# Design and Analysis of Fused Deposition Modeling 3D Printer Nozzle for Color Mixing

Authors: Shanling Han; Yu Xiao; Tao Qi; Zhiyong Li; Qingliang Zeng
Journal: Advances in Materials Science and Engineering
 (2017)

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## Abstract

Fused deposition modeling (FDM) has been one of the most widely used rapid prototyping (RP) technologies leading to the increase in market attention. Obviously it is desirable to print 3D objects; however, existing FDM printers are restricted to printing only monochrome objects because of the entry-level nozzle structure, and literature on the topic is also sparse. In this paper, the CAD model of the nozzle is established first by UG (Unigraphics NX) software to show the structure of fused deposition modeling 3D printer nozzle for color mixing. Second, the flow channel model of the nozzle is extracted and simplified. Then, the CAD and finite element model are established by UG and ICEM CFD software, respectively, to prepare for the simulation. The flow field is simulated by Fluent software. The nozzle’s suitable temperature at different extrusion speeds is obtained, and the reason for the blockage at the intersection of the heating block is revealed. Finally, test verification of the nozzle is performed, which can produce mixed-color artifacts stably.


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## Body

## 1. Introduction

3D printing technology’s areas include advanced materials manufacturing, software engineering, and control technology. This is a work of making three-dimensional solid objects from digital files [1–5]. Therefore, an increasing number of people consider that the future of 3D printing will usher in the next industrial revolution [6–10]. Most printing nozzle devices are currently based on 3D desktop FDM printers that can print using only monochrome filaments, which restrict the application of 3D printers [11–13]. So it is necessary to carry out research of color mixing printing.Reiner et al. [14] detailed a method that produces continuous tone imagery by using the two color heads of entry-level fused deposition modeling 3D printers. Arikan et al. [15] described a whole color-managed 3D printing workflow and paid attention to the measurement of colors of highly translucent printing materials later. Khalil et al. [16], from Drexel University independently developed a multinozzle biopolymer deposition system that consisted of four micronozzles: pneumatic microvalve, piezoelectric nozzle, solenoid valve, and precision extrusion deposition nozzle. Each nozzle system can work separately or simultaneously as required.In this paper, the design of a 3D printer nozzle for color mixing is completed by UG software where the flow channel model of the entire device is extracted and simplified. Optimal filament feed speed at different temperatures is studied through computer simulations which is supported by experiment later. The study of the distribution of the pressure field and the velocity field at the nozzle hole and the intersection is built on the combination of the temperature field and filament feed speed. The shortcomings of the device are analyzed and summarized.


## 2. Design of FDM 3D Printer Nozzle for Color Mixing

### 2.1. Establishment of the Heating Block Model

The heating block of a 3D printer nozzle device is usually set through throat pipe in the fixed block which is driven by a motor in the guide rail to realize the function of continuous print [17–19]. In order to ensure the mixing of filaments in the heating block, a larger heating block cavity is needed to meet the actual requirements. As a consequence, the size of the existing heating block is increased to ensure the smooth input of two kinds of filaments. In addition, the face of the throat threaded hole is designed to be at an angle of 30° to the horizontal position, which is not only conducive to the handling of the pipe, but also conducive to the heat dissipation of throat pipe. This design results in the loss of the function of the throat pipe connecting with the fixed block and the heating block. As a consequence, two threaded holes are arranged on one side of the heating block to connect the fixed block using a hex socket screw. The length of the heating block is 32 mm, the width of the bottom and the top is 22 mm and 6.5 mm, respectively, and the height is 20 mm. The heating block is as shown in Figure 1.Figure 1
Model of the heating block.


### 2.2. Establishment of the Whole Model

The nozzle device of the 3D printer is mainly composed of a fixed block, heating block, throat pipes, and nozzle [20–23]. The heating block consists of a throat pipe thread hole, nozzle thread hole, heating pipe hole, and thermistor hole. The nozzle, throat pipe, and thermistor are attached to a heating block using screw threads. The heating pipe is arranged in the heating pipe hole directly. The heating pipe is fastened into the threaded hole using screws. However, the throat pipe will be out of the function of connecting with the fixed block and the heating block after the completion of device design. As a consequence, two screw holes are set where the fixed block and the heating block occur. The heating block is installed into the fixed block by using a hex socket screw. The assembling simulation of the 3D printer nozzle model is done by UG software. The throat is installed into the pipe thread hole of the heating block; meanwhile, the nozzle is fastened into the nozzle thread hole of the heating block. It can be seen from Figure 2 that the heating block and thermistors are omitted. The assembly structure of the whole model is shown in Figure 2.Figure 2
Assembly structure of the entire model.


### 2.3. Simplification of Each Component of the Nozzle for Color Mixing

Finite element analysis is a numerical method that offers a means to find the approximate solution. The finite element analysis of structures requires the use of accurate and reliable finite element models, of equal importance, and the use of efficient finite element method and accurate calculating time. It is misunderstood that the more complex the models are, the more accurate the result will be. So the simplification of the model plays an important role in the finite element analysis. Reasonable simplification of the model can not only improve the efficiency of simulation and shorten the calculation time but also improve the accuracy of the calculation. Simplification mainly focuses on the processing of the models of the heating block, nozzle, and throat pipe. Therefore, the fixed block, hex socket screw, and other components are removed. The simplified heating block model, the simplified nozzle model, and the simplified throat pipe model are shown in Figure3.Figure 3
Simplified model of (a) heating block, (b) nozzle, and (c) throat pipe.
(a)
(b)
(c)


## 2.1. Establishment of the Heating Block Model

The heating block of a 3D printer nozzle device is usually set through throat pipe in the fixed block which is driven by a motor in the guide rail to realize the function of continuous print [17–19]. In order to ensure the mixing of filaments in the heating block, a larger heating block cavity is needed to meet the actual requirements. As a consequence, the size of the existing heating block is increased to ensure the smooth input of two kinds of filaments. In addition, the face of the throat threaded hole is designed to be at an angle of 30° to the horizontal position, which is not only conducive to the handling of the pipe, but also conducive to the heat dissipation of throat pipe. This design results in the loss of the function of the throat pipe connecting with the fixed block and the heating block. As a consequence, two threaded holes are arranged on one side of the heating block to connect the fixed block using a hex socket screw. The length of the heating block is 32 mm, the width of the bottom and the top is 22 mm and 6.5 mm, respectively, and the height is 20 mm. The heating block is as shown in Figure 1.Figure 1
Model of the heating block.


## 2.2. Establishment of the Whole Model

The nozzle device of the 3D printer is mainly composed of a fixed block, heating block, throat pipes, and nozzle [20–23]. The heating block consists of a throat pipe thread hole, nozzle thread hole, heating pipe hole, and thermistor hole. The nozzle, throat pipe, and thermistor are attached to a heating block using screw threads. The heating pipe is arranged in the heating pipe hole directly. The heating pipe is fastened into the threaded hole using screws. However, the throat pipe will be out of the function of connecting with the fixed block and the heating block after the completion of device design. As a consequence, two screw holes are set where the fixed block and the heating block occur. The heating block is installed into the fixed block by using a hex socket screw. The assembling simulation of the 3D printer nozzle model is done by UG software. The throat is installed into the pipe thread hole of the heating block; meanwhile, the nozzle is fastened into the nozzle thread hole of the heating block. It can be seen from Figure 2 that the heating block and thermistors are omitted. The assembly structure of the whole model is shown in Figure 2.Figure 2
Assembly structure of the entire model.


## 2.3. Simplification of Each Component of the Nozzle for Color Mixing

Finite element analysis is a numerical method that offers a means to find the approximate solution. The finite element analysis of structures requires the use of accurate and reliable finite element models, of equal importance, and the use of efficient finite element method and accurate calculating time. It is misunderstood that the more complex the models are, the more accurate the result will be. So the simplification of the model plays an important role in the finite element analysis. Reasonable simplification of the model can not only improve the efficiency of simulation and shorten the calculation time but also improve the accuracy of the calculation. Simplification mainly focuses on the processing of the models of the heating block, nozzle, and throat pipe. Therefore, the fixed block, hex socket screw, and other components are removed. The simplified heating block model, the simplified nozzle model, and the simplified throat pipe model are shown in Figure3.Figure 3
Simplified model of (a) heating block, (b) nozzle, and (c) throat pipe.
(a)
(b)
(c)


## 3. Flow Field Simulation Analysis of ABS Material in Printer Nozzle for Color Mixing

### 3.1. Establishment of the Flow Channel Model

In the previous chapter, the model of the 3D printer nozzle for color mixing has been simplified. The flow channel model of the entire mixing device, established by using UG software, is currently extracted and simplified. The parameters of a simplified flow channel model are presented in Table1. The model which will be imported into ICEM CFD meshing software is established by UG. In order to improve the quality of mesh, a Tetra/Mixed meshing type (which is mainly composed of tetrahedral mesh elements) is chosen to mesh the model. As a result, 4936 nodes and 27442 elements are generated. The first entrance, the second entrance, export, and wall are all defined in ICEM CFD software. The finite element model is imported into the Fluent software to carry out fluid analysis. Flow channel model and finite element model of the flow channel are shown in Figure 4.Table 1
Size of the simplified flow channel.
Item
Quantity
Branch pipe length (mm)
10
Main pipe length (mm)
11
Branch pipe angle (°)
60°
Branch pipe diameter (mm)
1.75
Main pipe diameter (mm)
2
Outlet diameter (mm)
0.4Figure 4
(a) 3D model and (b) finite element model of the flow channel.
(a)
(b)


### 3.2. Material Properties of ABS Material and Setting of Model Boundary Conditions

ABS material is one of the most widely used polymers in the world, touching virtually every part of our lives [24]. ABS materials are an excellent choice for models, prototypes, patterns, tools, and end-use parts. Much stronger than the FDM materials just a few years ago, ABS for FDM machines offers greater tensile, impact, and flexural strength today [25]. The ABS material existing in the flow channel is selected as the research object; meanwhile the situation of ABS mixing in the molten state is studied. Thus, the optimum combination of the different filament feed speed and the corresponding heating temperature is summarized. Properties of ABS material are shown in Table 2.Table 2
Properties of ABS material.
Item
Quantity
Density (kg/m3)
1020
Elastic modulus (GPa)
2
Poisson ratio
0.394
Specific heat capacity (J/(kg·K))
1386
Thermal conductivity (W/(m·K))
0.2256
Viscosity (Pa·s)
84The boundary conditions are set based on the simplified flow channel model. The boundary conditions are shown in Figure5. Both the first inlet and second inlet are set to the speed boundary. The material is ABS filament at a diameter of 1.75 mm. The initial temperature of ABS filament is set to 25°C; at the same time, the outlet is set to flow boundary.Figure 5
Boundary conditions of the flow channel model.


### 3.3. Result Analysis

#### 3.3.1. Simulation Theory Analysis

Printing molten ABS is complex due to high process temperature; in particular, there exists the phenomenon that two filaments mixing in a color mixing nozzle make the distribution of flow field more complex. It is significant that filament material melted completely and mixed at the intersection, in order to realize the function of color mixing print. The driving force will lose due to an abnormal process temperature, which even will be a cause of the failure in the extrusion of molten filament. That is why filament should not be overheated.The effect of color mixing print depends on whether filament material can be completely melted and mixed at the intersection. The temperature field of two filaments at the intersection is simulated and analyzed through changing the filament feed speed. The optimal combination of filament feed speed and temperature field of the flow channel is obtained by comparing the analysis results.


#### 3.3.2. Simulation Analysis of Two Inlets at a Velocity of 0.2 mm/s

The meshed finite element model is imported into the Fluent software. The filament feed speeds of the first inlet and the second inlet are both set to a velocity of 0.2 mm/s; meanwhile, the initial temperature is set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 493.15 K. The simulation time is set to 60 s to help the ABS filament material existing in the flow channel to be observed better; meanwhile the time nodes of 5 s, 30 s, 50 s, and 60 s are selected to represent the changes of ABS filament in the flow channel. The temperature distribution in the flow channel is obtained by using simulation, and the temperature contours at different time steps are shown in Figure6.Figure 6
Temperature contours of the flow channel at the temperature of 493.15 K: (a) at the time of 5 s; (b) at the time of 30 s; (c) at the time of 50 s; (d) at the time of 60 s.
(a)
(b)
(c)
(d)It can be seen from the temperature contours that the temperature of the flow channel is relatively low at the time of 5 s. In addition, the temperature will increase gradually as time goes on. Heat is constantly being absorbed by filaments, which leads to a decrease in the temperature of the wall surface. As a consequence, a larger temperature gradient appears in the pipe. As a consequence, the temperature inside the flow channel at a time of 50 s is considered as the steady state when the amount of ABS material entry into the pipe is 10 mm. The cross section of pipe at the intersection is chosen to make the temperature contours, which is shown in Figure7.Figure 7
Temperature contours of the intersection cross section in the steady state at the temperature of 493.15 K.As can be seen from Figure7, the temperature of the wall surface is high; on the contrary, the internal temperature of the filament is low. The lowest temperature occurs at the center of the filament, which is about 484.8 K equal to 211.6°C. This temperature does not reach the test temperature for smooth extrusion of the filament, which will result in an incomplete melt of filament. In the case where the filament cannot be melted completely, not only can the mixing effect of material be influenced, but also the extrusion will be blocked. Once the blockage occurs at the intersection, the filament cannot be input or output effectively, which will directly lead to the failure of color mixing printing.In order to melt the ABS filament material at the intersection, the boundary temperature rises to 503.15 K without any changes in other boundary conditions. The steady state temperature distribution of the flow channel at the time of 50 s is as shown in Figure8(a); the temperature distribution of the cross section of intersection is as shown in Figure 8(b).Figure 8
The temperature distribution in the steady state at the time of 50 s: (a) the temperature distribution of flow channel; (b) the temperature distribution of the cross section of the intersection.
(a)
(b)It can be seen from Figure8(a) that the steady state temperature distribution is similar to the temperature distribution of the boundary at a temperature of 493.15 K. It can be summed up that the temperature of the flow channel tends to be steady gradually within 50 s. As can be seen from Figure 9, the temperature distribution of intersection is not uniform; meanwhile, the temperature of the center of filament is the lowest, which is about 494 K equal to 221°C. The filament can be successfully extruded at this temperature.Figure 9
Temperature contours in the steady state at the temperature of 503.15 K at the time of 20 s: (a) temperature contours of the flow channel; (b) temperature contours of intersection cross section.
(a)
(b)Summaries can be made by using simulation. It is appropriate that the temperature of the heating block of the color mixing device is maintained around 503.15 K when the velocity of the inlet is 0.2 mm/s.


#### 3.3.3. Simulation Analysis of Two Inlets at a Velocity of 0.5 mm/s

The boundary conditions are changed during the simulation. The filament feed speed of both inlets is set to 0.5 mm/s with the initial temperature set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 503.15 K. The process of the filament material reaching the intersection through the branch pipe takes approximately 20 s. The simulation time is set to 60 s, in order to allow the temperature distribution of ABS filament at the intersection to be observed better and represent the changes in the temperature of ABS filament existing in flow channel at the time of 20 s. The temperature changes are shown in Figure9(a). The intersection position is chosen to make the temperature contours which are shown in Figure 9(b).As can be seen from Figure9(a), at the time of 20 s, filament gathers at the intersection, and the temperature of the filament is evidently lower than that of the flow channel. The temperature of the cross section shown in Figure 11 is in zonal distribution. The lowest temperature that is 489 K equal to approximately 216°C occurs in the center of filament material, which can meet the requirements for a smooth extrusion of the filament material. The temperature reaches a steady state after 50 s. The temperature of filament at the intersection will rise again, but it is still in a reasonable range for ABS filament melting.Summaries can be made by using the simulation when the velocity of two inlets is at 0.5 mm/s. The heating temperature should be maintained at around 503.15 K, which can meet the requirements for ABS filament melting and mixing at the intersection.


#### 3.3.4. Simulation Analysis of Two Inlets at a Velocity of 1 mm/s

The filament feed speed of both inlets is set to 1 mm/s with the initial temperature set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 508.15 K. The process of filament material reaching intersection through branch pipe takes approximately 10 s. The simulation time is set to 60 s, in order to better observe the temperature distribution of ABS filament at the intersection. The temperature distribution of ABS filament in the flow channel at the time of 10 s is selected to represent the temperature changes, which are shown in Figure10(a). The cross section of intersection is chosen to make temperature contours, which are shown in Figure 10(b).Figure 10
Temperature contours in the steady state at the temperature of 508.15 K at the time of 10 s: (a) temperature contours of the flow channel; (b) temperature contours of the intersection cross section.
(a)
(b)Figure 11
Temperature contours in the steady state at the temperature of 513.15 K at the time of 10 s: (a) temperature contours of the flow channel; (b) temperature contours of the intersection cross section.
(a)
(b)It can be observed from Figure10(a) that the filament material gathers at the intersection at the time of 10 s. Neither the flow channel nor the ABS filament has reached the highest steady state temperature. The temperature of the cross section shown in Figure 10(b) is in zonal distribution as well. Meanwhile, the lowest temperature that is approximately 485 K equal to 212°C occurs in the center of the filament, which is lower than the temperature for smooth extrusion of filament. As a consequence, when the filament feed speed is increased to 1 mm/s, the molten filament at the intersection will not be available at the wall surface temperature of 508.15 K.The temperature of the wall surface rises to 513.15 K without any other changes in boundary conditions. As is shown in Figure11(a), the temperature distribution of the entire flow channel at a time of 10 s is extracted through simulation analysis. The cross section of intersection is chosen to make the temperature contours, which are as shown in Figure 11(b).It can be seen from Figure11(a) that the temperature distribution of channel is similar to that at the temperature of 508.15 K. It can be seen from the temperature distribution of cross section in Figure 11(b) that the lowest temperature which occurs in the center of filament is approximately 489 K equal to 216°C, which can meet the requirements for smooth extrusion of filament. However, the highest temperature of ABS filament will be approximately 513.15 K, when the process is in a steady state. ABS filament will be decomposed at the temperature of 240°C; meanwhile, the temperature of ABS filament will become higher faster by adding heat as soon as it enters into the flow channel, which will result in a premature softening of filament in the flow channel. As a consequence, molten filament material will not be extruded successfully.Through the simulation analysis, it can be summed up that 1 mm/s is too fast for the feed of filament to match the temperature field. During the test process, although the temperature field can meet the requirement for print, the speed of 1 mm/s will lead to over speed of filament extrusion, as well as reduce the accuracy of print objects. In conclusion, a speed of 1 mm/s is not appropriate for filament feed.


#### 3.3.5. Simulation Analysis of Inlets at a Velocity of 0.2 mm/s and 0.5 mm/s, Respectively

It can be known from the analysis that when the velocity of two inlets is 0.2 mm/s and 0.5 mm/s, respectively, ABS filament at the intersection will be completely melted and mixed at the temperature of 503.15 K. In order to further study the feasibility of the device, the finite element model is imported into Fluent software. The speed of the first inlet is set to 0.2 mm/s with the speed of the second inlet being set to 0.5 mm/s. The initial temperature is set to 298.15 K. There is close contact between the heating block and the wall surface whose temperature is set to 503.15 K. The simulation time is set to 60 s, and the ABS filament reaches a steady state after 50 s. The distribution of velocity field, pressure field, and temperature field of ABS filament existing in the flow channel at the time of 50 s is observed.The pressure field and velocity field distribution of ABS filament existing in the flow channel in a steady state at the time of 50 s can be obtained through this simulation. The pressure contours of ABS filament existing in the flow channel in the steady state are shown in Figure12(a). It can be observed from Figure 12(a) that the flow channel is under high pressure because of high inlet velocity. The pressure of molten ABS filament at a speed of 0.5 mm/s is evidently higher than that of 0.2 mm/s. As a consequence, part of molten ABS filament under high pressure will move to an area of less pressure, which will cause a partial reflux. Also, the normal fluid under low pressure is restricted by the fluid under high pressure. It can be seen from the velocity contours in Figure 12(b) that the flow speed near the wall of the pipe is low, and, on the contrary, the flow speed near the center of the pipe is high, because great friction occurs between the molten filament material and the pipe wall surface. In a real world situation, a Teflon hollow tube that will be added to the inner wall of the pipe is composed of polytetrafluoroethylene. The material has a low coefficient of friction, remains stable at elevated temperatures, and offers good resistance to close connection between ABS filament and the inner wall of the device. In that case, the flow speed of the molten material in the pipeline will be increased.Figure 12
Pressure and velocity contours in the steady state: (a) pressure contours; (b) velocity contours.
(a)
(b)In order to realize the function of color mixing print better, the cross sections of pressure contours, velocity contours, and temperature contours are presented in Figure13. It can be seen from the pressure contours that there is a polygonal area with a lower pressure in the center as compared to the surrounding region while the pressure distribution is basically uniform. It can be seen from the velocity contours that there is an area with a higher speed in the center as compared to the surrounding region while the distribution of speed is basically uniform. It can be concluded that the velocity distribution in the nozzle hole area will not be affected by the velocity of the two-inlet area that only determines the peak velocity in the nozzle hole. It can be seen from the temperature contours that although cross section temperature field distribution in outlet area is zonal, the temperature gradient is small; meanwhile, the temperature difference between center area and boundary area is less than 1 K. It can be concluded that the filament reaching nozzle hole has been heated to be completely melted, so the possibility of blockage occurring in nozzle hole area can be ignored.Figure 13
Contours of cross section at nozzle: (a) pressure contours; (b) velocity contours; (c) temperature contours.
(a)
(b)
(c)


## 3.1. Establishment of the Flow Channel Model

In the previous chapter, the model of the 3D printer nozzle for color mixing has been simplified. The flow channel model of the entire mixing device, established by using UG software, is currently extracted and simplified. The parameters of a simplified flow channel model are presented in Table1. The model which will be imported into ICEM CFD meshing software is established by UG. In order to improve the quality of mesh, a Tetra/Mixed meshing type (which is mainly composed of tetrahedral mesh elements) is chosen to mesh the model. As a result, 4936 nodes and 27442 elements are generated. The first entrance, the second entrance, export, and wall are all defined in ICEM CFD software. The finite element model is imported into the Fluent software to carry out fluid analysis. Flow channel model and finite element model of the flow channel are shown in Figure 4.Table 1
Size of the simplified flow channel.
Item
Quantity
Branch pipe length (mm)
10
Main pipe length (mm)
11
Branch pipe angle (°)
60°
Branch pipe diameter (mm)
1.75
Main pipe diameter (mm)
2
Outlet diameter (mm)
0.4Figure 4
(a) 3D model and (b) finite element model of the flow channel.
(a)
(b)


## 3.2. Material Properties of ABS Material and Setting of Model Boundary Conditions

ABS material is one of the most widely used polymers in the world, touching virtually every part of our lives [24]. ABS materials are an excellent choice for models, prototypes, patterns, tools, and end-use parts. Much stronger than the FDM materials just a few years ago, ABS for FDM machines offers greater tensile, impact, and flexural strength today [25]. The ABS material existing in the flow channel is selected as the research object; meanwhile the situation of ABS mixing in the molten state is studied. Thus, the optimum combination of the different filament feed speed and the corresponding heating temperature is summarized. Properties of ABS material are shown in Table 2.Table 2
Properties of ABS material.
Item
Quantity
Density (kg/m3)
1020
Elastic modulus (GPa)
2
Poisson ratio
0.394
Specific heat capacity (J/(kg·K))
1386
Thermal conductivity (W/(m·K))
0.2256
Viscosity (Pa·s)
84The boundary conditions are set based on the simplified flow channel model. The boundary conditions are shown in Figure5. Both the first inlet and second inlet are set to the speed boundary. The material is ABS filament at a diameter of 1.75 mm. The initial temperature of ABS filament is set to 25°C; at the same time, the outlet is set to flow boundary.Figure 5
Boundary conditions of the flow channel model.


## 3.3. Result Analysis

### 3.3.1. Simulation Theory Analysis

Printing molten ABS is complex due to high process temperature; in particular, there exists the phenomenon that two filaments mixing in a color mixing nozzle make the distribution of flow field more complex. It is significant that filament material melted completely and mixed at the intersection, in order to realize the function of color mixing print. The driving force will lose due to an abnormal process temperature, which even will be a cause of the failure in the extrusion of molten filament. That is why filament should not be overheated.The effect of color mixing print depends on whether filament material can be completely melted and mixed at the intersection. The temperature field of two filaments at the intersection is simulated and analyzed through changing the filament feed speed. The optimal combination of filament feed speed and temperature field of the flow channel is obtained by comparing the analysis results.


### 3.3.2. Simulation Analysis of Two Inlets at a Velocity of 0.2 mm/s

The meshed finite element model is imported into the Fluent software. The filament feed speeds of the first inlet and the second inlet are both set to a velocity of 0.2 mm/s; meanwhile, the initial temperature is set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 493.15 K. The simulation time is set to 60 s to help the ABS filament material existing in the flow channel to be observed better; meanwhile the time nodes of 5 s, 30 s, 50 s, and 60 s are selected to represent the changes of ABS filament in the flow channel. The temperature distribution in the flow channel is obtained by using simulation, and the temperature contours at different time steps are shown in Figure6.Figure 6
Temperature contours of the flow channel at the temperature of 493.15 K: (a) at the time of 5 s; (b) at the time of 30 s; (c) at the time of 50 s; (d) at the time of 60 s.
(a)
(b)
(c)
(d)It can be seen from the temperature contours that the temperature of the flow channel is relatively low at the time of 5 s. In addition, the temperature will increase gradually as time goes on. Heat is constantly being absorbed by filaments, which leads to a decrease in the temperature of the wall surface. As a consequence, a larger temperature gradient appears in the pipe. As a consequence, the temperature inside the flow channel at a time of 50 s is considered as the steady state when the amount of ABS material entry into the pipe is 10 mm. The cross section of pipe at the intersection is chosen to make the temperature contours, which is shown in Figure7.Figure 7
Temperature contours of the intersection cross section in the steady state at the temperature of 493.15 K.As can be seen from Figure7, the temperature of the wall surface is high; on the contrary, the internal temperature of the filament is low. The lowest temperature occurs at the center of the filament, which is about 484.8 K equal to 211.6°C. This temperature does not reach the test temperature for smooth extrusion of the filament, which will result in an incomplete melt of filament. In the case where the filament cannot be melted completely, not only can the mixing effect of material be influenced, but also the extrusion will be blocked. Once the blockage occurs at the intersection, the filament cannot be input or output effectively, which will directly lead to the failure of color mixing printing.In order to melt the ABS filament material at the intersection, the boundary temperature rises to 503.15 K without any changes in other boundary conditions. The steady state temperature distribution of the flow channel at the time of 50 s is as shown in Figure8(a); the temperature distribution of the cross section of intersection is as shown in Figure 8(b).Figure 8
The temperature distribution in the steady state at the time of 50 s: (a) the temperature distribution of flow channel; (b) the temperature distribution of the cross section of the intersection.
(a)
(b)It can be seen from Figure8(a) that the steady state temperature distribution is similar to the temperature distribution of the boundary at a temperature of 493.15 K. It can be summed up that the temperature of the flow channel tends to be steady gradually within 50 s. As can be seen from Figure 9, the temperature distribution of intersection is not uniform; meanwhile, the temperature of the center of filament is the lowest, which is about 494 K equal to 221°C. The filament can be successfully extruded at this temperature.Figure 9
Temperature contours in the steady state at the temperature of 503.15 K at the time of 20 s: (a) temperature contours of the flow channel; (b) temperature contours of intersection cross section.
(a)
(b)Summaries can be made by using simulation. It is appropriate that the temperature of the heating block of the color mixing device is maintained around 503.15 K when the velocity of the inlet is 0.2 mm/s.


### 3.3.3. Simulation Analysis of Two Inlets at a Velocity of 0.5 mm/s

The boundary conditions are changed during the simulation. The filament feed speed of both inlets is set to 0.5 mm/s with the initial temperature set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 503.15 K. The process of the filament material reaching the intersection through the branch pipe takes approximately 20 s. The simulation time is set to 60 s, in order to allow the temperature distribution of ABS filament at the intersection to be observed better and represent the changes in the temperature of ABS filament existing in flow channel at the time of 20 s. The temperature changes are shown in Figure9(a). The intersection position is chosen to make the temperature contours which are shown in Figure 9(b).As can be seen from Figure9(a), at the time of 20 s, filament gathers at the intersection, and the temperature of the filament is evidently lower than that of the flow channel. The temperature of the cross section shown in Figure 11 is in zonal distribution. The lowest temperature that is 489 K equal to approximately 216°C occurs in the center of filament material, which can meet the requirements for a smooth extrusion of the filament material. The temperature reaches a steady state after 50 s. The temperature of filament at the intersection will rise again, but it is still in a reasonable range for ABS filament melting.Summaries can be made by using the simulation when the velocity of two inlets is at 0.5 mm/s. The heating temperature should be maintained at around 503.15 K, which can meet the requirements for ABS filament melting and mixing at the intersection.


### 3.3.4. Simulation Analysis of Two Inlets at a Velocity of 1 mm/s

The filament feed speed of both inlets is set to 1 mm/s with the initial temperature set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 508.15 K. The process of filament material reaching intersection through branch pipe takes approximately 10 s. The simulation time is set to 60 s, in order to better observe the temperature distribution of ABS filament at the intersection. The temperature distribution of ABS filament in the flow channel at the time of 10 s is selected to represent the temperature changes, which are shown in Figure10(a). The cross section of intersection is chosen to make temperature contours, which are shown in Figure 10(b).Figure 10
Temperature contours in the steady state at the temperature of 508.15 K at the time of 10 s: (a) temperature contours of the flow channel; (b) temperature contours of the intersection cross section.
(a)
(b)Figure 11
Temperature contours in the steady state at the temperature of 513.15 K at the time of 10 s: (a) temperature contours of the flow channel; (b) temperature contours of the intersection cross section.
(a)
(b)It can be observed from Figure10(a) that the filament material gathers at the intersection at the time of 10 s. Neither the flow channel nor the ABS filament has reached the highest steady state temperature. The temperature of the cross section shown in Figure 10(b) is in zonal distribution as well. Meanwhile, the lowest temperature that is approximately 485 K equal to 212°C occurs in the center of the filament, which is lower than the temperature for smooth extrusion of filament. As a consequence, when the filament feed speed is increased to 1 mm/s, the molten filament at the intersection will not be available at the wall surface temperature of 508.15 K.The temperature of the wall surface rises to 513.15 K without any other changes in boundary conditions. As is shown in Figure11(a), the temperature distribution of the entire flow channel at a time of 10 s is extracted through simulation analysis. The cross section of intersection is chosen to make the temperature contours, which are as shown in Figure 11(b).It can be seen from Figure11(a) that the temperature distribution of channel is similar to that at the temperature of 508.15 K. It can be seen from the temperature distribution of cross section in Figure 11(b) that the lowest temperature which occurs in the center of filament is approximately 489 K equal to 216°C, which can meet the requirements for smooth extrusion of filament. However, the highest temperature of ABS filament will be approximately 513.15 K, when the process is in a steady state. ABS filament will be decomposed at the temperature of 240°C; meanwhile, the temperature of ABS filament will become higher faster by adding heat as soon as it enters into the flow channel, which will result in a premature softening of filament in the flow channel. As a consequence, molten filament material will not be extruded successfully.Through the simulation analysis, it can be summed up that 1 mm/s is too fast for the feed of filament to match the temperature field. During the test process, although the temperature field can meet the requirement for print, the speed of 1 mm/s will lead to over speed of filament extrusion, as well as reduce the accuracy of print objects. In conclusion, a speed of 1 mm/s is not appropriate for filament feed.


### 3.3.5. Simulation Analysis of Inlets at a Velocity of 0.2 mm/s and 0.5 mm/s, Respectively

It can be known from the analysis that when the velocity of two inlets is 0.2 mm/s and 0.5 mm/s, respectively, ABS filament at the intersection will be completely melted and mixed at the temperature of 503.15 K. In order to further study the feasibility of the device, the finite element model is imported into Fluent software. The speed of the first inlet is set to 0.2 mm/s with the speed of the second inlet being set to 0.5 mm/s. The initial temperature is set to 298.15 K. There is close contact between the heating block and the wall surface whose temperature is set to 503.15 K. The simulation time is set to 60 s, and the ABS filament reaches a steady state after 50 s. The distribution of velocity field, pressure field, and temperature field of ABS filament existing in the flow channel at the time of 50 s is observed.The pressure field and velocity field distribution of ABS filament existing in the flow channel in a steady state at the time of 50 s can be obtained through this simulation. The pressure contours of ABS filament existing in the flow channel in the steady state are shown in Figure12(a). It can be observed from Figure 12(a) that the flow channel is under high pressure because of high inlet velocity. The pressure of molten ABS filament at a speed of 0.5 mm/s is evidently higher than that of 0.2 mm/s. As a consequence, part of molten ABS filament under high pressure will move to an area of less pressure, which will cause a partial reflux. Also, the normal fluid under low pressure is restricted by the fluid under high pressure. It can be seen from the velocity contours in Figure 12(b) that the flow speed near the wall of the pipe is low, and, on the contrary, the flow speed near the center of the pipe is high, because great friction occurs between the molten filament material and the pipe wall surface. In a real world situation, a Teflon hollow tube that will be added to the inner wall of the pipe is composed of polytetrafluoroethylene. The material has a low coefficient of friction, remains stable at elevated temperatures, and offers good resistance to close connection between ABS filament and the inner wall of the device. In that case, the flow speed of the molten material in the pipeline will be increased.Figure 12
Pressure and velocity contours in the steady state: (a) pressure contours; (b) velocity contours.
(a)
(b)In order to realize the function of color mixing print better, the cross sections of pressure contours, velocity contours, and temperature contours are presented in Figure13. It can be seen from the pressure contours that there is a polygonal area with a lower pressure in the center as compared to the surrounding region while the pressure distribution is basically uniform. It can be seen from the velocity contours that there is an area with a higher speed in the center as compared to the surrounding region while the distribution of speed is basically uniform. It can be concluded that the velocity distribution in the nozzle hole area will not be affected by the velocity of the two-inlet area that only determines the peak velocity in the nozzle hole. It can be seen from the temperature contours that although cross section temperature field distribution in outlet area is zonal, the temperature gradient is small; meanwhile, the temperature difference between center area and boundary area is less than 1 K. It can be concluded that the filament reaching nozzle hole has been heated to be completely melted, so the possibility of blockage occurring in nozzle hole area can be ignored.Figure 13
Contours of cross section at nozzle: (a) pressure contours; (b) velocity contours; (c) temperature contours.
(a)
(b)
(c)


## 3.3.1. Simulation Theory Analysis

Printing molten ABS is complex due to high process temperature; in particular, there exists the phenomenon that two filaments mixing in a color mixing nozzle make the distribution of flow field more complex. It is significant that filament material melted completely and mixed at the intersection, in order to realize the function of color mixing print. The driving force will lose due to an abnormal process temperature, which even will be a cause of the failure in the extrusion of molten filament. That is why filament should not be overheated.The effect of color mixing print depends on whether filament material can be completely melted and mixed at the intersection. The temperature field of two filaments at the intersection is simulated and analyzed through changing the filament feed speed. The optimal combination of filament feed speed and temperature field of the flow channel is obtained by comparing the analysis results.


## 3.3.2. Simulation Analysis of Two Inlets at a Velocity of 0.2 mm/s

The meshed finite element model is imported into the Fluent software. The filament feed speeds of the first inlet and the second inlet are both set to a velocity of 0.2 mm/s; meanwhile, the initial temperature is set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 493.15 K. The simulation time is set to 60 s to help the ABS filament material existing in the flow channel to be observed better; meanwhile the time nodes of 5 s, 30 s, 50 s, and 60 s are selected to represent the changes of ABS filament in the flow channel. The temperature distribution in the flow channel is obtained by using simulation, and the temperature contours at different time steps are shown in Figure6.Figure 6
Temperature contours of the flow channel at the temperature of 493.15 K: (a) at the time of 5 s; (b) at the time of 30 s; (c) at the time of 50 s; (d) at the time of 60 s.
(a)
(b)
(c)
(d)It can be seen from the temperature contours that the temperature of the flow channel is relatively low at the time of 5 s. In addition, the temperature will increase gradually as time goes on. Heat is constantly being absorbed by filaments, which leads to a decrease in the temperature of the wall surface. As a consequence, a larger temperature gradient appears in the pipe. As a consequence, the temperature inside the flow channel at a time of 50 s is considered as the steady state when the amount of ABS material entry into the pipe is 10 mm. The cross section of pipe at the intersection is chosen to make the temperature contours, which is shown in Figure7.Figure 7
Temperature contours of the intersection cross section in the steady state at the temperature of 493.15 K.As can be seen from Figure7, the temperature of the wall surface is high; on the contrary, the internal temperature of the filament is low. The lowest temperature occurs at the center of the filament, which is about 484.8 K equal to 211.6°C. This temperature does not reach the test temperature for smooth extrusion of the filament, which will result in an incomplete melt of filament. In the case where the filament cannot be melted completely, not only can the mixing effect of material be influenced, but also the extrusion will be blocked. Once the blockage occurs at the intersection, the filament cannot be input or output effectively, which will directly lead to the failure of color mixing printing.In order to melt the ABS filament material at the intersection, the boundary temperature rises to 503.15 K without any changes in other boundary conditions. The steady state temperature distribution of the flow channel at the time of 50 s is as shown in Figure8(a); the temperature distribution of the cross section of intersection is as shown in Figure 8(b).Figure 8
The temperature distribution in the steady state at the time of 50 s: (a) the temperature distribution of flow channel; (b) the temperature distribution of the cross section of the intersection.
(a)
(b)It can be seen from Figure8(a) that the steady state temperature distribution is similar to the temperature distribution of the boundary at a temperature of 493.15 K. It can be summed up that the temperature of the flow channel tends to be steady gradually within 50 s. As can be seen from Figure 9, the temperature distribution of intersection is not uniform; meanwhile, the temperature of the center of filament is the lowest, which is about 494 K equal to 221°C. The filament can be successfully extruded at this temperature.Figure 9
Temperature contours in the steady state at the temperature of 503.15 K at the time of 20 s: (a) temperature contours of the flow channel; (b) temperature contours of intersection cross section.
(a)
(b)Summaries can be made by using simulation. It is appropriate that the temperature of the heating block of the color mixing device is maintained around 503.15 K when the velocity of the inlet is 0.2 mm/s.


## 3.3.3. Simulation Analysis of Two Inlets at a Velocity of 0.5 mm/s

The boundary conditions are changed during the simulation. The filament feed speed of both inlets is set to 0.5 mm/s with the initial temperature set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 503.15 K. The process of the filament material reaching the intersection through the branch pipe takes approximately 20 s. The simulation time is set to 60 s, in order to allow the temperature distribution of ABS filament at the intersection to be observed better and represent the changes in the temperature of ABS filament existing in flow channel at the time of 20 s. The temperature changes are shown in Figure9(a). The intersection position is chosen to make the temperature contours which are shown in Figure 9(b).As can be seen from Figure9(a), at the time of 20 s, filament gathers at the intersection, and the temperature of the filament is evidently lower than that of the flow channel. The temperature of the cross section shown in Figure 11 is in zonal distribution. The lowest temperature that is 489 K equal to approximately 216°C occurs in the center of filament material, which can meet the requirements for a smooth extrusion of the filament material. The temperature reaches a steady state after 50 s. The temperature of filament at the intersection will rise again, but it is still in a reasonable range for ABS filament melting.Summaries can be made by using the simulation when the velocity of two inlets is at 0.5 mm/s. The heating temperature should be maintained at around 503.15 K, which can meet the requirements for ABS filament melting and mixing at the intersection.


## 3.3.4. Simulation Analysis of Two Inlets at a Velocity of 1 mm/s

The filament feed speed of both inlets is set to 1 mm/s with the initial temperature set to 298.15 K. There is a close contact between the heating block and the wall surface whose temperature is set to 508.15 K. The process of filament material reaching intersection through branch pipe takes approximately 10 s. The simulation time is set to 60 s, in order to better observe the temperature distribution of ABS filament at the intersection. The temperature distribution of ABS filament in the flow channel at the time of 10 s is selected to represent the temperature changes, which are shown in Figure10(a). The cross section of intersection is chosen to make temperature contours, which are shown in Figure 10(b).Figure 10
Temperature contours in the steady state at the temperature of 508.15 K at the time of 10 s: (a) temperature contours of the flow channel; (b) temperature contours of the intersection cross section.
(a)
(b)Figure 11
Temperature contours in the steady state at the temperature of 513.15 K at the time of 10 s: (a) temperature contours of the flow channel; (b) temperature contours of the intersection cross section.
(a)
(b)It can be observed from Figure10(a) that the filament material gathers at the intersection at the time of 10 s. Neither the flow channel nor the ABS filament has reached the highest steady state temperature. The temperature of the cross section shown in Figure 10(b) is in zonal distribution as well. Meanwhile, the lowest temperature that is approximately 485 K equal to 212°C occurs in the center of the filament, which is lower than the temperature for smooth extrusion of filament. As a consequence, when the filament feed speed is increased to 1 mm/s, the molten filament at the intersection will not be available at the wall surface temperature of 508.15 K.The temperature of the wall surface rises to 513.15 K without any other changes in boundary conditions. As is shown in Figure11(a), the temperature distribution of the entire flow channel at a time of 10 s is extracted through simulation analysis. The cross section of intersection is chosen to make the temperature contours, which are as shown in Figure 11(b).It can be seen from Figure11(a) that the temperature distribution of channel is similar to that at the temperature of 508.15 K. It can be seen from the temperature distribution of cross section in Figure 11(b) that the lowest temperature which occurs in the center of filament is approximately 489 K equal to 216°C, which can meet the requirements for smooth extrusion of filament. However, the highest temperature of ABS filament will be approximately 513.15 K, when the process is in a steady state. ABS filament will be decomposed at the temperature of 240°C; meanwhile, the temperature of ABS filament will become higher faster by adding heat as soon as it enters into the flow channel, which will result in a premature softening of filament in the flow channel. As a consequence, molten filament material will not be extruded successfully.Through the simulation analysis, it can be summed up that 1 mm/s is too fast for the feed of filament to match the temperature field. During the test process, although the temperature field can meet the requirement for print, the speed of 1 mm/s will lead to over speed of filament extrusion, as well as reduce the accuracy of print objects. In conclusion, a speed of 1 mm/s is not appropriate for filament feed.


## 3.3.5. Simulation Analysis of Inlets at a Velocity of 0.2 mm/s and 0.5 mm/s, Respectively

It can be known from the analysis that when the velocity of two inlets is 0.2 mm/s and 0.5 mm/s, respectively, ABS filament at the intersection will be completely melted and mixed at the temperature of 503.15 K. In order to further study the feasibility of the device, the finite element model is imported into Fluent software. The speed of the first inlet is set to 0.2 mm/s with the speed of the second inlet being set to 0.5 mm/s. The initial temperature is set to 298.15 K. There is close contact between the heating block and the wall surface whose temperature is set to 503.15 K. The simulation time is set to 60 s, and the ABS filament reaches a steady state after 50 s. The distribution of velocity field, pressure field, and temperature field of ABS filament existing in the flow channel at the time of 50 s is observed.The pressure field and velocity field distribution of ABS filament existing in the flow channel in a steady state at the time of 50 s can be obtained through this simulation. The pressure contours of ABS filament existing in the flow channel in the steady state are shown in Figure12(a). It can be observed from Figure 12(a) that the flow channel is under high pressure because of high inlet velocity. The pressure of molten ABS filament at a speed of 0.5 mm/s is evidently higher than that of 0.2 mm/s. As a consequence, part of molten ABS filament under high pressure will move to an area of less pressure, which will cause a partial reflux. Also, the normal fluid under low pressure is restricted by the fluid under high pressure. It can be seen from the velocity contours in Figure 12(b) that the flow speed near the wall of the pipe is low, and, on the contrary, the flow speed near the center of the pipe is high, because great friction occurs between the molten filament material and the pipe wall surface. In a real world situation, a Teflon hollow tube that will be added to the inner wall of the pipe is composed of polytetrafluoroethylene. The material has a low coefficient of friction, remains stable at elevated temperatures, and offers good resistance to close connection between ABS filament and the inner wall of the device. In that case, the flow speed of the molten material in the pipeline will be increased.Figure 12
Pressure and velocity contours in the steady state: (a) pressure contours; (b) velocity contours.
(a)
(b)In order to realize the function of color mixing print better, the cross sections of pressure contours, velocity contours, and temperature contours are presented in Figure13. It can be seen from the pressure contours that there is a polygonal area with a lower pressure in the center as compared to the surrounding region while the pressure distribution is basically uniform. It can be seen from the velocity contours that there is an area with a higher speed in the center as compared to the surrounding region while the distribution of speed is basically uniform. It can be concluded that the velocity distribution in the nozzle hole area will not be affected by the velocity of the two-inlet area that only determines the peak velocity in the nozzle hole. It can be seen from the temperature contours that although cross section temperature field distribution in outlet area is zonal, the temperature gradient is small; meanwhile, the temperature difference between center area and boundary area is less than 1 K. It can be concluded that the filament reaching nozzle hole has been heated to be completely melted, so the possibility of blockage occurring in nozzle hole area can be ignored.Figure 13
Contours of cross section at nozzle: (a) pressure contours; (b) velocity contours; (c) temperature contours.
(a)
(b)
(c)


## 4. Test Verification and Structure Improvement of the Nozzle for Color Mixing Device

### 4.1. Test Verification of the Nozzle for Color Mixing Device

Based on the simulation of flow for the whole device, the test of the whole device is carried out to verify whether it can meet the requirements for color mixing print. The heating block and the fixed block are produced in terms of design parameters. The parts of the heating block and fixed block are then assembled immediately and clamped together. The assembled color mixing head is shown in Figure14.Figure 14
3D printer device for color mixing.The whole mixing head is fixed on the 3D printer, and the heating pipe and the thermal resistor are arranged on the heating block. The 3D printer connects to a computer via a USB cable running Repetier-Host software that controls the heating block [26–28]. The temperature of the heating block is set in terms of the melting point of filament. When the temperature reaches the set temperature, the filament can be fed into the heating block along the throat pipe. Two kinds of filament will be melted at the end of the pipe and mix in the heating block. With the continuous supplies of material, mix melt will be extruded through the nozzle. Different mixing effects will be realized through controlling the speed of the stepper motor. The test is mainly to verify the feasibility of the device at a temperature of 220°C and 230°C, respectively. Orange and green ABS filaments are chosen to be tested. Meanwhile, a cylinder whose diameter and height are 10 mm and 10 mm, respectively, is regarded as a printing model. The color mixing nozzle is a mechanical device with dual inlets and a unique outlet. The cylinder model is sliced by Repetier-Host software. In order to meet the requirements for mixing color print, part of the codes is modified in terms of the color mixing requirements.For the first time, the temperature of the nozzle is set to 220°C to print objects. During the initial test, when one-third of the model is finished, as can be seen in Figure15(a), the extrusion stops, and the filament slips under continuous supply. The nozzle device is disassembled after cooling. Blockage occurs at the intersection of the end of pipe and heating block. Secondly, the test of the whole nozzle device at the temperature of 220°C is carried out after the whole nozzle device is cleaned up, as can be seen in Figure 15(b); the outcome of a mix of colors is obvious without evident phenomenon of stratification and accumulation. After the nozzle device is cleaned up, the temperature of the nozzle is set to 230°C for forming; as a result, the print test is a success. The test results are as shown in Figure 16.Figure 15
3D printing objects at the temperature of 220°C: (a) blocked; (b) successful.
(a)
(b)Figure 16
3D printing object at the temperature of 230°C.It can be seen from the outcome of the color mixing test that the filament at the intersection of the nozzle is not completely melted at the temperature of 220°C. When the feed of filament is not smooth or steady, the nozzle is at a great risk of being blocked by ABS material. The filament can be smoothly mixed at the nozzle temperature of 230°C; however, the phenomenon of molten filament accumulation can be seen clearly, which will harm the forming effects. It shows that molten ABS material existing in the nozzle has a low stickiness and a strong liquidity at a temperature of 230°C, which results in an incomplete extrusion of ABS material.The outcome of the test shows that the mixing nozzle device can realize the function of mixing print basically. By analyzing the outcome of the test, it can be found that there exists a risk that blockage may occur in the intersection of the heating block. Meanwhile, it can be seen from the outcome of the test that a flaw exists in the design of the intersection. In order to remove the risk of blockage existing in the device, the structure of the device needs improvement in the future.


## 4.1. Test Verification of the Nozzle for Color Mixing Device

Based on the simulation of flow for the whole device, the test of the whole device is carried out to verify whether it can meet the requirements for color mixing print. The heating block and the fixed block are produced in terms of design parameters. The parts of the heating block and fixed block are then assembled immediately and clamped together. The assembled color mixing head is shown in Figure14.Figure 14
3D printer device for color mixing.The whole mixing head is fixed on the 3D printer, and the heating pipe and the thermal resistor are arranged on the heating block. The 3D printer connects to a computer via a USB cable running Repetier-Host software that controls the heating block [26–28]. The temperature of the heating block is set in terms of the melting point of filament. When the temperature reaches the set temperature, the filament can be fed into the heating block along the throat pipe. Two kinds of filament will be melted at the end of the pipe and mix in the heating block. With the continuous supplies of material, mix melt will be extruded through the nozzle. Different mixing effects will be realized through controlling the speed of the stepper motor. The test is mainly to verify the feasibility of the device at a temperature of 220°C and 230°C, respectively. Orange and green ABS filaments are chosen to be tested. Meanwhile, a cylinder whose diameter and height are 10 mm and 10 mm, respectively, is regarded as a printing model. The color mixing nozzle is a mechanical device with dual inlets and a unique outlet. The cylinder model is sliced by Repetier-Host software. In order to meet the requirements for mixing color print, part of the codes is modified in terms of the color mixing requirements.For the first time, the temperature of the nozzle is set to 220°C to print objects. During the initial test, when one-third of the model is finished, as can be seen in Figure15(a), the extrusion stops, and the filament slips under continuous supply. The nozzle device is disassembled after cooling. Blockage occurs at the intersection of the end of pipe and heating block. Secondly, the test of the whole nozzle device at the temperature of 220°C is carried out after the whole nozzle device is cleaned up, as can be seen in Figure 15(b); the outcome of a mix of colors is obvious without evident phenomenon of stratification and accumulation. After the nozzle device is cleaned up, the temperature of the nozzle is set to 230°C for forming; as a result, the print test is a success. The test results are as shown in Figure 16.Figure 15
3D printing objects at the temperature of 220°C: (a) blocked; (b) successful.
(a)
(b)Figure 16
3D printing object at the temperature of 230°C.It can be seen from the outcome of the color mixing test that the filament at the intersection of the nozzle is not completely melted at the temperature of 220°C. When the feed of filament is not smooth or steady, the nozzle is at a great risk of being blocked by ABS material. The filament can be smoothly mixed at the nozzle temperature of 230°C; however, the phenomenon of molten filament accumulation can be seen clearly, which will harm the forming effects. It shows that molten ABS material existing in the nozzle has a low stickiness and a strong liquidity at a temperature of 230°C, which results in an incomplete extrusion of ABS material.The outcome of the test shows that the mixing nozzle device can realize the function of mixing print basically. By analyzing the outcome of the test, it can be found that there exists a risk that blockage may occur in the intersection of the heating block. Meanwhile, it can be seen from the outcome of the test that a flaw exists in the design of the intersection. In order to remove the risk of blockage existing in the device, the structure of the device needs improvement in the future.


## 5. Conclusions

As a kind of mature rapid prototyping technology, fused deposition modeling has been a new production method in the 21st century. In this paper, the CAD model of 3D printer color mixing nozzle device is established by UG software; meanwhile, the flow channel part of the whole device is extracted and simplified. The CAD model and the finite element model are established by UG and ICEM CFD, respectively, and then the flow field is simulated by Fluent software. Combined with the simulation results, the test print of the color mixing nozzle device is performed. According to the test, the structure of 3D printer nozzle is improved. After the above research, the conclusions are as follows.(1)
The flow field of the simplified flow channel of the mixing nozzle device is simulated by using the Fluent software. The results are as follows: The flow condition of the filament is complex, and the control of the temperature field is the key factor in mixing color print. The suitable temperature of the nozzle at different extrusion speeds is obtained, and the reason for the blockage of filament material at the intersection of the heating block is revealed.(2)
The feasibility and practicability of the device are verified through the test, but the defect of the whole device is also found through the test results. In order to remove the risk of blockage existing in the device, the improved structure of the device is needed in the future.



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*Source: 2095137-2017-08-13.xml*