The disclosure is directed to Fe—Cr—Mo—Ni—P—C—B metallic glasses having a high glass forming ability and a high thermal stability of the supercooled liquid against crystallization.
U.S. Pat. Nos. 8,529,712 and 8,911,572 entitled “Tough Iron-Based Bulk Metallic Glass Alloys,” the disclosures of which is incorporated herein by reference in their entirety, disclose Fe-based glass forming alloys comprising at least P, C, and B demonstrating a critical rod diameter of at least 2 mm and a shear modulus of less than 60 GPa, where the Fe atomic concentration is at least 60 percent, the P atomic concentration varies in the range of 5 to 17.5 percent, the C atomic concentration varies in the range of 3 to 6.5 percent, and the B atomic concentration varies in the range of 1 to 3.5 percent. The patents also disclose that the Fe-based alloys may optionally comprise Mo in an atomic concentration varying in the range of 2 to 8 percent, Cr in an atomic concentration varying in the range of 1 to 7 percent, and Ni in an atomic concentration varying in the range of 3 to 7 percent. The patents present several examples of amorphous Fe—P—C—B alloys that comprise Mo, Cr, and Ni demonstrating a critical rod diameter of up to 6 mm and a thermal stability of the supercooled liquid (i.e. a difference between the crystallization and glass transition temperatures at a heating rate of 20 K/min) of under 40° C.
The description will be more fully understood with reference to the following figures and data graphs, which are presented as various embodiments of the disclosure and should not be construed as a complete recitation of the scope of the disclosure, wherein:
The disclosure provides Fe—Cr—Ni—Mo—P—C—B metallic glass-forming alloys and metallic glasses that have a high glass forming ability along with a high thermal stability of the supercooled liquid against crystallization.
In one embodiment, the disclosure provides a metallic glass-forming alloy or a metallic glass having a composition represented by the following formula (subscripts denote atomic percentages):
Fe(100-a-b-c-d-e-f)CraNibMocPdCeBf EQ. (1)
In another embodiment of the metallic glass-forming alloy or metallic glass, a is up to 9, b ranges from 4 to 12, c ranges from 3 to 6.5, d+e+f ranges from 21.5 to 23.5, e ranges from 5.25 to 7.5, f ranges from 1.5 to 8.5, wherein the metallic glass-forming alloy has a critical rod diameter of at least 4 mm, and wherein the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 47.5° C.
In another embodiment of the metallic glass-forming alloy or metallic glass, a is up to 8, b ranges from 4.5 to 10, c ranges from 3.5 to 5.5, d+e+f ranges from 21.5 to 23, e ranges from 5.5 to 7, f ranges from 2 to 7.5, wherein the metallic glass-forming alloy has a critical rod diameter of at least 5 mm, and wherein the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 50° C.
In another embodiment of the metallic glass, a is less than 3.5, and wherein the critical bending diameter of the metallic glass is at least 0.5 mm.
In another embodiment of the metallic glass, a is less than 2.5, and wherein the critical bending diameter of the metallic glass is at least 0.6 mm.
In another embodiment of the metallic glass, a is less than 1.75, and wherein the critical bending diameter of the metallic glass is at least 0.7 mm.
In another embodiment of the metallic glass, a is less than 1.25, and wherein the critical bending diameter of the metallic glass is at least 0.8 mm.
In another embodiment of the metallic glass, c ranges from 2 to less than 6.5, and wherein the critical bending diameter of the metallic glass is at least 0.6 mm.
In another embodiment of the metallic glass, c ranges from 2 to less than 5.5, and wherein the critical bending diameter of the metallic glass is at least 0.7 mm.
In another embodiment of the metallic glass, c ranges from 2 to less than 4.25, and wherein the critical bending diameter of the metallic glass is at least 0.8 mm.
In another embodiment of the metallic glass, d+e+f ranges from 21.25 to less than 23.5, and wherein the critical bending diameter of the metallic glass is at least 0.6 mm.
In another embodiment of the metallic glass, d+e+f ranges from 21.25 to less than 22.75, and wherein the critical bending diameter of the metallic glass is at least 0.7 mm.
In another embodiment of the metallic glass, e ranges from greater than 5.25 to 8, and wherein the critical bending diameter of the metallic glass is at least 0.8 mm.
In another embodiment of the metallic glass, e ranges from greater than 6.75 to 8, and wherein the critical bending diameter of the metallic glass is at least 0.9 mm.
In another embodiment of the metallic glass, f ranges from 1 to less than 5, and wherein the critical bending diameter of the metallic glass is at least 0.5 mm.
In another embodiment of the metallic glass, f ranges from 1 to less than 4.5, and wherein the critical bending diameter of the metallic glass is at least 0.6 mm.
In another embodiment of the metallic glass, f ranges from 1 to less than 3, and wherein the critical bending diameter of the metallic glass is at least 0.7 mm.
In another embodiment of the metallic glass, f ranges from 1 to less than 2.5, and wherein the critical bending diameter of the metallic glass is at least 0.8 mm.
In another embodiment of the metallic glass-forming alloy or metallic glass, a ranges from 1 to 6.
In another embodiment of the metallic glass-forming alloy or metallic glass, a ranges from 1 to 5.
In another embodiment of the metallic glass-forming alloy or metallic glass, a ranges from 1 to 4.
In another embodiment of the metallic glass-forming alloy or metallic glass, a ranges from 1 to 3.
In another embodiment of the metallic glass-forming alloy or metallic glass, a ranges from 1 to 2.
In another embodiment of the metallic glass-forming alloy or metallic glass, b ranges from 4 to 11.
In another embodiment of the metallic glass-forming alloy or metallic glass, b ranges from 5 to 10.
In another embodiment of the metallic glass-forming alloy or metallic glass, b ranges from 6 to 10.
In another embodiment of the metallic glass-forming alloy or metallic glass, b ranges from 7 to 10.
In another embodiment of the metallic glass-forming alloy or metallic glass, b ranges from 8 to 10.
In another embodiment of the metallic glass-forming alloy or metallic glass, c ranges from 2.5 to 6.5.
In another embodiment of the metallic glass-forming alloy or metallic glass, c ranges from 3 to 6.
In another embodiment of the metallic glass-forming alloy or metallic glass, c ranges from 3.5 to 5.5.
In another embodiment of the metallic glass-forming alloy or metallic glass, c ranges from 3.75 to 5.25.
In another embodiment of the metallic glass-forming alloy or metallic glass, c ranges from 3.75 to 5.
In another embodiment of the metallic glass-forming alloy or metallic glass, c ranges from 3.75 to 4.75.
In another embodiment of the metallic glass-forming alloy or metallic glass, d+e+f ranges from 21.25 to 23.5.
In another embodiment of the metallic glass-forming alloy or metallic glass, d+e+f ranges from 21.5 to 23.
In another embodiment of the metallic glass-forming alloy or metallic glass, d+e+f ranges from 21.75 to 22.75.
In another embodiment of the metallic glass-forming alloy or metallic glass, e ranges from 5 to 7.75.
In another embodiment of the metallic glass-forming alloy or metallic glass, e ranges from 5.25 to 7.5.
In another embodiment of the metallic glass-forming alloy or metallic glass, e ranges from 5.25 to 7.25.
In another embodiment of the metallic glass-forming alloy or metallic glass, e ranges from 5.25 to 7.
In another embodiment of the metallic glass-forming alloy or metallic glass, e ranges from 5.25 to 6.75.
In another embodiment of the metallic glass-forming alloy or metallic glass, e ranges from 5.5 to 6.5.
In another embodiment of the metallic glass-forming alloy or metallic glass, f ranges from 2 to 5.
In another embodiment of the metallic glass-forming alloy or metallic glass, f ranges from 2 to 4.
In another embodiment of the metallic glass-forming alloy or metallic glass, f ranges from 2 to 3.
In another embodiment, the metallic glass-forming alloy has a critical rod diameter of at least 4 mm.
In another embodiment, the metallic glass-forming alloy has a critical rod diameter of at least 5 mm.
In another embodiment, the metallic glass-forming alloy has a critical rod diameter of at least 6 mm.
In another embodiment, the metallic glass-forming alloy has a critical rod diameter of at least 7 mm.
In another embodiment, the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 51° C.
In another embodiment, the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 52° C.
In another embodiment, the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 53° C.
In another embodiment, the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 54° C.
In another embodiment, the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 55° C.
In another embodiment, the critical bending diameter of the metallic glass is at least 0.5 mm.
In another embodiment, the critical bending diameter of the metallic glass is at least 0.6 mm.
In another embodiment, the critical bending diameter of the metallic glass is at least 0.7 mm.
In another embodiment, the critical bending diameter of the metallic glass is at least 0.8 mm.
In another embodiment, up to 5 atomic percent of Fe is substituted by Co, Ru, Mn, or a combination thereof.
In another embodiment, up to 2 atomic percent of Ni is substituted by Pd, Pt, or a combination thereof.
In another embodiment, up to 1 atomic percent of Mo is substituted by Nb, Ta, V, W, or a combination thereof.
In another embodiment, up to 2 atomic percent of P is substituted by Si.
The disclosure is also directed to a method of forming a metallic glass, or an article made of a metallic glass, from the metallic glass-forming alloy.
The method includes heating and melting an ingot comprising the metallic glass-forming alloy under inert atmosphere to create a molten alloy, and subsequently quenching the molten alloy fast enough to avoid crystallization of the molten alloy.
In one embodiment, prior to quenching the molten alloy is heated to at least 100° C. above the liquidus temperature of the metallic glass-forming alloy.
In another embodiment, prior to quenching the molten alloy is heated to at least 200° C. above the liquidus temperature of the metallic glass-forming alloy.
In yet another embodiment, prior to quenching the molten alloy is heated to at least 1200° C.
In yet another embodiment, prior to quenching the molten alloy is heated to at least 1300° C.
The disclosure is also directed to a method of thermoplastically shaping a metallic glass into an article, including:
In one embodiment, To is higher than Tg and lower the liquidus temperature of the metallic glass-forming alloy.
In another embodiment, To is greater than Tg and lower than T.
In another embodiment, To is higher than Tx and lower than the solidus temperature of the metallic glass-forming alloy.
In another embodiment, To is in the range of 550 to 850° C.
In another embodiment, To is in the range of 575 to 750° C.
In another embodiment, To is in the range of 600 to 700° C.
In another embodiment, To is such that the supercooling temperature is in the range of 200 to 300° C.
In another embodiment, To is such that the supercooling temperature is in the range of 225 to 275° C.
In another embodiment, To is such that the supercooling temperature is in the range of 235 to 265° C.
In another embodiment, To is such that the normalized supercooling temperature is in the range of 0.25 to 0.5.
In another embodiment, To is such that the normalized supercooling temperature is in the range of 0.3 to 0.4.
In another embodiment, To is such that the normalized supercooling temperature is in the range of 0.325 to 0.375.
In another embodiment, the viscosity of the sample at To is less than 105 Pa-s.
In another embodiment, the viscosity of the sample at To is in the range of 10° to 105 Pa-s.
In another embodiment, the viscosity of the sample at To is in the range of 101 to 104 Pa-s.
In another embodiment, heating of the sample of the metallic glass-forming alloy is performed by conduction to a hot surface.
In another embodiment, heating of the sample of the metallic glass-forming alloy is performed by inductive heating.
In another embodiment, heating of the sample of the metallic glass-forming alloy is performed by ohmic heating.
In another embodiment, the ohmic heating is performed by the discharge of at least one capacitor.
The disclosure is also directed to a metallic glass-forming alloy or a metallic glass having compositions selected from a group consisting of: Fe67Ni7Mo4P13.5C6B2.5, Fe67Ni7Mo4P13C6.5B2.5, Fe67Ni7Mo4P12.5C7B2.5, Fe67Ni7Mo4P14C6B2, Fe67Ni7Mo4P13C6B3, Fe67Ni7Mo4P12.5C6B3.5, Fe67Ni7Mo4P12C6B4, Fe66.5Ni7Mo4.5P13.5C6B2.5, Fe66Ni7Mo5P13.5C6B2.5, Fe69Ni5Mo4P13.5C6B2.5, Fe65Ni9Mo4P13.5C6B2.5, Fe64Ni9Cr1Mo4P13.5C6B2.5, Fe63.5Ni9Cr1.5Mo4P13.5C6B2.5, Fe63Ni9Cr2Mo4P13.5C6B2.5, Fe62Ni9Cr3Mo4P13.5C6B2.5, Fe63.7Ni9.03Cr1.51Mo4.01P13.35C5.93B2.47, Fe63.1Ni8.94Cr1.49Mo3.97P13.81C6.13B2.56, and Fe62.69Ni8.88Cr1.48Mo3.95P14.12C6.27B2.61.
The disclosure may be understood by reference to the following detailed description, taken in conjunction with the drawings as described below. It is noted that, for purposes of illustrative clarity, certain elements in various drawings may not be drawn to scale.
In the disclosure, the glass-forming ability of an alloy is quantified by the “critical rod diameter,” defined as maximum rod diameter in which the amorphous phase can be formed when processed by a method of water quenching a quartz tube with a 0.5 mm thick wall containing the molten alloy.
The “critical cooling rate”, which is defined as the cooling rate to avoid crystallization and form the amorphous phase of the alloy (i.e. a metallic glass), determines the “critical rod diameter”. The lower the critical cooling rate of an alloy, the larger its critical rod diameter. The critical cooling rate Rc in K/s and critical rod diameter d, in mm are related via the following approximate empirical formula:
Rc=1000/dc2 Eq. (2)
For example, according to Eq. (2), the critical cooling rate for an alloy having a critical rod diameter of about 3 mm is about 102 K/s.
Generally, three categories are known in the art for identifying the ability of an alloy to form a metallic glass (i.e. to bypass the stable crystal phase and form an amorphous phase). Alloys having critical cooling rates in excess of 1012 K/s are typically referred to as non-glass formers, as it is very difficult to achieve such cooling rates and form the amorphous phase over a meaningful cross-section thickness (i.e. at least 1 micrometer). Alloys having critical cooling rates in the range of 105 to 1012 K/s are typically referred to as marginal glass formers, as they are able to form glass over thicknesses ranging from 1 to 100 micrometers according to Eq. (2). Alloys having critical cooling rates on the order of 103 or less, and as low as 1 or 0.1 K/s, are typically referred to as bulk glass formers, as they are able to form glass over thicknesses ranging from 1 millimeter to several centimeters. The glass-forming ability of an alloy (and by extension its critical cooling rate and critical rod diameter) is, to a very large extent, dependent on the composition of the alloy. The compositional ranges for alloys capable of forming marginal glass formers are considerably broader than those for forming bulk glass formers.
Often in the art, a measure of glass forming ability of an alloy is reported as the critical plate thickness instead of the critical rod diameter. Due to its symmetry, the diameter of a rod to achieve a certain cooling rate at the centerline is about twice the thickness of a plate for achieving the same cooling rate at the centerline. Hence, the critical plate thickness to achieve a critical cooling rate is about half the critical rod diameter to achieve the same critical cooling rate. Therefore, a critical plate thickness can be approximately converted to a critical rod diameter by multiplying by 2.
In the disclosure, the thermal stability of the supercooled liquid ΔTx is defined as the difference between the crystallization temperature Tx and the glass transition temperature Tg of the metallic glass, ΔTx=Tx−Tg, measured by calorimetry at a heating rate of 20 K/min.
The thermal stability of the supercooled liquid ΔTx is a property defining the ability of the metallic glass to be shaped “thermoplastically” in the supercooled liquid region, i.e. to be shaped by heating the metallic glass to a softening temperature To above the glass transition temperature Tg, applying a deformational force to shape the metallic glass over a time to that is shorter than the time it takes for the softened metallic glass to crystallize at To, and cooling the metallic glass to a temperature below Tg. The higher the thermal stability of the supercooled liquid ΔTx, the longer the available time to, which allows for application of the deformational force for longer periods and thus enables larger shaping strains. Also, the higher the thermal stability of the supercooled liquid ΔTx, the higher the softening temperature To that the metallic glass can be heated, which would result in lower viscosities and thus allow larger shaping strains.
In the disclosure, the supercooling temperature is defined as the difference between the softening temperature To and the glass transition temperature Tg, i.e. To−Tg, expressed in units of either ° C. or K. Also, the normalized supercooling temperature is defined as the difference between the softening temperature To and the glass transition temperature Tg, divided by the glass transition temperature Tg, i.e. (To−Tg)/Tg, expressed in units of K/K.
In some embodiments, To is higher than Tg and lower than the liquidus temperature of the metallic glass-forming alloy. In one embodiment, To is greater than Tg and lower than T. In another embodiment, To is higher than Tx and lower than the solidus temperature of the metallic glass-forming alloy.
In another embodiment, To is in the range of 550 to 850° C. In another embodiment, To is in the range of 575 to 750° C. In yet another embodiment, To is in the range of 600 to 700° C. In another embodiment, To is such that the supercooling temperature is in the range of 200 to 300° C. In another embodiment, To is such that the supercooling temperature is in the range of 225 to 275° C. In yet another embodiment, To is such that the supercooling temperature is in the range of 235 to 265° C. In another embodiment, To is such that the normalized supercooling temperature is in the range of 0.25 to 0.5. In another embodiment, To is such that the normalized supercooling temperature is in the range of 0.3 to 0.4. In yet another embodiment, To is such that the normalized supercooling temperature is in the range of 0.325 to 0.375. In some embodiments, the viscosity at To is less than 105 Pa-s. In one embodiment, the viscosity at To is in the range of 100 to 105 Pa-s. In another embodiment, the viscosity at To is in the range of 101 to 104 Pa-s.
In addition to exhibiting large thermal stability of the supercooled liquid ΔTx, the metallic glasses can be capable of being formed in bulk (i.e. millimeter-thick) dimensions in order to enable “thermoplastic” shaping of bulk 3-dimensional articles. That is, metallic glasses having both a large ΔTx and a capability to be formed in bulk dimensions would be suitable for “thermoplastic” shaping of bulk articles. Discovering compositional regions where the alloy demonstrates a high glass forming ability is unpredictable. Discovering compositional regions where the metallic glass formed from an alloy demonstrates a large ΔTx is equally unpredictable. Discovering compositional regions where (1) the alloy demonstrates a high glass forming ability and (2) the metallic glass formed from the alloy demonstrates a large ΔTx is even more unpredictable than (1) and (2) independently. This is metallic glasses that are capable of being formed at bulk dimensions do not necessarily demonstrate a large ΔTx, and vice versa. In embodiments of the disclosure it is considered that a critical rod diameter of at least 3 mm for the disclosed alloys and a ΔTx of at least 45° C. for the metallic glasses formed from the disclosed alloys may be sufficient to enable “thermoplastic” shaping of bulk 3-dimensional articles. In other embodiments it is considered that a critical rod diameter of at least 3 mm for the disclosed alloys and a ΔTx of at least 50° C. for the metallic glasses formed from the disclosed alloys may be sufficient to enable “thermoplastic” shaping of bulk 3-dimensional articles. In yet other embodiments it is considered that a critical rod diameter of at least 5 mm for the disclosed alloys and a ΔTx of at least 50° C. for the metallic glasses formed from the disclosed alloys may be sufficient to enable “thermoplastic” shaping of bulk 3-dimensional articles.
In addition to glass-forming ability and thermal stability of the supercooled liquid, another important requirement for broad engineering applicability is the ability of the metallic glass to perform well under mechanical load. Good mechanical performance requires that the metallic glass has a relatively high fracture toughness. In the context of this disclosure, the mechanical performance of the metallic glass is characterized by a high fracture toughness and is quantified by the “critical bending diameter”. The critical bending diameter is defined as the maximum diameter in which a rod of the metallic glass, formed by water quenching a quartz capillary containing the molten alloy having a quartz wall thickness equal to about 10% of the rod diameter, can undergo macroscopic plastic bending without fracturing catastrophically.
Therefore, in some embodiments of the disclosure, the metallic glasses formed from the disclosed alloys demonstrate good mechanical performance in addition to exhibiting a large ΔTx and an ability to be formed in bulk dimensions. In the context of this disclosure it is considered that a critical bending diameter of at least 0.5 mm may be sufficient to ensure mechanical performance of the metallic glass.
In this disclosure, compositional regions in the Fe—Cr—Ni—Mo—P—C—B alloys are disclosed where the metallic glass-forming alloys demonstrate a high glass forming ability while the metallic glasses formed from the alloys demonstrate a large ΔTx. In embodiments of the disclosure, the metallic glass-forming alloys demonstrate a critical rod diameter of at least 3 mm, while the metallic glasses formed from the alloys demonstrate a ΔTx of at least 45° C. In some embodiments, the critical rod diameter is at least 4 mm, in other embodiments 5 mm, in other embodiments 6 mm, while in other embodiments the critical rod diameter is at least 7 mm. In some embodiments, the thermal stability of the supercooled liquid is at least 47.5° C., in other embodiments at least 50° C., in other embodiments at least 52.5° C., while in other embodiments the thermal stability of the supercooled liquid is at least 55° C.
In some embodiments, the disclose Fe—Cr—Ni—Mo—P—C—B alloys demonstrate a large critical bending diameter, in addition to a high glass forming ability and a large ΔTx. In embodiments of the disclosure, the metallic glasses formed from the alloys demonstrate a critical bending diameter of at least 0.5 mm. In some embodiments, the critical bending diameter is at least 0.6 mm, in other embodiments at least 0.7 mm, while in other embodiments the critical bending diameter is at least 0.8 mm.
The disclosure is also directed to methods of forming a metallic glass, or an article made of a metallic glass, from the metallic glass-forming alloy. In various embodiments, a metallic glass is formed by heating and melting an alloy ingot to create a molten alloy, and subsequently quenching the molten alloy fast enough to avoid crystallization of the molten alloy. In one embodiment, prior to cooling the molten alloy is heated to at least 100° C. above the liquidus temperature of the metallic glass-forming alloy. In another embodiment, prior to quenching the molten alloy is heated to at least 200° C. above the liquidus temperature of the metallic glass-forming alloy. In another embodiment, prior to quenching the molten alloy is heated to at least 1200° C. In yet another embodiment, prior to quenching the molten alloy is heated to at least 1300° C. In one embodiment, the alloy ingot is heated and melted using a plasma arc. In another embodiment, the alloy ingot is heated and melted using an induction coil. In some embodiments, the alloy ingot is heated and melted inside a quartz crucible or a ceramic crucible. In other embodiments, the alloy ingot is heated and melted over a water-cooled hearth, or within a water-cooled crucible. In one embodiment, the hearth or crucible is made of copper. In some embodiments, the alloy ingot is heated and melted under inert atmosphere. In one embodiment, the inert atmosphere comprises argon gas. In some embodiments, quenching of the molten alloy is performed by injecting or pouring the molten alloy into a metal mold. In some embodiments, the mold can be made of copper, brass, or steel, among other materials. In some embodiments, injection of the molten alloy is performed by a pneumatic drive, a hydraulic drive, an electric drive, or a magnetic drive. In some embodiments, pouring the molten alloy into a metal mold is performed by tilting a tandish containing the molten alloy.
The disclosure is also directed to methods of thermoplastically shaping a metallic glass into an article. In some embodiments, heating of the metallic glass is performed by conduction to a hot surface. In other embodiments, heating of the metallic glass to a softening temperature To above the glass transition temperature Tg is performed by inductive heating. In yet other embodiments, heating of the metallic glass to a softening temperature To above the glass transition temperature Tg is performed by ohmic heating. In one embodiment, the ohmic heating is performed by the discharge of at least one capacitor. In some embodiments, the application of the deformational force to thermoplastically shape the softened metallic glass in the supercooled liquid region is performed by a pneumatic drive, a hydraulic drive, an electric drive, or a magnetic drive.
Description of the Metallic Glass Forming Region
In various embodiments, the disclosure provides Fe—Cr—Ni—Mo—P—C—B alloys capable of forming metallic glasses. The alloys demonstrate a critical rod diameter of at least 3 mm, and the metallic glasses demonstrate a thermal stability of the supercooled liquid of at least 45° C.
Specifically, the disclosure provides Fe—Cr—Ni—Mo—P—C—B metallic glass-forming alloys and metallic glasses where the total metalloid concentration (i.e. the sum of P, C, and B concentrations) is confined over a narrow range, over which the alloys demonstrate a critical rod diameter of at least 3 mm, while the metallic glasses formed from the alloys demonstrate a thermal stability of the supercooled liquid of at least 45° C. In some embodiments, the metallic glasses formed from the alloys also demonstrate a critical bending diameter of at least 0.5 mm. In various embodiments of the disclosure, the concentration of metalloids ranges from 21.25 to 23.75 atomic percent. In other embodiments, the concentration of metalloids ranges from 21.5 to 23.5 atomic percent. In yet other embodiments, the concentration of metalloids ranges from 21.5 to 23 atomic percent.
In one embodiment, the disclosure provides an alloy capable of forming a metallic glass having a composition represented by the following formula (subscripts denote atomic percentages):
Fe(100-a-b-c-d-e-f)CraNibMocPdCeBf EQ. (1)
In another embodiment of the metallic glass-forming alloy or metallic glass, a is up to 9, b ranges from 4 to 12, c ranges from 3 to 6.5, d+e+f ranges from 21.5 to 23.5, e ranges from 5.25 to 7.5, f ranges from 1.5 to 8.5, wherein the metallic glass-forming alloy has a critical rod diameter of at least 4 mm, and wherein the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 47.5° C.
In another embodiment of the metallic glass-forming alloy or metallic glass, a is up to 8, b ranges from 4.5 to 10, c ranges from 3.5 to 5.5, d+e+f ranges from 21.5 to 23, e ranges from 5.5 to 7, f ranges from 2 to 7.5, wherein the metallic glass-forming alloy has a critical rod diameter of at least 5 mm, and wherein the thermal stability of the supercooled liquid of the metallic glass against crystallization is at least 50° C.
Specific embodiments of metallic glasses formed of metallic glass-forming alloys with compositions according to the formula Fe67Ni7Mo4P19.5-xCxB2.5 are presented in Tables 1 and 2. In these alloys, P is substituted by C, where the atomic fraction of C varies from 4 to 8 percent, the atomic fraction of P varies from 11.5 to 15.5 percent, while the atomic fractions of Fe, Ni, Mo, and B are fixed at 67, 7, 4, and 2.5, respectively.
As shown in Table 1 and
The critical rod diameter of the example alloys according to the composition formula Fe67Ni7Mo4P19.5-xCxB2.5 is listed in Table 2 and is plotted in
The critical bending diameter of the example metallic glasses according to the composition formula Fe67Ni7Mo4P19.5-xCxB2.5 is also listed in Table 2. As shown in Table 2, substituting P by C according to Fe67Ni7Mo4P19.5-xCxB2.5 results in increasing bending ductility. Specifically, the critical bending diameter increases from 0.7 mm for the metallic glasses containing 4-5 atomic percent C (Examples 1 and 2), to 0.8 mm for the metallic glasses containing 5.5-6.5 atomic percent C (Examples 3-5), to 0.9 mm for the metallic glasses containing 7-8 atomic percent C (Examples 6-8).
Specific embodiments of metallic glasses formed of metallic glass-forming alloys with compositions according to the formula Fe67Ni7Mo4P16-xC6Bx are presented in Tables 3 and 4. In these alloys, P is substituted by B, where the atomic fraction of B varies from 1 to 9 percent, the atomic fraction of P varies from 7 to 15 percent, while the atomic fractions of Fe, Ni, Mo, and C are fixed at 67, 7, 4, and 6, respectively.
As shown in Table 3 and
The critical rod diameter of the example alloys according to the composition formula Fe67Ni7Mo4P16-xC6Bx is listed in Table 4 and is plotted in
The critical bending diameter of the example metallic glasses according to the composition formula Fe67Ni7Mo4P16-xC6Bx is also listed in Table 4. As shown in Table 4, substituting P by B according to Fe67Ni7Mo4P16-xC6Bx results in decreasing bending ductility. Specifically, the critical bending diameter decreases from 0.8 mm for the metallic glasses containing 1-2.5 atomic percent B (Examples 4 and 9-11), to 0.6 mm for the metallic glasses containing 3-4 atomic percent B (Examples 12-14), to 0.4 mm for the metallic glasses containing 5-7 atomic percent B (Examples 15-17), to 0.3 mm for the metallic glasses containing 8-9 atomic percent B (Examples 18 and 19).
Specific embodiments of metallic glasses formed of metallic glass-forming alloys with compositions according to the formula Fe71-xNi7MoxP13.5C6B2.5 are presented in Tables 5 and 6. In these alloys, Fe is substituted by Mo, where the atomic fraction of Mo varies from 2 to 7 percent, the atomic fraction of Fe varies from 64 to 69 percent, while the atomic fractions of Ni, P, C, and B are fixed at 7, 13.5, 6, and 2.5, respectively.
As shown in Table 5 and
The critical rod diameter of the example alloys according to the composition formula Fe71-xNi7MoxP13.5C6B2.5 is listed in Table 6 and is plotted in
The critical bending diameter of the example metallic glasses according to the composition formula Fe71-xNi7MoxP13.5C6B2.5 is also listed in Table 6. As shown in Table 6, substituting Fe by Mo according to Fe71-xNi7MoxP13.5C6B2.5 results in decreasing bending ductility. Specifically, the critical bending diameter decreases from 1.0 mm for the metallic glass containing 2 atomic percent Mo (Example 20), to 0.9 mm for the metallic glass containing 3 atomic percent Mo (Example 21), to 0.8 mm for the metallic glass containing 4 atomic percent Mo (Example 4), to 0.7 mm for the metallic glasses containing 4.5-5 atomic percent Mo (Examples 22 and 23), to 0.6 mm for the metallic glass containing 6 atomic percent Mo (Example 24), to 0.5 mm for the metallic glass containing 7 atomic percent Mo (Example 25).
Specific embodiments of metallic glasses formed of metallic glass-forming alloys with compositions according to the formula Fe74-xNixMo4P13.5C6B2.5 are presented in Tables 5 and 6. In these alloys, Fe is substituted by Ni, where the atomic fraction of Ni varies from 3 to 13 percent, the atomic fraction of Fe varies from 61 to 71 percent, while the atomic fractions of Mo, P, C, and B are fixed at 4, 13.5, 6, and 2.5, respectively.
As shown in Table 7 and
The critical rod diameter of the example alloys according to the composition formula Fe74-xNixMo4P13.5C6B2.5 is listed in Table 8 and is plotted in
The critical bending diameter of the example metallic glasses according to the composition formula Fe74-xNixMo4P13.5C6B2.5 is also listed in Table 8. As shown in Table 8, substituting Fe by Ni according to Fe74-xNixMo4P13.5C6B2.5 results in fairly constant bending ductility. Specifically, the critical bending diameter increases slightly from 0.8 mm for the metallic glasses containing 3-7 atomic percent Ni (Examples 26-28 and 4), to 0.9 mm for the metallic glasses containing 9-13 atomic percent Ni (Examples 29-31).
Specific embodiments of metallic glasses formed of metallic glass-forming alloys with compositions according to the formula Fe65-xNi9CrxMo4P13.5C6B2.5 are presented in Tables 5 and 6. In these alloys, Cr is introduced at the expense of Fe, where the atomic fraction of Cr varies from 0 to 10 percent, the atomic fraction of Fe varies from 55 to 65 percent, while the atomic fractions of Ni, Mo, P, C, and B are fixed at 9, 4, 13.5, 6, and 2.5, respectively.
As shown in Table 9 and
The critical rod diameter of the example alloys according to the composition formula Fe65-xNi9CrxMo4P13.5C6B2.5 is listed in Table 10 and is plotted in
The critical bending diameter of the example metallic glasses according to the composition formula Fe65-xNi9CrxMo4P13.5C6B2.5 is also listed in Table 10. As shown in Table 10, introducing Cr at the expense of Fe according to Fe65-xNi9CrxMo4P13.5C6B2.5 results in decreasing bending ductility. Specifically, the critical bending diameter decreases from 0.9 mm for the Cr-free metallic glass (Example 29), to 0.7 mm for the metallic glasses containing 1-1.5 atomic percent Cr (Examples 32 and 33), to 0.6 mm for the metallic glass containing 2 atomic percent Cr (Example 34)), to 0.5 mm for the metallic glass containing 3 atomic percent Cr (Example 35), to 0.4 mm for the metallic glass containing 4 atomic percent Cr (Example 36), to 0.3 mm for the metallic glasses containing 6-10 atomic percent Cr (Examples 37-40).
Specific embodiments of metallic glasses formed of metallic glass-forming alloys with compositions according to the formula [Fe0.814Ni0.116Cr0.019Mo0.051]100-x[P0.613C0.273B0.114]x are presented in Tables 11 and 12. In these alloys, metals are substituted by metalloids, where the atomic fraction of metalloids (combined fractions of P, C, and B), denoted by x, varies from 21 to 24 percent, while the atomic fraction of metals (combined atomic fractions Fe, Ni, Cr, Mo), (1−x), varies from 76 to 79 percent.
As shown in Table 11 and
The critical rod diameter of the example alloys according to the composition formula [Fe0.814Ni0.116Cr0.019Mo0.051]100-x[P0.613C0.273B0.114]x is listed in Table 12 and is plotted in
The critical bending diameter of the example metallic glasses according to the composition formula [Fe0.814Ni0.116Cr0.019Mo0.051]100-x[P0.613C0.273B0.114]x is also listed in Table 12. As shown in Table 12, substituting metals by metalloids according to [Fe0.814Ni0.116Cr0.019Mo0.051]100-x[P0.613C0.273B0.114]x results in decreasing bending ductility. Specifically, the critical bending diameter decreases from 0.8 mm for the metallic glasses containing 21-21.5 atomic percent metalloids x (Examples 41 and 42), to 0.7 mm for the metallic glasses containing 21.75-22.5 atomic percent metalloids x (Examples 33, 43 and 44), to 0.6 mm for the metallic glasses containing 23-23.5 atomic percent metalloids x (Examples 45 and 46), to 0.5 mm for the metallic glass containing 24 atomic percent metalloids x (Example 47).
Description of Methods of Processing the Example Alloys
The particular method for producing the alloy ingots involves inductive melting of the appropriate amounts of elemental constituents in a quartz tube under inert atmosphere. The purity levels of the constituent elements were as follows: Fe 99.95%, Cr 99.996% (crystalline), Ni 99.995%, Mo 99.95%, P 99.9999%, C 99.9995%, and B 99.5%. The melting crucible may alternatively be a ceramic such as alumina or zirconia, graphite, sintered crystalline silica, or a water-cooled hearth made of copper or silver.
The particular method for producing the rods of metallic glasses from the alloy ingots involves re-melting the alloy ingots in quartz tubes having 0.5 mm thick walls in a furnace at 1350° C. under high purity argon and rapidly quenching in a room-temperature water bath. Alternatively, the bath could be ice water or oil. Metallic glass articles could be alternatively formed by injecting or pouring the molten alloy into a metal mold. The mold could be made of copper, brass, or steel, among other materials.
In some embodiments, prior to producing a metallic glass article, the alloyed ingots could be fluxed with a reducing agent by re-melting the ingots in a quartz tube under inert atmosphere, bringing the alloy melt in contact with the molten reducing agent, and allowing the two melts to interact for about 1000 s at a temperature of about 1200° C. or higher, and subsequently water quenching. In one embodiment, the reducing agent is boron oxide.
Test Methodology for Assessing Glass-Forming Ability
The glass-forming ability of each alloy was assessed by determining the maximum rod diameter in which the amorphous phase of the alloy (i.e. the metallic glass phase) could be formed when processed by the methods described above. X-ray diffraction with Cu-Kα radiation was performed to verify the amorphous structure of the alloys.
Test Methodology for Assessing Bending Ductility
The bending ductility of each metallic glass was assessed by determining the maximum rod diameter in which the metallic glass subject to a bending load is capable of permanently (i.e. irreversibly, inelastically) bending without fracturing catastrophically.
Test Methodology for Differential Scanning Calorimetry
Differential scanning calorimetry was performed on sample metallic glasses at a scan rate of 20 K/min to determine the glass-transition and crystallization temperatures of sample metallic glasses formed from the glass-forming alloys, and also to determine the solidus and liquidus temperatures of the alloys.
Having described several embodiments, it will be recognized by those skilled in the art that various modifications, alternative constructions, and equivalents may be used without departing from the spirit of the disclosure. Those skilled in the art will appreciate that the presently disclosed embodiments teach by way of example and not by limitation. Therefore, the matter contained in the above description or shown in the accompanying drawings should be interpreted as illustrative and not in a limiting sense. Additionally, a number of well-known processes and elements have not been described in order to avoid unnecessarily obscuring the disclosure.
The following claims are intended to cover all generic and specific features described herein, as well as all statements of the scope of the present method and system, which, as a matter of language, might be said to fall therebetween.
The present application claims priority under 35 U.S.C. 119(e) to U.S. Provisional Application No. 62/805,845, entitled “Tough Iron-Based Glasses with High Glass Forming Ability and High Thermal Stability” to Na et al., filed Feb. 14, 2019, the disclosure of which is incorporated herein by reference in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
2106145 | Floraday | Jan 1938 | A |
2124538 | Boyer | Jul 1938 | A |
2190611 | Sembdner | Feb 1940 | A |
3322546 | Tanzman et al. | May 1967 | A |
3539192 | Prasse | Nov 1970 | A |
3558846 | Ujiie | Jan 1971 | A |
3696228 | Thomas, Jr. et al. | Oct 1972 | A |
3742585 | Wentzell | Jul 1973 | A |
3776297 | Williford et al. | Dec 1973 | A |
3856513 | Chen et al. | Dec 1974 | A |
3948613 | Weill | Apr 1976 | A |
3970445 | Gale et al. | Jul 1976 | A |
3986867 | Masumoto et al. | Oct 1976 | A |
3986892 | Eve et al. | Oct 1976 | A |
3989517 | Tanner et al. | Nov 1976 | A |
4024902 | Baum | May 1977 | A |
4050931 | Tanner et al. | Sep 1977 | A |
4064757 | Hasegawa | Dec 1977 | A |
4067732 | Ray | Jan 1978 | A |
4113478 | Tanner et al. | Sep 1978 | A |
4115682 | Kavesh et al. | Sep 1978 | A |
4116682 | Polk et al. | Sep 1978 | A |
4116687 | Hasegawa | Sep 1978 | A |
4124472 | Riegert | Nov 1978 | A |
4125737 | Andersson | Nov 1978 | A |
4126284 | Ichikawa et al. | Nov 1978 | A |
4126449 | Tanner et al. | Nov 1978 | A |
4135924 | Tanner et al. | Jan 1979 | A |
4144058 | Chen et al. | Mar 1979 | A |
4148669 | Tanner et al. | Apr 1979 | A |
4152144 | Hasegawa et al. | May 1979 | A |
4163071 | Weatherly et al. | Jul 1979 | A |
4260416 | Kavesh et al. | Apr 1981 | A |
4268564 | Narasimhan | May 1981 | A |
4289009 | Festag et al. | Sep 1981 | A |
4309587 | Nakano et al. | Jan 1982 | A |
4321289 | Bartsch | Mar 1982 | A |
4330027 | Narasimhan | May 1982 | A |
4373128 | Asai et al. | Feb 1983 | A |
4374900 | Hara et al. | Mar 1983 | A |
4381943 | Dickson et al. | May 1983 | A |
4385932 | Inomata et al. | May 1983 | A |
4385944 | Hasegawa | May 1983 | A |
4396820 | Puschner | Aug 1983 | A |
4409296 | Ward | Oct 1983 | A |
4472955 | Nakamura et al. | Sep 1984 | A |
4482612 | Kuroki et al. | Nov 1984 | A |
4487630 | Crook et al. | Dec 1984 | A |
4488882 | Dausinger et al. | Dec 1984 | A |
4499158 | Onuma et al. | Feb 1985 | A |
4515870 | Bose et al. | May 1985 | A |
4523625 | Ast | Jun 1985 | A |
4526618 | Keshavan et al. | Jul 1985 | A |
4557981 | Bergmann | Dec 1985 | A |
4564396 | Johnson et al. | Jan 1986 | A |
4570568 | Fair | Feb 1986 | A |
4582536 | Raybould | Apr 1986 | A |
4585617 | Tenhover et al. | Apr 1986 | A |
4612059 | Mori et al. | Sep 1986 | A |
4621031 | Scruggs | Nov 1986 | A |
4623387 | Masumoto et al. | Nov 1986 | A |
4648609 | Deike | Mar 1987 | A |
4656099 | Sievers | Apr 1987 | A |
4668310 | Kudo et al. | May 1987 | A |
4707581 | Blaskovits et al. | Nov 1987 | A |
4710235 | Scruggs | Dec 1987 | A |
4721154 | Christ et al. | Jan 1988 | A |
4725512 | Scruggs | Feb 1988 | A |
4728580 | Grasselli et al. | Mar 1988 | A |
4731253 | DuBois | Mar 1988 | A |
4741974 | Longo et al. | May 1988 | A |
4743513 | Scruggs | May 1988 | A |
4770701 | Henderson et al. | Sep 1988 | A |
4781803 | Harris et al. | Nov 1988 | A |
4810850 | Tenkula et al. | Mar 1989 | A |
4850524 | Schick | Jul 1989 | A |
4854370 | Nakamura | Aug 1989 | A |
4892628 | Guilinger | Jan 1990 | A |
4900638 | Emmerich | Feb 1990 | A |
4960643 | Lemelson | Oct 1990 | A |
4968363 | Hashimoto et al. | Nov 1990 | A |
4976417 | Smith | Dec 1990 | A |
4987033 | Abkowitz et al. | Jan 1991 | A |
4990198 | Masumoto et al. | Feb 1991 | A |
5030519 | Scruggs et al. | Jul 1991 | A |
5032196 | Masumoto et al. | Jul 1991 | A |
5053084 | Masumoto et al. | Oct 1991 | A |
5053085 | Masumoto et al. | Oct 1991 | A |
5074935 | Masumoto et al. | Dec 1991 | A |
5112388 | Schulz et al. | May 1992 | A |
5117894 | Katahira | Jun 1992 | A |
5127969 | Sekhar | Jul 1992 | A |
5131279 | Lang et al. | Jul 1992 | A |
5169282 | Ueda et al. | Dec 1992 | A |
5189252 | Huffman et al. | Feb 1993 | A |
5213148 | Masumoto et al. | May 1993 | A |
5225004 | O'Handley et al. | Jul 1993 | A |
5250124 | Yamaguchi et al. | Oct 1993 | A |
5279349 | Horimura | Jan 1994 | A |
5288344 | Peker et al. | Feb 1994 | A |
5294462 | Kaiser et al. | Mar 1994 | A |
5296059 | Masumoto et al. | Mar 1994 | A |
5306463 | Horimura | Apr 1994 | A |
5312495 | Masumoto et al. | May 1994 | A |
5324368 | Masumoto et al. | Jun 1994 | A |
5338376 | Liu et al. | Aug 1994 | A |
5368659 | Peker et al. | Nov 1994 | A |
5380349 | Taniguchi et al. | Jan 1995 | A |
5380375 | Hashimoto et al. | Jan 1995 | A |
5384203 | Apfel | Jan 1995 | A |
5390724 | Yamauchi et al. | Feb 1995 | A |
5429725 | Thorpe et al. | Jul 1995 | A |
5440995 | Levitt | Aug 1995 | A |
5449425 | Renard et al. | Sep 1995 | A |
5482577 | Hashimoto et al. | Jan 1996 | A |
5482580 | Scruggs et al. | Jan 1996 | A |
5567251 | Peker et al. | Oct 1996 | A |
5567532 | Peker et al. | Oct 1996 | A |
5589012 | Hobby et al. | Dec 1996 | A |
5593514 | Giessen et al. | Jan 1997 | A |
5618359 | Lin et al. | Apr 1997 | A |
5634989 | Hashimoto et al. | Jun 1997 | A |
5711363 | Scruggs et al. | Jan 1998 | A |
5735975 | Lin et al. | Apr 1998 | A |
5797443 | Lin et al. | Aug 1998 | A |
5807468 | Sakamoto et al. | Sep 1998 | A |
5886254 | Chi | Mar 1999 | A |
5950704 | Johnson et al. | Sep 1999 | A |
5961745 | Inoue et al. | Oct 1999 | A |
6004661 | Sakai et al. | Dec 1999 | A |
6010580 | Dandliker et al. | Jan 2000 | A |
6021840 | Colvin | Feb 2000 | A |
6027586 | Masumoto et al. | Feb 2000 | A |
6039860 | Cooper et al. | Mar 2000 | A |
6044893 | Taniguchi et al. | Apr 2000 | A |
6053989 | Orillion et al. | Apr 2000 | A |
6077367 | Mizushima et al. | Jun 2000 | A |
6183889 | Koshiba et al. | Feb 2001 | B1 |
6200685 | Davidson | Mar 2001 | B1 |
6218029 | Rickerby | Apr 2001 | B1 |
6258183 | Onuki et al. | Jul 2001 | B1 |
6261386 | Perepezko et al. | Jul 2001 | B1 |
6303015 | Thorpe et al. | Oct 2001 | B1 |
6306228 | Inoue et al. | Oct 2001 | B1 |
6325868 | Kim et al. | Dec 2001 | B1 |
6326295 | Figura | Dec 2001 | B1 |
6371195 | Onuki et al. | Apr 2002 | B1 |
6376091 | Croopnick | Apr 2002 | B1 |
6408734 | Cohen | Jun 2002 | B1 |
6446558 | Peker et al. | Sep 2002 | B1 |
6620264 | Kundig et al. | Sep 2003 | B2 |
6623566 | Senkov et al. | Sep 2003 | B1 |
6638369 | Tucker et al. | Oct 2003 | B1 |
6689234 | Branagan | Feb 2004 | B2 |
6695936 | Johnson | Feb 2004 | B2 |
6749698 | Shimizu et al. | Jun 2004 | B2 |
7008490 | Peker | Mar 2006 | B2 |
7141127 | Yoshizawa | Nov 2006 | B2 |
7282103 | Sakamoto et al. | Oct 2007 | B2 |
7582172 | Schroers et al. | Sep 2009 | B2 |
7622011 | Inoue et al. | Nov 2009 | B2 |
7918011 | Boylan et al. | Apr 2011 | B2 |
7918946 | Sato | Apr 2011 | B2 |
8052923 | Langlet | Nov 2011 | B2 |
8287664 | Brunner | Oct 2012 | B2 |
8529712 | Demetriou et al. | Sep 2013 | B2 |
8911572 | Kim et al. | Dec 2014 | B2 |
9085814 | Na et al. | Jul 2015 | B2 |
9359664 | Demetriou et al. | Jun 2016 | B2 |
9365916 | Floyd et al. | Jun 2016 | B2 |
9534283 | Na et al. | Jan 2017 | B2 |
9556504 | Na et al. | Jan 2017 | B2 |
9862024 | Tomita et al. | Jan 2018 | B2 |
9920400 | Na et al. | Mar 2018 | B2 |
9920410 | Na et al. | Mar 2018 | B2 |
9957596 | Na et al. | May 2018 | B2 |
10000834 | Na et al. | Jun 2018 | B2 |
10287663 | Na et al. | May 2019 | B2 |
20020036034 | Xing et al. | Mar 2002 | A1 |
20040140016 | Sakamoto et al. | Jul 2004 | A1 |
20050263216 | Chin et al. | Dec 2005 | A1 |
20060037361 | Johnson et al. | Feb 2006 | A1 |
20060213586 | Kui | Sep 2006 | A1 |
20060231169 | Park et al. | Oct 2006 | A1 |
20060254386 | Inoue et al. | Nov 2006 | A1 |
20070003812 | Wende | Jan 2007 | A1 |
20070048164 | Demetriou et al. | Mar 2007 | A1 |
20070079907 | Johnson et al. | Apr 2007 | A1 |
20070175545 | Urata et al. | Aug 2007 | A1 |
20090014096 | Wiest et al. | Jan 2009 | A1 |
20090101244 | Ogawa et al. | Apr 2009 | A1 |
20090110955 | Hartmann et al. | Apr 2009 | A1 |
20090114317 | Collier et al. | May 2009 | A1 |
20100089761 | Wang et al. | Apr 2010 | A1 |
20100096045 | Sato | Apr 2010 | A1 |
20100300148 | Demetriou | Dec 2010 | A1 |
20120073710 | Kim et al. | Mar 2012 | A1 |
20120168037 | Demetriou et al. | Jul 2012 | A1 |
20130048152 | Na et al. | Feb 2013 | A1 |
20130263973 | Kurahashi et al. | Oct 2013 | A1 |
20140007991 | Demetriou et al. | Jan 2014 | A1 |
20140076467 | Na et al. | Mar 2014 | A1 |
20140096873 | Na et al. | Apr 2014 | A1 |
20140116579 | Na et al. | May 2014 | A1 |
20140130942 | Floyd et al. | May 2014 | A1 |
20140130945 | Na et al. | May 2014 | A1 |
20140190593 | Na et al. | Jul 2014 | A1 |
20140213384 | Johnson et al. | Jul 2014 | A1 |
20140238551 | Na et al. | Aug 2014 | A1 |
20140345755 | Na et al. | Nov 2014 | A9 |
20150047755 | Na et al. | Feb 2015 | A1 |
20150096652 | Na et al. | Apr 2015 | A9 |
20150158126 | Hartmann et al. | Jun 2015 | A1 |
20150159242 | Na et al. | Jun 2015 | A1 |
20150176111 | Na et al. | Jun 2015 | A1 |
20150197837 | Schramm et al. | Jul 2015 | A9 |
20150240336 | Na et al. | Aug 2015 | A1 |
20160047023 | Na et al. | Feb 2016 | A1 |
20160060739 | Na et al. | Mar 2016 | A1 |
20160090644 | Na et al. | Mar 2016 | A1 |
20170152587 | Na et al. | Jun 2017 | A9 |
20170152588 | Na et al. | Jun 2017 | A9 |
20180312949 | Na et al. | Nov 2018 | A1 |
Number | Date | Country |
---|---|---|
PI 1010960-9 | Apr 2019 | BR |
PI 1010960-9 | Feb 2020 | BR |
1354274 | Jun 2002 | CN |
1442866 | Sep 2003 | CN |
1653200 | Aug 2005 | CN |
101289718 | Oct 2008 | CN |
102459680 | May 2012 | CN |
103917673 | Jul 2014 | CN |
3929222 | Mar 1991 | DE |
10237992 | Mar 2003 | DE |
102011001783 | Oct 2012 | DE |
102011001784 | Oct 2012 | DE |
0014335 | Aug 1980 | EP |
0161363 | Nov 1985 | EP |
0161393 | Nov 1985 | EP |
0164200 | Dec 1985 | EP |
0260706 | Mar 1988 | EP |
0747498 | Dec 1996 | EP |
1077272 | Feb 2001 | EP |
1108796 | Jun 2001 | EP |
1522602 | Apr 2005 | EP |
2432909 | Mar 2012 | EP |
2748345 | Aug 2018 | EP |
2005302 | Apr 1979 | GB |
2106145 | Feb 1987 | GB |
2236325 | Apr 1991 | GB |
1168875 | Jan 2013 | HK |
337634 | May 2020 | IN |
S5476423 | Jun 1979 | JP |
55141537 | Nov 1980 | JP |
S55148752 | Nov 1980 | JP |
56112449 | Sep 1981 | JP |
S5713146 | Jan 1982 | JP |
60024346 | Feb 1985 | JP |
61238423 | Oct 1986 | JP |
63079930 | Apr 1988 | JP |
63079931 | Apr 1988 | JP |
S63277734 | Nov 1988 | JP |
H01205062 | Aug 1989 | JP |
06-264200 | Sep 1994 | JP |
08269647 | Oct 1996 | JP |
2008333660 | Dec 1996 | JP |
H09143642 | Jun 1997 | JP |
11071657 | Mar 1999 | JP |
H1171659 | Mar 1999 | JP |
2011293427 | Oct 1999 | JP |
2000-256811 | Sep 2000 | JP |
2001049407 | Feb 2001 | JP |
2001338808 | Dec 2001 | JP |
2000237902 | Feb 2002 | JP |
2002069549 | Mar 2002 | JP |
2002275605 | Sep 2002 | JP |
2005264260 | Sep 2005 | JP |
2007075867 | Mar 2007 | JP |
2014132116 | Jul 2014 | JP |
2014529013 | Oct 2014 | JP |
6178073 | Jul 2017 | JP |
100582579 | May 2006 | KR |
1020090038016 | Apr 2009 | KR |
199902748 | Jan 1999 | WO |
200068469 | Nov 2000 | WO |
2003040422 | May 2003 | WO |
2004059019 | Jul 2004 | WO |
2010135415 | Nov 2010 | WO |
2010135415 | Mar 2011 | WO |
2012047651 | Apr 2012 | WO |
2012047651 | Apr 2012 | WO |
2012053570 | Apr 2012 | WO |
2013028790 | Feb 2013 | WO |
2013028790 | Jun 2013 | WO |
2014043722 | Mar 2014 | WO |
2014058893 | Apr 2014 | WO |
2014078697 | May 2014 | WO |
2014078697 | May 2015 | WO |
Entry |
---|
“Interbike Buyer Official Show Guide”, advertisement, 1995, 1 page. |
Extended European Search Report for European Application No. 10778319.3, Search completed Feb. 20, 2017, dated Feb. 27, 2017, 16 Pgs. |
Extended European Search Report for European Application No. 11831296.6, Search completed Apr. 24, 2017, dated May 3, 2017, 11 Pgs. |
International Preliminary Report on Patentability for Application PCT/US2013/070370, Report dated May 19, 2015, dated May 28, 2015, 09 pgs. |
International Preliminary Report on Patentability for International Application No. PCT/US10/35382, Report dated Nov. 22, 2011, dated Dec. 1, 2011, 5 Pgs. |
International Preliminary Report on Patentability for International Application No. PCT/US2012/051921, Report dated Feb. 25, 2014, dated Mar. 6, 2014, 8 Pgs. |
International Preliminary Report on Patentability for International Application No. PCT/US2013/060226, dated Mar. 17, 2015, dated Mar. 26, 2015, 9 Pgs. |
International Preliminary Report on Patentability for International Application No. PCT/US2013/063902, Report dated Apr. 8, 2015, dated Apr. 16, 2015, 12 Pgs. |
International Search Report and Written Opinion for Application PCT/US2013/070370, search completed on Mar. 30, 2015, dated Apr. 13, 2015, 12 pgs. |
International Search Report and Written Opinion for International Application No. PCT/US2010/035382, completed Dec. 27, 2010, dated Dec. 29, 2010, 7 pgs. |
International Search Report and Written Opinion for International Application PCT/US2013/060226, Search completed Dec. 5, 2013, dated Jun. 11, 2014, 14 Pgs. |
International Search Report and Written Opinion for International Application No. PCT/US2013/063902, Search completed Nov. 29, 2013, dated Feb. 14, 2014, 18 Pgs. |
International Search Report and Written Opinion for International Application PCT/US2012/051921, dated Apr. 16, 2013, 14 pgs. |
International Search Report and Written Opinion for International Application PCT/US2013/067519, report completed Dec. 6, 2013, dated Dec. 18, 2013, 13 Pgs. |
International Search Report for International Application PCT/US2005/045955 filed Dec. 16, 2005, completed Jun. 29, 2006, dated Aug. 18, 2006, 3 pgs. |
UES, Inc. Software Products Center, “ProCAST . . . not just for castings!”, Sep. 30, 1996, 1 pg. |
Kimura et al., “Fracture Toughness of Amorphous Metals”, Scripta Metallurgy, 1975, vol. 9, pp. 211-222. |
Koch et al., “Preparation of “Amorphous” Ni60Nb40 by Mechanical Alloying”, Appl. Phys. Lett., Dec. 1, 1983, vol. 43, No. 11, pp. 1017-1019. |
Laws et al., “Electron-band theory inspired design of magnesium—precious metal bulk metallic glasses with high thermal stability and extended ductility”, Scientific Reports, Jun. 13, 2017, vol. 7, No. 3400, 11 pgs, doi: 10.1038/s41598-017-03643-7. |
Lewandowski et al., “Tough Fe⋅based bulk metallic glasses”, Applied Physics Letters, vol. 92, pp. 091918-1-091918-3, published online Mar. 7, 2008, http://dx.doi.org/10.1063/1.2890489. |
Li et al., “Effects of Cu, Fe, and Cu Addition on the Glass Forming Ability and Mechanical Properties of Zr—Al—Ni Bulk Metallic Glasses”, Science China, Physics, Mechanics & Astronomy, Dec. 2012, vol. 55, No. 12, pp. 2367-2371. |
Li et al., “Excellent soft-magnetic properties of (Fe,Co)—Mo—(P,C,B,Si) bulk glassy alloys with ductile deformation behavior”, Applied Physics Letters, 2007), vol. 91, pp. 234101-1-234101-3, https://doi.org/10.1063/1.2820608. |
Liu et al., “Ductile Fa-Based BMGs with High Glass Forming Ability and High Strength”, Materials Transactions, Jan. 28, 2008, vol. 49, No. 2, pp. 231-234, http://doi.org/10.2320/matertrans.MRA2007186. |
Lu et al., “Structural Amorphous Steels”, Physical Review Letters, Jun. 18, 2004, vol. 92, No. 24, pp. 244503-1-245503-4, DOI: 10.1103/PhysRevLett.92.245503. |
Makino et al., “Fe-Metalloid Metallic Glasses with High Magnetic Flux Density and High Glass-Forming Ability”, Materials Science Forum 2007, vols. 561-565, pp. 1361-1366. |
Maret et al., “Structural Study of Be43HfxZr57-x Metallic Glasses by X-Ray and Neutron Diffraction”, J. Physique, 1986, vol. 47, pp. 863-871. |
Masumoto, “Recent Progress in Amorphous Metallic Materials in Japan”, Materials Science and Engineering, 1994, vol. A179/A180, pp. 8-16. |
Masumoto et al., “Tensile Properties of Iron-base Amorphous Alloy (Fe—P—C) Quenched from Liquid”, Science Reports of the Research Institutes, Tohoku University, 1974, vol. 6, pp. 200-215. |
Mitsuhashi et al., “The corrosion behavior of amorphous nickel base alloys in a hot concentrated phosphoric acid”, Corrosion Science, 1987, vol. 27, No. 9, pp. 957-970. |
Morrison et al., “Cyclic-anodic-polarization studies of a Zr41.2Ti13.8Ni10Cu12.5Be22.5 bulk metallic glass”, Intermetallics, 2004, vol. 12, pp. 1177-1181. |
Murakami, “Stress Intensity Factors Handbook”, Oxford: Pergamon Press, 1987, vol. 2, 4 pages. |
Murakami, “Stress Intensity Factors Handbook”, vol. 2. Oxford (United Kingdom): Pergamon Press; 1987, 11 pgs. |
Nouri et al., “Chemistry (intrinsic) and inclusion (extrinsic) effects on the toughness and Weibull modulus of Fe⋅based bulk metallic”, Philosophical Magazine Letters, Nov. 2008, vol. 88, No. 11, pp. 853⋅861, DOI:10.1080/09500830802438131. |
Park et al., “Development of new Ni-based amorphous alloys containing no metalloid that have large undercooled liquid regions”, Scripta Materialia, 2000, vol. 43, No. 2, pp. 109-114. |
Peker et al., “A highly processible metallic glass: Zr41.2Ti13.8Cu12.5Ni10.0Be22.5”, Applied Physics Letters, Oct. 25, 1993, vol. 63, No. 17, pp. 2342-2344. |
Polk et al, “The Effect of Oxygen Additions on the Properties of Amorphous Transition Metal Alloys”, source and date unknown, pp. 220-230. |
Ponnambalam et al., “Fe-Based Bulk Metallic Glasses with Diameter Thickness Larger Than One Centimeter”, J Mater Res, Feb. 17, 2004. vol. 19; pp. 1320-1323, DOI: 10.1557/JMR.2004.0176. |
Ponnambalam et al., “Fe—Mn—Cr—Mo—(Y,Ln)—C-8 (Ln=Lanthanides) bulk metallic glasses as formable amorphous steel alloys”, Journal of Materials Research, Oct. 2004, vol. 19, No. 10, pp. 3046-3052, DOI:10.1557/JMR.2004.0374. |
Rabinkin et al., “Brazing Stainless Steel Using New MBF-Series of Ni—Cr—B—Si Amorphous Brazing Foils New Brazing Alloys Withstand High-Temperature and Corrosive Environments”, Welding Research Supplement, Feb. 1998, pp. 66-75. |
Roshenow, “Heat Transfer”, Handbook of Engineering, 1936, Section 12, pp. 1113-1119. |
Schroers, “The Superplastic Forming of Bulk Metallic Glasses”, JOM, May 2005, pp. 35-39. |
Shamlaye et al., “Exceptionally broad bulk metallic glass formation in the Mg—Cu—Yb system”, Acta Materialia, Apr. 15, 2017, vol. 128, pp. 188-196, doi: 10.1016/j.actamat.2017.02.013. |
Shen et al., “Bulk ferromagnetic glasses prepared by flux melting and water”, Applied Physics Letters, Jul. 5, 1999, vol. 75, No. 1, pp. 49-51, published online Jun. 29, 1999, doi.org/10.1063/1.124273. |
Shen et al., “Excellent soft-ferromagnetic bulk glassy alloys with high saturation magnetization”, Applied Physics Letters, 2006, vol. 88, pp. 131907-1-131907-3, published online Mar. 28, 2006, DOI:10.1063/1.2189910. |
Suh, Jin-Yoo, “Fracture Toughness Study on Bulk Metallic Glasses and Novel Joining Method Using Bulk Metallic Glass Solder”, Thesis, California Institute of Technology, 2009, 48 pgs. |
Sunderman, “Potential toxicity from nickel contamination of intravenous fluids”, Annals of Clinical & Laboratory Science, 1983, vol. 13, pp. 1-4. |
Tanner et al., “Metallic Glass Formation and Properties in Zr and Ti Alloyed with Be—I The Binary Zr—Be and Ti—Be Systems”, Acta Metallurgica, 1979, vol. 27, pp. 1727-1747. |
Tanner, et al., “Physical Properties of Ti50Be40Zr10 Glass”, Scripta Metallurgica, 1977, vol. 11, pp. 783-789. |
Tanner, L.C., “The Stable and Metastable Phase Relations in the Hf—Be Alloy System”, Metallurgica, vol. 28, 1980, pp. 1805-1815. |
Tanner, L.E, “Physical Properties of Ti—Be—Si Glass Ribbons”, Scripta Metallurgica, 1978, vol. 12, pp. 703-708. |
Wang et al., “Bulk Amorphous Ni75-xNb5MxP20-yBy(M=Cr,Mo)Alloys with Large Supercooling and High Strength”, Materials Transactions, JIM, 1999, vol. 40, No. 10, pp. 1130-1136. |
Wang et al., “Fatigue behavior and fracture morphology of Zr50Al10Cu40 and Zr50Al10Cu30Ni10 bulk-metallic glasses”, Intermetallics, 2004, vol. 12, pp. 1219-1227. |
Wesseling et al., “Preliminary assessment of flow, notch toughness, and high temperature behavior of Cu60Zr20Hf10Ti10 bulk metallic glass”, Scripta Materialia, Jul. 2004, vol. 51, pp. 151-154, doi:10.1016/j.scriptamat.2004.03.034. |
Xi et al., “Fracture of Brittle Metallic Glasses: Brittleness or Plasticity”, Physical Review Letters, Apr. 1, 2005, vol. 94, pp. 125510-1-125510-4, doi: 10.1103/PhysRevLett.94.125510. |
Yamamoto et al., “Cytotoxicity evaluation of 43 metal salts using murine fibroblasts and osteoblastic cells”, Journal of Biomed. Materials Research, 1998, vol. 39, 331-340. |
Yokoyama et al., “Hot-press workability of Ni-based glassy alloys in supercooled liquid state and production of the glassy alloy separators for proton exchange membrane fuel cell”, Journal of the Japan Society of Powder and Powder Metallurgy, 2007, vol. 54, No. 11, pp. 773-777. |
Yokoyama et al., “Viscous Flow Workability of Ni—Cr—P—B Metallic Glasses Produced by Melt-Spinning in Air”, Materials Transactions, Nov. 2007 vol. 48, No. 12, pp. 3176-3180. |
Zhang et al., “Amorphous Zr—A1—TM (TM=Co, Ni, Cu) Alloys with Significant Supercooled Liquid Region of Over 100K”, Materials Transactions, JIM, 1991, vol. 32, No. 11, pp. 1005-1010. |
Zhang et al., “Ductile Fe-Based Bulk MetallicGlass with Good Soft-Magnetic Properties”, Materials Transactions, 2007, vol. 48, No. 5, pp. 1157-1160, doi:10.2320/matertrans.48.1157. |
Zhang et al., “The corrosion behavior of amorphous Ni—Cr—P alloys in concentrated hydrofluoric acid”, Corrosion Science, Oct. 1992, vol. 33, No. 10, pp. 1519-1528. |
Written Opinion for International Application No. PCT/US2005/045955 filed Dec. 16, 2005, completed Jun. 29, 2006, dated Aug. 18, 2006, 5 pgs. |
Abrosimova et al., “Phase segregation and crystallization in the amorphous alloy Ni70Mo10P20”, Physics of the Solid State, 1998, vol. 40., No. 9, pp. 1429-1432. |
American Society for Metals, “Forging and Casting”, Metals Handbook, Jan. 1970, vol. 5, 8th Edition, 16 pgs. |
ASM Committee on Tooling, Materials “Superhard Tool Materials”, Metals Handbook, Ninth Edition, vol. 3, Properties and Selection: Stainless Steels, Tool Materials and Special Purpose Metals, American Society for Metals, 1980, pp. 448-465, title page and copyright page. |
Author Unknown, “A World of Superabrasives Experience at Your Service”, source unknown, 4 pgs. |
Author Unknown, “GE Superabrasives—Micron Powders”, source unknown, 1 pg. |
Author Unknown, “GE Superabrasives—The MBS—900 Series Product Line”, source unknown, 2 pgs. |
Author Unknown, “GE Superabrasives—The MBS 700 Series Product Line”, source unknown, 2 pgs. |
Author Unknown, “GE Superabrasives—The Metal Bond System”, source unknown, 1 pg. |
Author Unknown, “GE Superabrasives—The Resin Bond System”, source unknown, 1 pg. |
Author Unknown, “Standard Practice for Conducting Dry Sand/Rubber Wheel Abrasion Tests”, ASTM Designation: G 65-81, pp. 351-368. |
Burke, “The Corrosion of Metals in Tissues; and an Introduction to Tantalum”, The Canadian Medical Association Journal, Aug. 1940, pp. 125-128. |
Chen et al., “Transient liquid-phase bonding of T91 steel pipes using amorphous foil”, Materials Science and Engineering, 2009, A, vol. 499, No. 1-2, pp. 114-117, doi:10.1016/jmsea.2007.11.133. |
Debold et al., “How to Passivate Stainless Steel Parts”, Modern Machine Shop, article posted Oct. 1, 2003, 10 pgs. |
Demetriou et al., “Glassy steel optimized for glass-forming ability and toughness”, Applied Physics Letters, Jul. 31, 2009, vol. 95; pp. 041907-1-041907-3; http:/idx.doi.org/10.1063/1.3184792. |
Duan et al., “Thermal and elastic properties of Cu—Zr—Be bulk metallic glass forming alloys”, Applied Physics Letters, 2007, vol. 90, pp. 211901-1-211901-3, doi: 10.1063/1.2741050. |
Duwez et al., “Amorphous Ferromagnetic Phase in Iron-Carbon Phosphorus Alloys”, Journal of Applied Physics, vol. 38, No. 10, pp. 4096⋅4097, ISSN 0021⋅8979, http:// dx.doi.org/10.1063/1.1709084. |
Geurtsen, “Biocompatibility of Dental Casting Alloys”, Crit. Rev. Oral Biol. Med., 2002, vol. 13, No. 1, pp. 71-84. |
Greer et al., “Bulk Metallic Glasses: At the Cutting Edge of Metals Research”, MRS Bulletin, Aug. 2007, vol. 32, pp. 611-619. |
Gu et al., “Ductility improvement of amorphous steels : Roles of shear modulus and electronic structure”, Acta Materialia, Jan. 2008, vol. 56, Issue 1, pp. 88-94, available online Oct. 24, 2007, doi:10.1016/j.actamat.2007.09.011. |
Gu et al., “Effects of carbon content on the mechanical properties of amorphous steel alloys”, Scripta Materialia, vol. 57, Issue 4, Aug. 2007, pp. 289-292, doi:10.1016/j.scriptamat.2007.05.006. |
Gu et al., “Mechanical properties of iron-based bulk metallic glasses”, Journal of Materials Research, vol. 22, Issue 2, Feb. 2007, pp. 344-351, doi.org/10.1557/jmr.2007.0036. |
Guo et al., “Enhancement of plasticity of Fe-based bulk metallic glass by Ni substitution for Fe”, Journal of Alloys and Compounds, Feb. 18, 2010, vol. 504, pp. S78-S81, doi:10.1016/j.jallcom.2010.02.058. |
Habazaki et al., “Preparation of corrosion-resistant amorphous Ni—Cr—P—B bulk alloys containing molybdenum and tantalum”, Material Science and Engineering, 2001, vol. A304-306, pp. 696-700. |
Hartmann et al., “New Amorphous Brazing Foils for Exhaust Gas Application”, Proceedings of the 4th International Brazing and Soldering Conference, Apr. 26-29, 2009, Orlando, Florida, USA, 9 pgs. |
Hasegawa et al., “Superconducting Properties of Be—Zr Glassy Alloys Obtained by Liquid Quenching”, May 9, 1977, pp. 3925-3928. |
Hess et al., “Indentation fracture toughness of amorphous steel”, Journal of Materials Research, Apr. 2005, vol. 20, Issue 4, pp. 783-786, DOI:10.1557/JMR.2005.0104. |
Hiromoto et al., “Effect of chloride ion on the anodic polarization behavior of the Zr65Al7.5Ni10Cu17.5 amorphous alloy in phosphate buffered solution”, Corrosion Science, 2000, vol. 42, pp. 1651-1660. |
Hiromoto et al., “Effect of pH on the polarization behavior of Zr65Al7.5Ni10Cu17.5 amorphous alloy in a phosphate-buffered solution”, Corrosion Science, 2000, vol. 42, pp. 2193-2200. |
Inoue, “Stabilization of Metallic Supercooled Liquid and Bulk Amorphous Alloys”, Acta Materialia, 2000, vol. 48, pp. 279-306. |
Inoue et al., “Bulky La—A1—TM (TM=Transition Metal) Amorphous Alloys with High Tensile Strength Produced by a High-Pressure Die Casting Method”, Materials Transactions, JIM, vol. 34, No. 4, 1993, pp. 351-358. |
Inoue et al., “Mg—Cu—Y Bulk Amorphous Alloys with High Tensile Strength Produced by High-Pressure Die Casting Method”, Materials Transactions, JIM, 1992, vol. 33, No. 10, pp. 937-945. |
Inoue et al., “Preparation of Bulky Amorphous Zr—Al—Co—Ni—Cu Alloys by Copper Mold Casting and Their Thermal and Mechanical Properties”, Materials Transactions, JIM, 1995, vol. 36, No. 3, pp. 391-398. |
Inoue et al., “Production of Fe—P—C amorphous wires by in-rotating-water spinning method and mechanical properties of the wires”, Journal of Materials Science, Feb. 1982, vol. 17, Issue 2, pp. 580-588, doi:10.1007/BF00591492. |
Inoue et al., “Zr—A1—Ni Amorphous Alloys with High Glass Transition Temperature and Significant Supercooled Liquid Region”, Materials Transactions, JIM, 1990, vol. 31, No. 3, pp. 177-183. |
Johnson, “Bulk Glass-Forming Metallic Alloys: Science and Technology”, MRS Bulletin, Oct. 1999, pp. 42-56. |
Johnson et al., “A Universal Criterion for Plastic Yielding of Metallic Glasses with a (T/Tg)2/3 Temperature Dependence”, Physical Review Letters, Nov. 4, 2005, vol. 95, Issue 19, pp. 195501-195501-4, DOI: 10.1103/PhysRevLett.95.195501. |
Jost et al., “The Structure of Amorphous Be—Ti—Zr Alloys”, Zeitschrift fur Physikalische Chemie Neue Folge, Bd. 157, 1988, pp. 11-15. |
Katagiri et al., “An attempt at preparation of corrosion-resistant bulk amorphous Ni—Cr—Ta—Mo—P—B alloys”, Corrosion Science, Jan. 2001, vol. 43, No. 1,pp. 183-191, doi: 10.1016/S0010-938X(00)00068-8. |
Kato et al., “Production of Bulk Amorphous Mg85Y10Cu5 Alloy by Extrusion of Atomized Amorphous Powder”, Materials Transactions, JIM, vol. 35, No. 2, 1994, pp. 125-129. |
Kawamura et al., “Full Strength Compacts by Extrusion of Glassy Metal Powder at the Supercooled Liquid State”, American Institute of Physics, May 30, 1995, vol. 67, No. 14, pp. 2008-2010. |
Kawashima et al., “Change in corrosion behavior of amorphous Ni—P alloys by alloying with chromium, molybdenum or tungsten”, Journal of Non-Crystalline Solids, 1985, vol. 70, No. 1, pp. 69-83. |
Number | Date | Country | |
---|---|---|---|
20200263267 A1 | Aug 2020 | US |
Number | Date | Country | |
---|---|---|---|
62805845 | Feb 2019 | US |