Rare earth-iron magnetostrictive materials and devices using these materials
AssigneeThe United States of America as represented by the Secretary of the Navy
InventorsHoward T. Savage, Arthur E. Clark, O. Dale McMasters
Life of this patent
Estimating the term…
Abstract
Grain-oriented polycrystalline or single crystal magnetostrictive materials n the general formula Tb.sub.x Dy.sub.1-x Fe.sub.2-w, Tb.sub.x Ho.sub.1-x Fe.sub.2-w, Sm.sub.x Dy.sub.1-x Fe.sub.x-w, Sm.sub.x Ho.sub.1-x Fe.sub.2-w, Tb.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w, or Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w, wherein O.ltoreq.w.ltoreq.0.20, and x+y+z=1. X, y, and z are selected to maximize the magnetostrictive effect and the magnetomechanical coupling coefficient K.sub.33. These material may be used in magnetostrictive transducers, delay lines, variable frequency resonators, and filters.
Claims102
A grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Tb.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.20.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.10.ltoreq.x.ltoreq.1 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Sm.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.80.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.10.ltoreq.x<1.00, 0.ltoreq.y.ltoreq.0.90, 0.ltoreq.z.ltoreq.0.80, and 0.ltoreq.w.ltoreq.0.20, wherein x+y+z=1, and wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.60.ltoreq.x<1.00, 0.ltoreq.y.ltoreq.0.40, 0.ltoreq.z.ltoreq.0.40, and 0.ltoreq.w.ltoreq.0.20, wherein x+y+z=1, and wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A single crystal rare earth-iron magnetostrictive material of the formula TB.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.20.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A single crystal rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.10.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A single crystal rare earth-iron magnetostrictive material of the formula Sm.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.80.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A single crystal rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A single crystal rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w where 0.1.ltoreq.x<1.00, 0.ltoreq.y.ltoreq.0.90, 0.ltoreq.z.ltoreq.0.80, and 0.ltoreq.w.ltoreq.0.20, x+y+z=1 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A single crystal rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.60.ltoreq.x<1.0, 0.ltoreq.y.ltoreq.0.40, 0.ltoreq.z.ltoreq.0.40, and 0.ltoreq.w.ltoreq.0.20, x+y+z=1 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Tb.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.20.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
The transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.10.ltoreq.x.ltoreq.1 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Sm.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.80.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20, wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having an magnetostrictive element comprising:
- a grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.10.ltoreq.x<1.00, 0.ltoreq.y.ltoreq.0.90, 0.ltoreq.z.ltoreq.0.80, and 0.ltoreq.w.ltoreq.0.20, wherein x+y+z=1, and wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magentic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a grain-oriented polycrystalline rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.00, 0.ltoreq.y.ltoreq.0.40, 0.ltoreq.z.ltoreq.0.40, and 0.ltoreq.w.ltoreq.0.20, wherein x+y+z=1, and wherein the grains of the material have their common principal axes substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a single crystal rare earth-iron magnetostrictive material of the formula Tb.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.20.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree.0 of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a single crystal rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.10.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a single crystal rare earth-iron magnetostrictive material of the formula Sm.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.80.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a single crystal rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.00 and 0.ltoreq.w.ltoreq.0.20 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a single crystal rare earth-iron magnetostrictive material of the formula Tb.sub.x Ho.sub.Y Dy.sub.z Fe.sub.2-w wherein 0.1.ltoreq.x.ltoreq.1.00, 0.ltoreq.y.ltoreq.0.90, 0.ltoreq.z.ltoreq.0.80, and 0.ltoreq.w.ltoreq.0.20, x+y+z=1 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A transducer for converting magnetic energy into mechanical energy or vice versa having a magnetostrictive element comprising:
- a single crystal rare earth-iron magnetostrictive material of the formula Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.0, 0.ltoreq.y.ltoreq.0.40, 0.ltoreq.z.ltoreq.0.40, and 0.ltoreq.w.ltoreq.0.20, x+y+z=1 having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis.
A device for varying the velocity of sound waves comprising:
- (1) a sound wave transmission element comprising a grain-oriented polycrystalline magnetostrictive material selected from the group consisting of
- (a) Tb.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.20.ltoreq.x.ltoreq.1.00;
- (b) Tb.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.10.ltoreq.x.ltoreq.1.00;
- (c) Sm.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.80.ltoreq.x.ltoreq.1.00;
- (d) Sm.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.00;
- (e) Tb.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.10.ltoreq.x.ltoreq.1.00;
- 0 y 0.90, 0 z 0.80, and
- x+y+z=1;
- and
- (f) Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.60x<1.00, 0.ltoreq.y.ltoreq.0.40, 0.ltoreq.z.ltoreq.0.40, and x+y+z=1;
- wherein 0.ltoreq.w.ltoreq.0.20 for (a) through (f) and wherein the grains of the material have their common principal axis substantially pointed along the growth axis of the material which is within 10.degree. of the .lambda..sub.111 axis;
- and
- (2) means for generating a magnetic field of adjustable strength in the transmission element.
A device for varying the velocity of sound waves comprising:
- (1) a sound wave transmission element comprising a single crystal of a magnetostrictive material selected from the group consisting of
- (a) Tb.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.20.ltoreq.x.ltoreq.1.00;
- (b) Tb.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.10.ltoreq.x.ltoreq.1.00;
- (c) Sm.sub.x Dy.sub.1-x Fe.sub.2-w wherein 0.80.ltoreq.x.ltoreq.1.00;
- (d) Sm.sub.x Ho.sub.1-x Fe.sub.2-w wherein 0.60.ltoreq.x.ltoreq.1.00;
- (e) Tb.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.10.ltoreq.x<1.00, 0.ltoreq.y.ltoreq.0.90, 0.ltoreq.z.ltoreq.0.80, and x+y+z=1;
- and
- (f) Sm.sub.x Ho.sub.y Dy.sub.z Fe.sub.2-w wherein 0.60.ltoreq.x<1.00, 0.ltoreq.y.ltoreq.0.40, 0.ltoreq.z.ltoreq.0.40, and x+y+z=1;
- wherein 0.ltoreq.w.ltoreq.0.20 for (a) through (f) having angle grain boundaries of less than 5.degree., wherein the principal axis of the Laves phase is pointed along the growth axis of the material which is within 10.degree. of the .sub.111 axis;
- and
- (2) means for generating a magnetic field of adjustable strength in the transmission element.
Dependencies are inferred from the claim text.