Zirconium arc melting parameters and process conditions are shown in Tables 1 to 3. Table 1 Zirconium vacuum consumable melting parameters å©åŸš diameter / cm twenty two twenty two Electrode diameter / cm 15 16 Smelting times 1 2 Arcing current / kA 3.5 3.5 Smelting current / kA 4.5 7.0 to 7.5 Current density / A · cm - 2 (by å©åŸš section) 11.8 18.2 to 19.7 Melting voltage / V 33～35 34~38 Stable arc magnetic field / A · åŒ 1.5×1800 1.5×1800 Vacuum degree / kPa (1.3 to 6.7) × 10 - 4 (1.3 to 6.7) × 10 - 4 Air leak rate / kPa · min - 1 ≤6.7×10 - 5 ≤6.7×10 - 5 Table 2 Relationship between melting voltage, current and electrode diameter during arc melting of zirconium consumable electrode Electrode diameter / cm 5.08 7.62 10.16 12.70 15.24 17.78 20.39 22.86 25.4 Melting voltage / V 25 28 30 40 40 40 40 40 40 Smelting current / kA 0.8 1 0.8 2.5 3.5 4 4.5 5 5.5 Table 3 Zirconium arc melting process conditions project Non-consumable method Self-consumption Consumable remelting Electrode size / cm Diameter 1.27 ~ 1.90 Length 1.9 to 3.8 (tungsten or tungsten coated with 1% to 2% ThO 2 ) 5.08×5.08×50.8 Diameter 15.2 å©åŸš size / cm Inner diameter 10.2 Inner diameter 15.2 Wall thickness 0.635～1.587 Inner diameter 25.4 Cooling water flow rate of cooling copper crucible / L · min - 1 302 atmosphere/% 80He+20Ar 80He+20Ar 80He+20Ar Pressure / kPa 101.3 101.3 0.067～0.4 Melting voltage / V 50 45 35 Smelting current / kA 1.1 3 6 Zirconium melting speed / kg · h - 1 5.4 108 270 1kg zirconium electricity consumption / kW · h 10.2 1.23 0.77 The main equipment for arc melting is shown in Figures 1 to 3. Figure 1 Multi-furnace non-consumable electrode arc furnace 1-negative joint; 2-vacuum pressure gauge; 3-observation port; 4-insulating ring; 5-water-cooled six-inch; 6- mica support; 7-rotary handle; 8-inch cooling water pipe; Positive electrode joint; 10- vacuum pump valve; 11-clam pot mixed gas valve; 12-tungsten electrode head; 13-vacuum pipe; 14-cooling water pipe; 15-electrode; 16-water-cooled electrode Figure 2 Schematic diagram of consumable electrode arc furnace 1-backup electrode; 2-welding box; 3-welding rail; 4-plate glass; 5-rubber glove; 6-welding wire; 7-gearbox; 8-steel roll; 9-hand crank; 10-arc Power supply wire (cathode); 11-copper contact roll; 12-insulation; 13-water jacket; 14-zirconium ingot; 15-water inlet; 16-water outlet; 17-arc power supply wire (anode); Window; 19-zirconium ingot transport trolley Figure 3 consumable electrode remelting electric arc furnace 1-electrode cooling water; 2-electrode joint (cathode); 3-observation window; 4-assembly inlet and outlet; 5-vacuum pipe joint; 6-power joint; 7-water jacket; 8-zirconium ingot; Insulating ring; 10--operating car The electron beam is a very pure source of high-energy, electron beam melting in a high vacuum (less than 1.3 × 10 - 5 kPa) for the lower, so the melting metals to achieve highly efficient purification. By adjusting the electron beam orientation, any part of the material to be smelted can be heated. Electron beam melting has no mechanical action on the molten pool, does not blow the molten pool, and can melt materials of various shapes. Purification mechanism of electron beam melting: first, evaporation by alloy components, and second, evaporation and deoxidation of base metal suboxides. The various parameters for electron beam melting are shown in Figure 4 and Table 4. Figure 4 Relationship between power required for electron beam melting and metal melting point and ingot diameter 1-960kW; 2-480kW; 3-240kW; 4-120kW; 5-60kW; 6-30kW Table 4 Trend of deoxidation of metals (represented by the vapor pressure ratio of metal to its oxide) Deoxygenated Not deoxidizing The electron beam melting furnace is shown in Fig. 5. The comparison between the melting method and the vacuum sintering method is shown in Table 5. Figure 5 Schematic diagram of NRC electron beam furnace melting furnace 1-cathode; 2-accelerated anode; 3-electron gun chamber; 4-focus coil; 5- spacer; 6-4in gate valve; 7-melting chamber; 8-ion vacuum gauge; 9-vibration feeder ; 10 - water-cooled copper crystallizer; 11 - puller; 12 - pull down; 13 - zirconium ingot; 14 - 10in oil diffusion pump; 15 - peep window; 16 - electron beam; 17 - 4in oil diffusion pump; 18-water cooling coil Table 5 Electron beam melting on a productive scale, vacuum arc Comparison of smelting (self-consumption electrode) and vacuum sintering Comparison project Electron beam melting Vacuum arc melting Vacuum sintering Remarks Starting material (material to be melted) When the drop method is used, the material to be smelted must be made into a consumable electrode type. When using the molten pool smelting method, the feeding form is arbitrary: sponge, powder, granule, and the like. In the case of smelting for casting, even large pieces of waste can be added to the charge. Materials with high gas content should be pre-vacuum degassed The material to be smelted must be made into a consumable electrode. Limited possibilities for smelting waste Only powder can be applied. When using waste, the waste must be powdered first. Electron beam melting method is the most superior Ingot size It is easy to smelt long and medium-section long ingots. For large-section ingots, the melting equipment is expensive (the vacuum pump needs to have a large exhaust speed) Can easily smelt ingots of any reasonable size Sintering of small ingots (10 to 20 kg) is easy. For medium-sized ingots, (1) large presses, sometimes hydraulic presses are available; (2) high energy must be supplied to keep the entire ingot at the sintering temperature. Vacuum arc melting is the most superior Insulation power consumption Varying with smelting speed Minimal power required Because the sintering efficiency (similar to the smelting speed) is extremely low, the energy required is extremely high. The reason is that the diffusion of impurities to the surface is extremely slow and takes a long time; the entire ingot must reach the sintering temperature; sometimes secondary sintering is required. Vacuum arc melting is the most superior Pressure in the melting chamber Any small pressure can be achieved. Usually around 4 × 10 - 5 ~ 10 - 6 kPa (related to metal gas content, pump capacity and melting method) It is best to use a pressure of 6.7 × 10 - 3 to 10 - 4 kPa, and the pressure is low and useless. Any small pressure can be achieved. Normal sintered 1.3 × 10 - 7 kPa pressure at - 5 ~ 6.7 × 10 Electron beam melting is as beneficial as vacuum sintering Processing time medium least most Vacuum arc melting is most beneficial Annual production medium maximum Minimum Vacuum furnace smelting is most beneficial Degree of metal purification Best (reason: high vacuum, highest temperature reached, long metal in molten state) Worst (lower vacuum, lower temperature than electron beam melting, shorter time in molten state) The purity obtained by electron beam melting is poor, but it is still good (high vacuum, long sintering time, lowest temperature) E-beam smelting is superior Grain size Very coarse (since the melting rate is small, the metal purity is high) Thick, but still much thinner than electron beam melting Very fine (because of the powder as the starting material) Sintered grain is the finest Recent research results on smelting and refining methods of zirconium include: rotating electrode smelting high-purity metal zirconium (non-consumable rotating water-cooled copper electrode, water-cooled copper crucible, vacuum); electroslag smelting of zirconium; recrystallization of zirconium in vacuum region; electrode Zirconium is transported and purified (Principle: When direct current is applied at high temperature, the solute atoms migrate under the action of an external electric field, and the migration of oxygen, nitrogen and carbon is the same as the direction of electron flow. The raw material used is zirconium smelted in the electron beam region, and the degree of vacuum (1) ～2)×10 - 8 Pa, temperature 1402～1627°C); BB Suming (Cy MNH ) measures the transfer coefficient of titanium and iron when zirconium is smelted in the electron beam region, the transfer coefficient of iron is 0.29±0.06, and the transfer of titanium The coefficient is 0.48±0.15. The literature studies the absorption of gas phase impurities in the regional refined zirconium process. It is found that the rate of oxygen absorption is extremely fast. The absorption depends on the partial pressure, the moving speed of the melting zone and the number of melting times. It has been found that oxygen is in the zirconium solution ( Solubility in oxygen: metal <0.1) follows Henry's law. Choosing the right Swivel can help you clean it more easily,we provide 350 Bar Swivel,5000 PSI Swivel. 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