous cycle’s part is ejected. The mold is now in the mold open stage. Saturated steam that is usually controlled by the pressure of the boiler is allowed to fill the rapid heating and cooling channel. Once the channel is filled with steam the channel exit is blocked off and the saturated steam pressure is maintained in the channel for a specified time or until a thermocouple in the mold has reached a required temperature. During this period the steam condenses, releasing its latent heat of condensation to heat the mold. Once the mold has been heated for a specified time or has reached the required temperature, the mold closes and mold filling by injection begins. Usually once the part has filled and packing is about to commence the heating stage is stopped by cutting off the steam supply to the channel. The channel is then purged with compressed air for a short time to expel the remaining steam and condensate from the channel. After this primary air purge the cooling stage of the rapid heating and cooling process commences where chilled coolant is cycled through the rapid heating and cooling channel. The reason for the primary air purge is that “explosive vaporization” may occur if coolant and steam come into contact. This may result in pitting on the surfaces of the channel reducing their heat transfer effectiveness. The cooling stage ends after a specified time or once a thermocouple has reached a required temperature. The part is then ready for ejection. Once the cooling stage has completed a secondary air purge occurs where the channel is cleared of coolant, allowing a clear passage for the steam to enter for the next cycle. These cycles repeat themselves for each part that is manufactured. If heater cartridges are used in the mold the heater cartridges are turned on and off at various times during the cycle. The cooling channels are separate entities and work in conjunction with the heater cartridges. When using conformal cooling channels in the mold it is very important that the flow regime is understood before the mold manufacturing process begins. In order to have a thorough understanding of the fluid dynamics in the conformal cooling channel, the manufacturing process needs to be used in conjunction with simulation. Simulation allows the user to extract the full potential of their investment in their manufacturing technology or process providing them with the consequences of the part and mold design decisions before mold manufacturing begins. Computational Fluid Dynamics (CFD) is a robust technology that uses numerical methods and algorithms to analyze fluid flows by solving the Navier-Stokes equations. Commercial CFD packages have been in existence for many years and are considered to be a robust technology. The benefits of CFD technology can be leveraged to design optimum conformal cooling channels for plastic injection molds. In order to get the full benefit of CFD for conformal cooling the CFD solver needs to be customized to integrate it with plastic injection molding simulation technology requirements. Simulation technology The transient mold cooling module that has been developed to support 3-D tetrahedral meshes of the mold is used for simulating conformal cooling and rapid heating and cooling. [2]. In order to simulate the flow dynamics in the conformal cooling channels an existing CFD solver was used to provide the flow and temperature solutions in 3-D conformal cooling channels [2]. Conformal cooling channels can also be represented by several (1-D) channels following the contour of the part closely. These representations do not require the CFD solver for simulation and a (1-D) solution is preferable in such channels due to the complexity of the CFD solutions. A rapid heating and cooling boundary condition can be specified on a conformal or conventional cooling channel, in order to simulate rapid heating and cooling. The purpose of this paper is to present the conformal and rapid heating and cooling capabilities of the transient mold cooling solver. Conformal cooling and rapid heating and cooling analyses are performed on both arbitrary shaped 3-D cooling channels and conventional cooling channels in the mold. Conformal cooling The incorporation and application of the CFD solver in the transient mold cooling module is discussed. The capabilities of the conformal cooling solver are demonstrated on a fully 3-D conformal cooling channel. Only CAD bodies are considered for conformal cooling geometries to be analyzed with the CFD solution. If a 3-D CFD solution is desired on 1-D geometry then the geometry needs to be modeled in 3-D in CAD. The CFD solver used for simulating the fluid flow in the conformal cooling channel is a finite element based solver requiring tetrahedral element meshes in the solution domain [2]. The tetrahedral element mesh requires special treatment relating to the geometry of the channel, hence a standard tetrahedral element mesh cannot be used. The CFD software package’s mesher places enhancement layers close to the boundary wall of the channel and allows the user the option of specifying the number of enhancement layers. Enhancement layers should not be placed on the inlet and outlet surfaces of the conformal cooling channel. In order to guarantee this, the user must specify the inlet and outlet faces on the CAD body prior to meshing. The mesher then meshes the body appropriately and the enhancement layers are clearly visible on these inlet and exit regions. The CFD solution is sensitive to the mesh density. Solution accuracy is proportional to mesh density; however the analysis time also increases with a finer mesh. Various other mesh options are also supported allowing more complex flow phenomena such as recirculation zones to be captured if needed. The CFD solver has been fully integrated into the previously developed transient cooling module Error! Reference source not found. and the combined operation is fully automated. The CFD pressure and flow velocity solution is a steady state solution, as is used for the 1-D coolant solution. The CFD temperature solution in the conformal cooling channels is a transient solution and is solved in conjunction with the mold and part temperature solutions. The cooling channel wall temperature is constantly updated by the mold temperature solution which is used as the boundary condition for the transient CFD temperature analysis of the coolant. The transient CFD temperature solution provides the transient mold temperature solution with a transient convection boundary condition. Once the transient coolant, mold and part temperature solutions have converged for a particular time step the computation is advanced to the next time step until the entire cycle time is completed. The velocity plot of the fluid in the conformal cooling channel needs to be viewed with a cutting plane due to there being a zero velocity boundary condition on the channel wall. The velocity vectors can be shown as darts with the magnitude shown by the color. The velocity can also be shown as a streamline plot. A heat flux plot also shows the heat transfer between the fluid in the conformal cooling channel and the mold. The pressure of the fluid in the conformal channel can also be shown. When viewing the velocity plot in conjunction with the temperature plot the correlation between the temperature on the surface of the conformal cooling channel and the flow inside the channel is evident. The velocity plot is used to identify areas of flow stagnation. The temperature and heat flux plot can therefore be used to guide design changes to the mold. The solver uses a zero outlet pressure boundary condition in the solution. Hence the calculated inlet pressure is equivalent to the pressure drop along the cooling circuit. The inlet temperature is also specified as a boundary condition and the outlet temperature is calculated by the CFD solver. Rapid Heating and Cooling A rapid heating and cooling inlet can be specified on both 1-D channels or on the inlet face of the conformal cooling channel. This inlet boundary condition gives access to specify the rapid heating and cooling cycle process information. The solver supports both steam and hot water heating and cooling fluids. When considering rapid heating, the condensation of steam in the cooling channels is modeled taking the latent heat into account. To calculate the latent heat of condensation during simulation, saturated steam tables are used. [8] Appropriate, well known, film-wise condensation formulations were applied to obtain the heat transfer coefficient for each time step during the steam heating phase. [9] As the steam condenses the changing quality of the steam, which is the ratio of vapor mass to total mass, is also considered. In order to model the cooling stage in the rapid heating and cooling solver the boundary conditions specified on the rapid heating and cooling node are used. The process settings dialog was modified for rapid heating and cooling. A new “mold close time before injection” option has been added. This time represents the time duration after the mold has closed and before the commencement of the next injection cycle. In some rapid heating and cooling cases the mold is heated up whilst awaiting injection in this mold close position. When temperature control is selected the mold may remain in this state whilst awaiting a trigger signal from a thermocouple somewhere in the mold before injection will commence. On each rapid heating and cooling boundary condition node the user can select “Time controlled” or “Temperature controlled” boundary conditions for the steam heating and cooling of the rapid heating and cooling channel. The “Time controlled” option allows the user to set the stages as fixed times during the cycle and the solution should converge to identical cycles. The “Temperature controlled” option allows the user to set a threshold temperature on any node in the mold that will stop the heating or cooling when the node reaches this temperature. When using this option the mold may require a long time to reach the specified temperature in the cycle and this may alter the specified cycle time. The user is given the choice of “Extend mold open time”, “Extend mold close time before injection” or “Do not delay injection”. If the mold is kept open during rapid heating by using the “Extend mold open time” option, heat will be lost through the parting plane via air convection to the surroundings. If the mold is kept closed by using the “Extend mold close time before injection” option, heat conduction would take place through the closed parting plane to the opposing mold half during the rapid heating stage. Depending upon the thermocouple settings this heat transfer could be significant. Hence, the user has the option of setting the mold position during this delay. Each mold component can be specified as belonging to the fixed or moving mold half. If the user chooses to use heater cartridges for the rapid heating of the mold, three new heater control options are available: The options are “Time”, “Thermocouple” and “Time with Target Temperature”. The “Time” option allows the user to turn on the heater cartridge at a specified time late in the cycle and to turn it off early in the next cycle, preferably just after filling. The “Thermocouple” option allows the user to specify a thermocouple node with two temperatures representing the switch on and switch off temperatures with accompanying delay times. When the node reaches these temperatures the heater will behave accordingly. “Time with Target Temperature” allows the user to specify times in the cycle when the heater cartridge will turn on or off together with a node on which the temperature target is specified which will trigger the heater to turn off. This can lead to cycle time extension occurring as a result of the thermocouple not reaching the required temperature within the specified cycle time. The same options for extending the cycle time are available to the user, namely “Extend mold open time”, “Extend mold close time before injection” or “Do not delay injection”. These options have the same meaning as for steam heating. Similar results are provided from the conformal cooling rapid heating and cooling solver as are provided from the 1-D channel rapid heating and cooling solver. Results and Discussion By referring to [10] it can be seen that the conformal cooling channel results match those obtained from the 1-D solution very closely. The real benefits of the 3-D CFD solution become evident when arbitrary shaped conformal cooling channels need to be analyzed where the 1-D solution cannot be used for these geometries. Figure 1 shows the conformal cooling channels which may be used in a mold used for manufacturing satellite dishes. The conformal cooling channels follow the contour of the part as closely as possible with solid mold sections obstructing the flow where either the feed system or ejector pins are placed. These obstructions have an effect on the flow pattern, which in turn has an effect on the coolant temperature distribution in the cooling channel. The temperature distribution then influences the heat transfer in the mold. Figure 3: Coolant temperatures in the lower channel. Figure 4: Heat flux at mold-coolant interface. Figure 1: Satellite dish model with conformal channels. Figure 2: Streamline plot of velocity in lower channel. Figure 2 shows the streamline plot of the velocity distribution in the lower conformal cooling channel. Streamlines close together signify a higher flow rate though these regions, which means that the velocity is also generally higher. This is confirmed by the color of the streamlines. It can be seen that at the entrance of the conformal cooling channel, on the left of the plot, a large recirculation zone exists, while behind all the obstructions the velocities are very low and streamlines are absent. By looking at Figure 3, which shows the coolant temperature in the lower conformal cooling channel, it can be seen that where the velocity is high the coolant temperature is low and vice versa. The coolant temperature is approximately 30C hotter behind the obstruction than at the inlet of the conformal cooling channel. Figure 4, showing the plot of the heat flux between the conformal cooling channel and the mold, shows that where the coolant stagnates there is very little heat transfer between the coolant and the mold. In the regions where the velocity is high there is much better heat transfer. Figures 2, 3 and 4 show that proper simulation of the fluid flow and heat transfer in the conformal cooling channel is vital in designing an appropriate conformal cooling system for the mold. Simulation can help the mold designer refine the design to create optimum cooling conditions. Without simulation a designer may arrive at a very complex and expensive mold design that will have very poor heat dissipation. To demonstrate the rapid heating and cooling, the component presented in Figure 5 is molded using rapid heating and cooling technology. The fixed side of the mold, the side with the feed system, is heated using the rapid heating and cooling channel shown close to the surface of the part. The moving half of the mold uses 4 conventional cooling channels using water set at 30 C flowing with a Reynolds number of 10000. Figure 6: Sensor node on mold in contact with the part. Figure 5: Rapid Heating and Cooling part and mold. The rapid heating and cooling boundary conditions are specified on the rapid heating and cooling boundary condition node as shown in Figure 5. This case uses the “Time controlled” option for rapid heating and cooling. As the mold opens for part ejection the rapid heating and cooling begins with a 2 second air purge to remove all the excess coolant in the channels. This air purge time corresponds to a 2 second mold open time set in the process settings. After the air purge, the channel is heated with saturated steam at 10 bar pressure for 15 seconds. The 15 seconds corresponds to the mold-close time before injection in the process settings. After the steam heating has finished, the filling process occurs during which the cavity is filled with polymer and the cavity surface is at its hottest. The start of filling also corresponds to the beginning of the primary air purge where the cooling channels are cleared of excess steam and condensate from the steam heating phase. After the primary air purge has completed the rapid heating and cooling channel is cooled down with chilled water set at 25 C for 13 seconds flowing with a Reynolds number of 10000. Figure 7 shows the temperature change of that node during the injection molding cycle. It can be seen from Figure 7 that at the time of injection the surface temperature of the mold is at 135.4 C and is still heating up even though the rapid heating and cooling channel is being purged with air. This phenomena is called “thermal inertia” when the effects of the steam heating are still being transmitted through the mold whilst the steam heating has ended. The surface reaches a maximum temperature of 143.6 C after 2 seconds which corresponds to the start of the cooling phase in the rapid heating and cooling channel. During the cooling phase chilled water is circulated through the cooling channel and it can be seen that the surface temperature decreases to 111.6 C after 18.8 seconds which corresponds to the end of the mold open time, which is also the end of the secondary air purge. This temperature is as expected. After 18.0 seconds the mold surface starts to heat up again very quickly. This corresponds to the steam heating phase of the next cycle and is as expected. At the end of the cycle the temperature has reached 135.4 C again which corresponds to the temperature at the start of the cycle. To see the effect of the rapid heating and cooling cycling on the surface of the mold in contact with the part, a sensor node N1930 (see Figure 6) is chosen to monitor the temperature change during the cycle. Figure 7: Temperature plot of sensor node in the mold. Figure 8 shows the temperature change of the fluid (steam, air or coolant) in the rapid heating and cooling channel. For this model very low pressure air was used to purge the channel. By looking at the temperature trace for the inlet element B89, it can be seen that air enters the channel at 25 C. It can also be seen that the air heats up as it cycles through the channel by looking at the mid channel element B64 and the exit element B76. After 2 seconds the air purge is completed and the cooling cycle begins. It can be seen that the temperature rise of the coolant across the cycle is significant. At the end of the coolant cycling the inlet temperature of the coolant is 25 C and the exit temperature is 38.2 C. This 13.2 degree temperature variation is a large rise indicating that a large amount of heat is removed from the mold during this phase. After 15 seconds the cooling phase is stopped and the primary air purge begins. It can be seen that the air heats up during this stage. After 17 seconds the steam heating phase begins. For this model the saturated steam is set to a pressure of 10bar in the boiler which, from steam tables, corresponds to a saturation temperature of 179.9 C. The temperature of the steam remains at this temperature as it condenses, heating the mold with the latent heat of condensation. Figure 8: Time dependent temperature plot of fluid in rapid heating and cooling channel. Figure 9 is a plot showing the surface temperature of the rapid heating and cooling channel that is in contact with the steam, air or coolant. It can be seen that at the end of the steam heating cycle the temperatures are around 150 C which are the hottest during the cycle. During the air purge the temperature reduces on the channels. However, after 2 seconds the coolant starts flowing in the circuit and the surface temperature decreases significantly very quickly. The inlet element B89 cools to 80.78 C and the exit element B76 cools to 88.22 C during the cooling stage. The mid channel element B64’s temperatures are midway between the inlet and exit elements temperature’s which is as expected. After 15 seconds the primary air purge begins and the temperature starts to rise again, as air does not remove heat as well as the coolant. Once the primary air purge is complete, the steam heating begins and the surface temperature of channel heats up quickly to 150 C. This is as expected. Figure 9: Time dependent temperature plot of the rapid heating and cooling channel surface. Figure 10 shows the mold cavity temperature in contact with the part at the time of the flow front arrival. This result is a Flow solver result which takes advantage of the transient mold temperature solution. Figure 10 shows both the top of the part temperature exposed to the rapid heating and cooling channel as well as the part temperature on the other side that is exposed to conventional cooling. By looking at these temperatures it can be seen that the top part temperature is much higher than the bottom temperature. This would be desirable if the user would prefer a better surface finish on the top of the part. However, the temperature distribution is not very uniform across the top surface which may necessitate a mold re-design so that the rapid heating and cooling channel can be a consistent distance from the part. Subsequent warp analysis to predict the final part shape as a consequence of these uneven cavity surface temperatures is also possible. Figure 10 is the most useful plot for a part and mold designer as the ultimate goal of rapid heating and cooling is to obtain a mold surface temperature as hot as possible during the filling stage. Figure 10 provides the user with this information. Figure 10: Flow front temperature of the top and bottom of the mold cavity. Conclusions The conformal cooling functionality added to the transient cool simulation is a worthwhile enhancement to the existing simulation technology when simulating conformal cooling channels that follow the contour of the part closely. Previous work has shown that the results from the conformal cooling solver match those from the 1-D solution very well. Rapid Heating and cooling functionality can also be used with conformal cooling and the numerical results obtained from these simulations agree with observations made from actual processes. References [1]. Hofmann tool innovation.com. manufacturing, www.hofmann- Error! Reference source not found.. C. Kietzmann, L Chen, H Lin-Feng, F. Costa, Rapid Heating and Cooling Simulation for the Injection Molding Process, SPE ANTEC Proceedings, Orlando (2012). Error! Reference source not found.. Peter Kennedy, Flow Analysis of Injection Molds, Hanser New York, (1995) Error! Reference source not found.. K. Talwar, F Costa, V Rajuplaem, L. Antanovski and C Friedl, Three Dimensional Simulation of Plastic Injection Molding, SPE ANTEC Proceedings, 1. 563566(1998). Error! Reference source not found.. M. Rezayat and T.E Burton, A Boundary-integral Formulation for Complex Three-dimensional Geometries, International Journal for Numerical Methods in Engineering, Wiley, Vol. 29, No 2, 223-452(1990). Error! Reference source not found.. C. Kietzmann, L Chen, H Lin-Feng, F. Costa, R Le Goff, Transient Mold Cooling Simulation for the Injection Molding Process, SPE ANTEC Proceedings, Boston(2011). [2]. Schnipke, R.J, Streamline upwind finite-element method for laminar and turbulent flow, Thesis, Virginia Univ., Charlottesville (USA), 1986 Jan 01. [8]. International Association for the properties of Water and Steam, IAPWS-IF97, available at www.iapws.org (August 2007) [9]. Rohsenow, W.M, Film Condensation, chap 12 in "Handbook of Heat Transfer,” McGraw-Hill Book Company, New York, 1973 [10].C. Kietzmann, L. Chen, F. Costa, Conformal Cooling Simulation for the Plastic Injection Molding Process, SPE ANTEC Proceedings, Cincinnati(2013) Key Words: Injection molding, Autodesk, transient cool, simulation, conformal cooling, CFD