Method for producing metal or ceramic components and components
US-2019070818-A1 · Mar 7, 2019 · US
US11584101B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11584101-B2 |
| Application number | US-201916719357-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 18, 2019 |
| Priority date | Feb 13, 2017 |
| Publication date | Feb 21, 2023 |
| Grant date | Feb 21, 2023 |
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An apparatus includes a first electrode exhibiting a first Seebeck coefficient, a second electrode exhibiting a second Seebeck coefficient greater than the first Seebeck coefficient, and particles between the first and second electrodes exhibiting a third Seebeck coefficient between the first and second Seebeck coefficients. An alternating current power supply is electrically connected to the first and second electrodes. Heat is generated due to the Peltier effect at a junction between the first electrode and the particles and at a junction between the second electrode and the particles. Heat is removed due to the Peltier effect at the junction between the first electrode and the particles and at the junction between the second electrode and the particles. The particles are densified due to heating and cooling phase transitions between a higher-temperature solid phase and a lower-temperature solid phase while compressing the particles.
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What is claimed is: 1. An apparatus comprising: a first electrode exhibiting a first Seebeck coefficient and a second electrode exhibiting a second Seebeck coefficient greater than the first Seebeck coefficient; a die cavity between the first electrode and the second electrode such that electrically conductive particles, when placed therein, contact the first electrode and the second electrode and provide a conductive path between the first and second electrodes; an alternating current power supply electrically connected to the first electrode and to the second electrode, the power supply having a variable frequency; the power supply being configured to apply an electric current from the second electrode through the particles to the first electrode or to apply the electric current from the first electrode through the particles to the second electrode; the power supply being configured to allow producing a sufficient current frequency and a sufficient current amount to generate Peltier effect heating and Peltier effect cooling, depending on the direction of current flow, at a junction between the first electrode and the particles and at a junction between the second electrode and the particles, the sufficiency of the current frequency depending on a distance between the first and second electrodes through the particles, wherein the sufficient current comprises 1-15 amp/mm 2 at the junction between the first electrode and the particles and at the junction between the second electrode and the particles; and a compaction press configured to allow sufficient compression of the particles when the alternating electric current is applied to densify the particles due to heating and cooling phase transitions while compressing the particles. 2. The apparatus of claim 1 , wherein the second Seebeck coefficient is greater than the first Seebeck coefficient by 5 μV/K or greater when measured at 20° C. 3. The apparatus of claim 1 , wherein the first electrode consists essentially of molybdenum or tungsten at the junction between the first electrode and the particles and/or the second electrode consists essentially of palladium, graphite, or constantan at the junction between the second electrode and the particles. 4. The apparatus of claim 1 , wherein the sufficient current frequency is matched to a distance between the electrodes and, wherein the sufficient compression comprises less than 7 ksi as applied by the first and/or second electrode on the particles. 5. The apparatus of claim 1 , wherein the first electrode is parallel to the second electrode. 6. The apparatus of claim 1 , further comprising a first side wall and a second side wall, wherein the die cavity is formed between the first side wall, the first electrode, the second side wall, and the second electrode. 7. The apparatus of claim 6 , wherein the alternating current power supply is electrically connected to the first electrode and to the second electrode via connecting wires, wherein a portion of the connecting wires passes through a slot in the first side wall. 8. The apparatus of claim 7 , wherein the portion of the connecting wires that passes through the slot is a flexible portion of wire. 9. The apparatus of claim 1 , further comprising a first thermal block positioned adjacent to the first electrode, wherein the first thermal block is heated by a thermal element. 10. The apparatus of claim 9 , further comprising a second thermal block positioned adjacent to the second electrode, wherein the second thermal bock is heated by a thermal element. 11. The apparatus of claim 1 , wherein the particles contain greater than 50 weight % titanium. 12. An apparatus comprising: a first electrode exhibiting a first Seebeck coefficient and a second electrode exhibiting a second Seebeck coefficient greater than the first Seebeck coefficient; a die cavity between the first electrode and the second electrode such that electrically conductive particles, when placed therein, contact the first electrode and the second electrode and provide a conductive path between the first and second electrodes; an power supply electrically connected to the first electrode and to the second electrode, wherein the power supply is a direct current (DC) power supply; the power supply being configured to allow selectively changing a direction of current flow to apply an electric current from the second electrode through the particles to the first electrode or to apply the electric current from the first electrode through the particles to the second electrode; the power supply being configured to allow producing a sufficient current frequency and a sufficient current amount to generate Peltier effect heating and Peltier effect cooling, depending on the direction of current flow, at a junction between the first electrode and the particles and at a junction between the second electrode and the particles, the sufficiency of the current frequency depending on a distance between the first and second electrodes through the particles, wherein the sufficient current comprises 1-15 amp/mm 2 at the junction between the first electrode and the particles and at the junction between the second electrode and the particles; and a compaction press configured to allow sufficient compression of the particles when the alternating electric current is applied to densify the particles due to heating and cooling phase transitions while compressing the particles. 13. The apparatus of claim 12 , wherein the DC power supply is coupled to with polarity switch to allow selectively change the direction of current flow. 14. The apparatus of claim 13 , wherein the polarity switch is a bipolar amplifier. 15. The apparatus of claim 12 , wherein the second Seebeck coefficient is greater than the first Seebeck coefficient by 5 μV/K or greater when measured at 20° C. 16. The apparatus of claim 12 , wherein the first electrode consists essentially of molybdenum or tungsten at the junction between the first electrode and the particles and/or the second electrode consists essentially of palladium, graphite, or constantan at the junction between the second electrode and the particles. 17. The apparatus of claim 12 , wherein the sufficient current frequency is matched to a distance between the electrodes. 18. The apparatus of claim 12 , wherein the sufficient compression comprises less than 7 ksi as applied by the first and/or second electrode on the particles. 19. The apparatus of claim 12 , wherein the particles contain greater than 50 weight % titanium. 20. The apparatus of claim 12 , further comprising a first thermal block positioned adjacent to the first electrode, wherein the first thermal block is heated by a first thermal element and a second thermal block positioned adjacent to the second electrode, wherein the second thermal block is heated by a second thermal element.
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