Comparative Study on the Activity of GaF 3 and Ga 2 O 3 Nanoparticle-Doped CsF-AlF 3 Flux for Brazing 6061 Al / Q235 Steel Joints

: The e ﬀ ect of trace amounts of GaF 3 and Ga 2 O 3 nanoparticles on the wettability and spreadability of CsF-AlF 3 ﬂux matched Zn-15Al ﬁller metal were comparatively studied on 6061 aluminum alloy and Q235 low-carbon steel. The experimental results indicate that appropriate amounts of GaF 3 and Ga 2 O 3 added into the ﬂux could signiﬁcantly promote the Zn-15Al ﬁller metal to wet and spread on the surface of 6061 aluminum alloy and Q235 low-carbon steel. The optimum ranges for GaF 3 and Ga 2 O 3 were 0.0075–0.01wt.% and 0.009–0.01 wt.%, respectively. Comparative analysis showed that the activity of CsF-AlF 3 ﬂux bearing GaF 3 was higher than that bearing Ga 2 O 3 . The reason for this is that the former ﬂux has a stronger ability to remove oxides of the base metal and reduce the interfacial tension of the molten ﬁller metal and the base metal.


Introduction
Considering their excellent physical and chemical properties as well as good mechanical processability and corrosion resistance, aluminum alloys has become the most widely used non-ferrous metal structural materials in modern industries, including appliances, construction, light industry, storage tanks, aviation, aerospace, automobile and weapons. Among them, 6061 aluminum alloy has the advantages of excellent formability, welding performance, machinability and corrosion resistance [1,2]. Despite their outstanding properties, the mechanical strength of aluminum alloys is occasionally insufficient to meet the requirements of rigid structures such as car body keel, while the welding structure of aluminum and steel can effectively reduce the weight and additionally exhibit an enhanced strength. Therefore, the combination of aluminum alloy and steel shows great potential in the manufacturing industry.
Although the combination of aluminum alloy and steel plays an important role in the modern manufacturing industry, it remains a hot topic and difficult problem to obtain stable and reliable welded joints in the welding field, particularly for complicated situation in aluminum/steel dissimilar metals [3,4]. Domestic and foreign scholars were committed to the problem of aluminum steel welding in recent years and have proposed various welding approaches, such as cold metal transition brazing [5], aluminum alloy/galvanized steel MIG welding [6] and so on. The difficulties in the welding of aluminum/steel dissimilar metals is mainly related to the following two aspects: the different physical properties of aluminum and steel, which lead to considerable welding stress in the joints, and the brittle intermetallic compounds of the Fe-Al phase generated at the interface between aluminum and steel which exert a great impact on the mechanical properties of joints. The latter is the main contributor to a less reliable connection between aluminum and steel. Iron has a rather low solubility

Materials and Methods
The base metals used in this work were the 6061 aluminum alloy and the Q235 steel, and the compositions of these two materials are respectively listed in Tables 1 and 2. The filler metal was Zn-15Al alloy. A series of CsF-AlF 3 -GaF 3 fluxes with different contents of GaF 3 were prepared by using 99.9% GaF 3 flux and GaF 3 of AR purity, and the variation range of GaF 3 is 0.0001-0.1 wt.%. Nano Ga 2 O 3 powder in the range of 0.0001-0.1 wt.% were added into the commercial CsF-AlF 3 flux to obtain a series of CsF-AlF 3 -Ga 2 O 3 fluxes. As an advance preparation, all the filler metal alloys were extruded as a wire with a 2 mm diameter. The base metals for the spreading test were processed into plates with the dimensions of 40 mm × 40 mm × 3 mm in advance. All the specimens and filler metals were mechanically polished using SiC paper. In addition, the above-mentioned experimental materials were degreased with acetone and cleaned using ethanol before brazing.  The spreading test was carried out strictly in accordance with China's National Standard GB 11364-2008. In this process, 0.1 g filler metal was accurately weighted and placed on the Q235 steel or 6061 aluminum alloy covered with the prepared CsF-AlF 3 -GaF 3 flux or CsF-AlF 3 -Ga 2 O 3 flux and then carefully put into an electrical resistance furnace as Figure 1. The heating temperature was set at 530 • C and the holding time was 1 min. After the test, the flux residues were collected from the surface of the base metal with clean tweezers and the components in the residues were analyzed with an XRD diffractometer (Brucker D8). CuKα radiation was used in the test, with the voltage of 40 kV, the current of 110 mA, and the scanning speed of 1 • /min. The brazing alloy sample should be polished before test. A 3 mm × 3 mm sample was cut on one side of the brazed joint and used for XRD analysis after cleaning. Then, ultrasonic wave waits were incorporated to clean the test board of base material and calculate the spreading area. In order to ensure the accuracy of the test results, the above tests were repeated 5 times under the same conditions, and the results were averaged.  The spreading test was carried out strictly in accordance with China's National Standard GB 11364-2008. In this process, 0.1 g filler metal was accurately weighted and placed on the Q235 steel or 6061 aluminum alloy covered with the prepared CsF-AlF3-GaF3 flux or CsF-AlF3-Ga2O3 flux and then carefully put into an electrical resistance furnace as Figure 1. The heating temperature was set at 530 °C and the holding time was 1 min. After the test, the flux residues were collected from the surface of the base metal with clean tweezers and the components in the residues were analyzed with an XRD diffractometer (Brucker D8). CuKα radiation was used in the test, with the voltage of 40 kV, the current of 110 mA, and the scanning speed of 1 °/min. The brazing alloy sample should be polished before test. A 3 mm × 3 mm sample was cut on one side of the brazed joint and used for XRD analysis after cleaning. Then, ultrasonic wave waits were incorporated to clean the test board of base material and calculate the spreading area. In order to ensure the accuracy of the test results, the above tests were repeated 5 times under the same conditions, and the results were averaged.

The Spreadability and Wettability of Zn-15Al Filler Metal
The effect of GaF3 and Ga2O3 particles on the spreadability of Zn-15Al filler metal was evaluated by the spreading tests that were carried out on the surface of 6061 aluminum alloy and Q235 lowcarbon steel with aid of the prepared flux bearing nanoparticles. The spreading areas were measured and averaged. Figure 2a showed the relationship between the concentration of GaF3 and Ga2O3 and spreading area on 6061 aluminum alloy. When the concentration of GaF3 was 0.01 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 328 mm 2 , which is 64% higher than that without GaF3 addition (200 mm 2 ). The maximum spreading area of Zn-15Al on 6061 aluminum alloy was 319 mm 2 and was increased by 60% compared with that without doping Ga2O3 into the flux, while the concentration of Ga2O3 was 0.009 wt.%.

The Spreadability and Wettability of Zn-15Al Filler Metal
The effect of GaF 3 and Ga 2 O 3 particles on the spreadability of Zn-15Al filler metal was evaluated by the spreading tests that were carried out on the surface of 6061 aluminum alloy and Q235 low-carbon steel with aid of the prepared flux bearing nanoparticles. The spreading areas were measured and averaged. Figure 2a showed the relationship between the concentration of GaF 3 and Ga 2 O 3 and spreading area on 6061 aluminum alloy. When the concentration of GaF 3 was 0.01 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 328 mm 2 , which is 64% higher than that without GaF 3 addition (200 mm 2 ). The maximum spreading area of Zn-15Al on 6061 aluminum alloy was 319 mm 2 and was increased by 60% compared with that without doping Ga 2 O 3 into the flux, while the concentration of Ga 2 O 3 was 0.009 wt.%. indicates that the spreadability of Zn-15Al filler metal over Q235 steel than Ga 2 O 3 was clearly improved by the addition of GaF 3 into the CsF-AlF 3 flux. When the concentration of GaF 3 was 0.0075 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 188 mm 2 . When the concentration of Ga 2 O 3 was 0.01 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 160 mm 2 . Under this circumstance, by adding GaF 3 , the spreading area of Zn-15Al filler metal over Q235 steel was increased by 104% comparing to that of CsF-AlF 3 flux (92 mm 2 ) and by 17.5% comparing to the addition of Ga 2 O 3 .
Considering the spreading of Zn-15Al filler metal on both 6061 aluminum alloy and Q235 low-carbon steel, the optimum ranges for GaF 3 and Ga 2 O 3 in CsF-AlF 3 flux were 0.0075-0.01 wt.% and 0.009-0.01 wt.%, respectively.
Crystals 2020, 10, x FOR PEER REVIEW 4 of 10 Figure 2b indicates that the spreadability of Zn-15Al filler metal over Q235 steel than Ga2O3 was clearly improved by the addition of GaF3 into the CsF-AlF3 flux. When the concentration of GaF3 was 0.0075 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 188 mm 2 . When the concentration of Ga2O3 was 0.01 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 160 mm 2 . Under this circumstance, by adding GaF3, the spreading area of Zn-15Al filler metal over Q235 steel was increased by 104% comparing to that of CsF-AlF3 flux (92 mm 2 ) and by 17.5% comparing to the addition of Ga2O3.

The Mechanism of Interfacial Reaction
The CsF-AlF3-GaF3 flux could effectively improve the spreadability of Zn-15Al filler metal over 6061 aluminum alloy and Q235 steel, but how it worked was not clear yet and deserved a detailed investigation. Therefore, the theory of interfacial tension was applied reasonably to confirm some potential explanations. On the basis of the Young's equation illustrated by Figure 3 and Equation (1), the liquid balance over solid surface was determined by the interfacial tensions between solids, liquids and gases. Specifically, these interfacial tensions could be summed up as between base metal and molten flux (γSF), molten filler metal and molten flux (γLF) and base metal and molten filler metal (γSL) in this study.
Non-reactive wetting and reactive wetting were two approaches to wetting a solid with molten metal, and the interfacial tension between the base metal and molten filler metal (γSL) decreased due to the reaction and the spreading was improved. Because the molted flux reacted with the surface metallic oxides over the base metal and removed them, the reactive wetting was what we discussed in this research. While balancing, the relationship of interfacial tensions is shown as Equation (1).
Alumina reacted with melted XF-AlF3 (X = Na, K, Rb, Cs) flux and formed AlF3 to be dissolved, and the interfacial tension of solid-liquid (γSL) changed from Zn-Al alloy-alumina to Zn-Al alloyaluminum [13]. The remarkable intersolubility of Zn and Al made the interfacial tension between

The Mechanism of Interfacial Reaction
The CsF-AlF 3 -GaF 3 flux could effectively improve the spreadability of Zn-15Al filler metal over 6061 aluminum alloy and Q235 steel, but how it worked was not clear yet and deserved a detailed investigation. Therefore, the theory of interfacial tension was applied reasonably to confirm some potential explanations. On the basis of the Young's equation illustrated by Figure 3 and Equation (1), the liquid balance over solid surface was determined by the interfacial tensions between solids, liquids and gases. Specifically, these interfacial tensions could be summed up as between base metal and molten flux (γ SF ), molten filler metal and molten flux (γ LF ) and base metal and molten filler metal (γ SL ) in this study. Figure 2b indicates that the spreadability of Zn-15Al filler metal over Q235 steel than Ga2O3 was clearly improved by the addition of GaF3 into the CsF-AlF3 flux. When the concentration of GaF3 was 0.0075 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 188 mm 2 . When the concentration of Ga2O3 was 0.01 wt.%, the maximum spreading area of Zn-15Al on 6061 aluminum alloy was 160 mm 2 . Under this circumstance, by adding GaF3, the spreading area of Zn-15Al filler metal over Q235 steel was increased by 104% comparing to that of CsF-AlF3 flux (92 mm 2 ) and by 17.5% comparing to the addition of Ga2O3.

The Mechanism of Interfacial Reaction
The CsF-AlF3-GaF3 flux could effectively improve the spreadability of Zn-15Al filler metal over 6061 aluminum alloy and Q235 steel, but how it worked was not clear yet and deserved a detailed investigation. Therefore, the theory of interfacial tension was applied reasonably to confirm some potential explanations. On the basis of the Young's equation illustrated by Figure 3 and Equation (1), the liquid balance over solid surface was determined by the interfacial tensions between solids, liquids and gases. Specifically, these interfacial tensions could be summed up as between base metal and molten flux (γSF), molten filler metal and molten flux (γLF) and base metal and molten filler metal (γSL) in this study.
Non-reactive wetting and reactive wetting were two approaches to wetting a solid with molten metal, and the interfacial tension between the base metal and molten filler metal (γSL) decreased due to the reaction and the spreading was improved. Because the molted flux reacted with the surface metallic oxides over the base metal and removed them, the reactive wetting was what we discussed in this research. While balancing, the relationship of interfacial tensions is shown as Equation (1).
Alumina reacted with melted XF-AlF3 (X = Na, K, Rb, Cs) flux and formed AlF3 to be dissolved, and the interfacial tension of solid-liquid (γSL) changed from Zn-Al alloy-alumina to Zn-Al alloyaluminum [13]. The remarkable intersolubility of Zn and Al made the interfacial tension between Non-reactive wetting and reactive wetting were two approaches to wetting a solid with molten metal, and the interfacial tension between the base metal and molten filler metal (γ SL ) decreased due to the reaction and the spreading was improved. Because the molted flux reacted with the surface metallic oxides over the base metal and removed them, the reactive wetting was what we discussed in this research. While balancing, the relationship of interfacial tensions is shown as Equation (1).
Alumina reacted with melted XF-AlF 3 (X = Na, K, Rb, Cs) flux and formed AlF 3 to be dissolved, and the interfacial tension of solid-liquid (γ SL ) changed from Zn-Al alloy-alumina to Zn-Al alloy-aluminum [13]. The remarkable intersolubility of Zn and Al made the interfacial tension between AA6061 and Zn-15Al alloy (γ SL ) decrease rapidly and the spreading area of Zn-15Al alloy over AA6061 increased significantly under this condition. However, no research has reported that the CsF-AlF 3 -based flux could react with iron oxide immediately and the surface oxide was still the largest obstacle. The phase diagram of Fe-Zn showed that intermetallics, such as FeZn and FeZn 4 , formed below 600 • C. It could be included that the Zn-15Al filler metal spread over Q235 steel made γ' SL decreased gradually by the reaction of Zn and Fe.
The wetting angles of different fluxes over AA6061 are shown in Table 3. Molten Zn-Al filler metal wetted AA6061 alloy and Q235 steel and spread on the base metal, which reduced the γ SL shown in Equation (2) and the balance of Young's equation was broken. The new flux breaks the tension balance of the original interface and thus the spreading area of Zn-15Al is promoted with the addition of GaF 3 . Ga 3+ ion in GaF 3 has a "skin effect", which is analogous to the chemical representation of a thin layer of electrical current concentrated on the outer surface of a conductor, and its small surface tension can significantly reduce γ SL . Due to the enrichment of Ga 3+ ions, γ SL decreases rapidly, while the spreading area of the liquid filler metal increases further. However, with the consumption of liquid flux, the ability to remove the Al 2 O 3 oxide film gradually weakens and finally the reactivity disappears. The interfacial tension (γ SF ) between the base metal and flux decreases. The equilibrium of interfacial tension in Equation (1) is reassumed. The spreading area of filler metal attains saturation and the spreading shape is fixed. Table 3. Wetting angles of different fluxes.

Flux CsF-AlF 3 CsF-AlF 3 -Ga 2 O 3 CsF-AlF 3 -GaF 3
Wetting It could be demonstrated that Ga 3+ was released from GaF 3 , whose reaction equation was Equation (3), considering the activity of molten Zn-15Al filler metal. Ga could permeate into the molten filler metal spontaneously with its similar chemical property to Al. The EDX (Energy Dispersive X-ray Spectroscopy) results are shown in Figure 4, and it can be seen that in the interface of base metal and filler metal, a weak peak of Ga appeared. Original balance was broken and the spreading area increased significantly because of the decrease in γ SL . The diagrammatic sketch of the interfacial tension of spread Zn-Al filler metal is shown as Figure 5.
Crystals 2020, 10, x FOR PEER REVIEW 5 of 10 AA6061 and Zn-15Al alloy (γSL) decrease rapidly and the spreading area of Zn-15Al alloy over AA6061 increased significantly under this condition. However, no research has reported that the CsF-AlF3-based flux could react with iron oxide immediately and the surface oxide was still the largest obstacle. The phase diagram of Fe-Zn showed that intermetallics, such as FeZn and FeZn4, formed below 600 °C. It could be included that the Zn-15Al filler metal spread over Q235 steel made γ'SL decreased gradually by the reaction of Zn and Fe. The wetting angles of different fluxes over AA6061 are shown in Table 3. Molten Zn-Al filler metal wetted AA6061 alloy and Q235 steel and spread on the base metal, which reduced the γSL shown in Equation (2) and the balance of Young's equation was broken. The new flux breaks the tension balance of the original interface and thus the spreading area of Zn-15Al is promoted with the addition of GaF3. Ga 3+ ion in GaF3 has a "skin effect", which is analogous to the chemical representation of a thin layer of electrical current concentrated on the outer surface of a conductor, and its small surface tension can significantly reduce γSL. Due to the enrichment of Ga 3+ ions, γSL decreases rapidly, while the spreading area of the liquid filler metal increases further. However, with the consumption of liquid flux, the ability to remove the Al2O3 oxide film gradually weakens and finally the reactivity disappears. The interfacial tension (γSF) between the base metal and flux decreases. The equilibrium of interfacial tension in Equation (1) is reassumed. The spreading area of filler metal attains saturation and the spreading shape is fixed. It could be demonstrated that Ga 3+ was released from GaF3, whose reaction equation was Equation (3), considering the activity of molten Zn-15Al filler metal. Ga could permeate into the molten filler metal spontaneously with its similar chemical property to Al. The EDX (Energy Dispersive X-Ray Spectroscopy) results are shown in Figure 4, and it can be seen that in the interface of base metal and filler metal, a weak peak of Ga appeared. Original balance was broken and the spreading area increased significantly because of the decrease in γSL. The diagrammatic sketch of the interfacial tension of spread Zn-Al filler metal is shown as Figure 5.  The XRD results of the flux residue were shown in Figure 6. It revealed the residue products over AA6061 were MgMnSi2O6, Al2SiO5, MgSiO3, Zn2SiO4, CuO, Cu4O3, Al2O3, Cs11O3, AlF3, MnF2 and ZnGa2O4, and which were Al2SiO5, Fe2SiO4, AlPO4, FePO4, Al2O3, ZnO, SiO2, AlF3, MnF2 and MnAlF5 over Q235 steel.
The compounds over AA6061 surface were mainly made up of Mg2Si, MgO, MgAl2O4, amorphous Al2O3 and a little Cu, Mn, Cr, Fe according to report [14]. The content of Mg, Mn and Si increased while over 520 °C. Figure 6 reveals that the Cs11O3, silicate and fluoride came from the reaction between the oxide and flux. It could be confirmed that ZnGa2O4 arose from the residue of the trace amounts of GaF3 in the flux. It was reported [15] the additional Ga tended to enrich on the surface, which led to the speculation that GaF3 might be involved in some kind of reaction. Because of this, ZnGa2O4 was validated to show its diffraction peaks in the XRD pattern, whose reaction equation is Equation (4).
The mechanism for alumina removal from CsF-AlF3 flux was the dissolution and reaction of the active ingredients such as F − , HF, SiF6 2− and Zn 2+ ions. Zn 2+ and SiF6 2− ions were liable to be generated during the spreading test because of the massive amount of Zn in the filler metal and a little Si on the base metal surface. The major flux reaction is listed in Equation (5), which refers to the flux with the addition of Ga2O3 nanoparticles. In addition, trace amounts of H2O, NH4F and NH4AlF4 appeared in the CsF-AlF3-GaF3 flux, which produced HF and further promoted the removal. According to Figure 6, the XRD result of residue over Q235 steel was not the same as that in AA6061. Research showed that Fe2O3, Fe3O4 and FeO were distributed systematically on Q235 steel [16]. Thus, the removal of iron oxide was the primary step. According to the XRD result shown in Figure 6, the reaction of SiO2, iron oxide and alumina formed Fe2SiO5 and Al2SiO5. MnF2 and MnAlF5 were formed by the reaction between F − , HF, Mn compounds and AlF3. However, the appearance of The compounds over AA6061 surface were mainly made up of Mg 2 Si, MgO, MgAl 2 O 4 , amorphous Al 2 O 3 and a little Cu, Mn, Cr, Fe according to report [14]. The content of Mg, Mn and Si increased while over 520 • C. Figure 6 reveals that the Cs 11 O 3 , silicate and fluoride came from the reaction between the oxide and flux. It could be confirmed that ZnGa 2 O 4 arose from the residue of the trace amounts of GaF 3 in the flux. It was reported [15] the additional Ga tended to enrich on the surface, which led to the speculation that GaF 3 might be involved in some kind of reaction. Because of this, ZnGa 2 O 4 was validated to show its diffraction peaks in the XRD pattern, whose reaction equation is Equation (4).
The mechanism for alumina removal from CsF-AlF 3 flux was the dissolution and reaction of the active ingredients such as F − , HF, SiF 6 2− and Zn 2+ ions. Zn 2+ and SiF 6 2− ions were liable to be generated during the spreading test because of the massive amount of Zn in the filler metal and a little Si on the base metal surface. The major flux reaction is listed in Equation (5), which refers to the flux with the addition of Ga 2 O 3 nanoparticles. In addition, trace amounts of H 2 O, NH 4 F and NH 4 AlF 4 appeared in the CsF-AlF 3 -GaF 3 flux, which produced HF and further promoted the removal. According to Figure 6, the XRD result of residue over Q235 steel was not the same as that in AA6061. Research showed that Fe 2 O 3 , Fe 3 O 4 and FeO were distributed systematically on Q235 steel [16]. Thus, the removal of iron oxide was the primary step. According to the XRD result shown in Figure 6, the reaction of SiO 2 , iron oxide and alumina formed Fe 2 SiO 5 and Al 2 SiO 5 . MnF 2 and MnAlF 5 were formed by the reaction between F -, HF, Mn compounds and AlF 3 . However, the appearance of a trifle phosphate, FePO 4 and AlPO 4 in the XRD result led to the conclusion that FePO 4 and AlPO 4 were formed as Equation (9), under the condition that no phosphorus was contained in the flux and its content was below 0.04 wt.% in Q235 steel.
Because the content of phosphorus in Q235 could not be detected by the XRD, it meant that P enriched over Q235 surface, which was a normal phenomenon occurring when heating P-containing alloys such that the phosphorus was burnt out, producing phosphorus oxide. Although the existence of P removed a little of the metallic oxide, it was insufficient to remove all oxide films. Therefore, it was clear that the main reaction mechanism of removing metallic oxides referred to the reaction between Al and iron oxide as Equation (10).
Because of the large concentration of Al and Zn elements in the Zn-Al filler metal, the surface oxide film of the filler metal and Q235 steel is prone to react and the oxide film can be effectively removed. Fe, Cr, Ni and other elements obtained by the reaction were then rapidly dissolved into Q235 steel base material, so Al 2 O 3 and ZnO were detected in large quantities in the reaction residue, which reasonably explained the XRD results in Figure 6. 36CsF + 2SiO 2 + 6HF + 5MnO → 2Cs 11 O 3 + 2Cs 2 SiF 6 + 5Cs 2 MnF 6 + 3H 2 O ↑ Crystals 2020, 10, 498 8 of 10 The reaction shown in Equation (11) explains the decrease in the flux activity due to the huge consumption of the CsF and its lowered flowability. The formation of Ga 3+ enhanced the spreadability of Zn-15Al filler metal while leading to less activity.
According to the proposed mechanisms, molten flux reacted with oxide and the spread of filler metal was promoted simultaneously. Nevertheless, the efficiency of alumina removal was decreased by the rapid effective loss of molten flux and the spreading speed of Zn-15Al was further delayed. The reason could be the consumption of active substances such as SiF 6 2-, HF and F -, and the production of silicates. Different from the lower efficiency of CsF-AlF 3 flux on iron deoxidation, the addition of GaF 3 significantly improved the activity on account of the enrichment and production of Ga 3+ , and thus decreased the interfacial tension between base metal and Zn-15Al [17]. In addition, the dissolving reaction between GaF 3 with ZnO occurred and consequently the spreading of molten Zn-15Al was further promoted.
Instead of reacting and producing Ga 3+ for the addition of GaF 3 , Ga 2 O 3 tends to react with ZnO to produce ZnGa 2 O 4 according to Equation (5). Meanwhile, when nano-Ga 2 O 3 particles were added into the flux as a chemical agent, Ga element can only be released by the reaction of Zn-Al alloy and Ga 2 O 3 particles. As a typical spinel oxide, ZnGa 2 O 4 belongs to a cubic crystal system and the chemical stability and thermal stability are very high [18]. Accordingly, more energy is needed to separate Ga from Ga 2 O 3 . The formation of ZnGa 2 O 4 somehow facilitates the release of active substances, such as F and Al, which remove the oxide film on the surface of the 6061 Al alloy and the Q235 steel.
Combining the above issues with the XRD results shown in Figure 6, it was speculated that the main reactions are shown as Equations (3)- (11). The formation of active substances such as SiF 6 2− , HF and Fhelped the molten flux remove the surface oxide over AA6061, and the iron oxide over Q235 steel was removed by active Al in the filler metal and enriched element P, which led to the improvement in the spreadability of molten Zn-15Al on the base metal.

Comparative Analysis on the Effect of GaF 3 and Ga 2 O 3 Addition
Combined with the analysis of the enhancement mechanism of doping Ga 2 O 3 nanoparticles into the flux in a previous study [12], it can be concluded that surface-active Ga obtained from the reaction of the flux and base metals during brazing plays a major enhancement role in promoting the spreading of Zn-Al filler metal on the base metal.
As an ionic compound, GaF 3 consists of cations Ga 3+ and anions F − , which means Ga 3+ and F − ions can be dissociated more easily from GaF 3 than Ga 2 O 3 when heated. The dissociation product Ga 3+ can rapidly and effectively reduce the interfacial tension between the Zn-15Al filler metal and the base metal to further promote the spreadability of the filler metal. In addition, the synergistic effect of GaF 3 can promote the surface enrichment of P element according to the above "skin effect" and partially remove the surface oxide film of Q235 carbon steel, which further improve the spreadability of the filler metal. Meanwhile when nano-Ga 2 O 3 particles were added into the flux as a chemical agent, Ga can only be released by the reaction of Zn-Al alloy and Ga 2 O 3 particles. Therefore, compared with GaF 3 , more energy is needed to separate Ga from Ga 2 O 3 during brazing.
Compared with the results of previous analysis [12,19], the addition of GaF 3 and Ga 2 O 3 in this study increases the spreading area of the filler metal on both 6061 aluminum alloy and Q235 steel, and the flux bearing GaF 3 has better activity than that bearing Ga 2 O 3 .

Conclusions
In this study, trace amounts of GaF 3 and Ga 2 O 3 nanoparticles were respectively added into CsF-AlF 3 flux for brazing aluminum to carbon steels. The effects of these two nanoparticles on the flux activity and the spreadability of Zn-15Al filler metal on the base metal were comparatively investigated. The major conclusions were as follows: Crystals 2020, 10, 498 9 of 10 (1) The spreading tests showed that with the addition of trace amounts of GaF 3 and Ga 2 O 3 in CsF-AlF 3 flux, the spreadability of Zn-15Al filler metal both on Q235 steel and AA6061 alloy was effectively improved, and the enhancement effect of GaF 3 was more obvious. The optimal contents of GaF 3 and Ga 2 O 3 were 0.0075-0.01 wt.% and 0.009-0.01 wt.%, respectively. (2) The "skin effect" of GaF 3 improved the activity of fluxes by reacting with Al atoms to produce Ga 3+ , and enrichment of Ga 3+ on molten filler metal decreased the interfacial tension and enlarged the spreading area of molten Zn-15Al filler metal on the base metals. (3) In addition, as an ionic compound, GaF 3 could easily react and generate Ga 3+ to promote the enrichment of P element in the base metal to remove the oxide film on Q235 carbon steel and promote the wetting of the filler metal. Therefore, the activity of CsF-AlF 3 flux with the addition of GaF 3 was higher than that with the addition of Ga 2 O 3 .