Magnetic refrigeration apparatus and method

Claim 1

A method of refrigeration approximating a Brayton cycle utilizing near its Curie temperature, a ferromagnetic body which is geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, said body being rotatable about an axis substantially perpendicular to the field between substantially magnetized and substantially demagnetized positions, and an internal heat exchange fluid containing regenerator slidably positioned about the body along the axis between a bottom position and a top position and thermally communicating with two external heat exchange transfer fluids, the method comprising the steps of: (a) positioning the regenerator and body in a substantially demagnetized orientation within the field at a temperature essentially T H , the body being oriented so that its demagnetizing factor due to its geometric structure is near unity, the regenerator being in its bottom position; (b) rotating the body within the regenerator to a substantially magnetized position, thereby magnetizing the body and increasing its temperature from essentially T H to essentially T H +Δ T H ; (c) moving the generator from its bottom position to its top position, thereby warming the internal heat exchange fluid therein and cooling the still magnetized body to a temperature of essentially T C ; (d) again rotating the body within the regenerator to a substantially demagnetized position to adiabatically demagnetize the body from its temperature of essentially T C to a temperature of essentially T C -Δ T C ; (e) moving the regenerator to its bottom position to cool the internal heat exchange fluid therein and warm the body to essentially T H ; and (f) transferring heat from the internal heat exchange fluid appropriately during the cycle to two external heat exchange transfer fluids to accomplish refrigeration.

Claim 2

A method of refrigeration approximating a Brayton cycle utilizing near its Curie temperature, a ferromagnetic body which is geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, said body being rotatable about an axis substantially perpendicular to the field between substantially magnetized and substantially demagnetized positions, and an internal heat exchange fluid containing regenerator slidably positioned about the body along the axis between a bottom position and a top position and thermally communicating with two external heat exchange transfer fluids, the method comprising the steps of: (a) positioning the regenerator and body in a substantially demagnetized orientation within the field at a temperature essentially T H , the body being oriented so that its demagnetizing factor due to its geometric structure is near unity, the regenerator being in its bottom position; (b) rotating the body within the regenerator to a substantially magnetized position, thereby magnetizing the body and increasing its temperature from essentially T H to essentially T H +Δ T H ; (c) moving the generator from its bottom position to its top position, thereby warming the internal heat exchange fluid therein and cooling the still magnetized body to a temperature of essentially T C ; (d) again rotating the body within the regenerator to a substantially demagnetized position to adiabatically demagnetize the body from its temperature of essentially T C to a temperature of essentially T C -Δ T C ; (e) moving the regenerator to its bottom position to cool the internal heat exchange fluid therein and warm the body to essentially T H ; and (f) transferring heat from the internal heat exchange fluid appropriately during the cycle to two external heat exchange transfer fluids to accomplish refrigeration.

Claim 3

A method of refrigeration approximating a Carnot cycle utilizing near its Curie temperature a ferromagnetic body which is geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, said body being rotatable about an axis substantially perpendicular to the field between substantially magnetized and substantially demagnetized positions, and an internal two-phase heat exchange fluid containing housing disposed over the body, said housing thermally communicating with first and second external two-phase fluids, the method comprising the steps of: (a) locating the housing enclosed body within the field at a temperature essentially T C with the body oriented in a substantially demagnetized orientation; (b) rotating the body to a state of partail magnetization, thereby causing an adiabatic temperature rise within the body from essentially T C to essentially T H ; (c) continuing the rotation of the body while transferring heat from the body to the first of the two-phase fluids during the completion of the rotation to a magnetized orientation, thereby creating an isothermal magnetization of the body; (d) partially rotating the body within the field towards a demagnetized orientation thereby causing a temperature decrease back to essentially T C , completing rotation of the body to a demagnetized orientation during which heat is transferred to the second two-phase fluid; and (e) transferring heat from the first and second two-phase fluids at appropriate times to external heat sink and source to accomplish refrigeration.

Claim 4

A method of refrigeration approximating a Carnot cycle utilizing near its Curie temperature a ferromagnetic body which is geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, said body being rotatable about an axis substantially perpendicular to the field between substantially magnetized and substantially demagnetized positions, and an internal two-phase heat exchange fluid containing housing disposed over the body, said housing thermally communicating with first and second external two-phase fluids, the method comprising the steps of: (a) locating the housing enclosed body within the field at a temperature essentially T C with the body oriented in a substantially demagnetized orientation; (b) rotating the body to a state of partail magnetization, thereby causing an adiabatic temperature rise within the body from essentially T C to essentially T H ; (c) continuing the rotation of the body while transferring heat from the body to the first of the two-phase fluids during the completion of the rotation to a magnetized orientation, thereby creating an isothermal magnetization of the body; (d) partially rotating the body within the field towards a demagnetized orientation thereby causing a temperature decrease back to essentially T C , completing rotation of the body to a demagnetized orientation during which heat is transferred to the second two-phase fluid; and (e) transferring heat from the first and second two-phase fluids at appropriate times to external heat sink and source to accomplish refrigeration.

Claim 6

A method of refrigeration approximating an Ericsson cycle utilizing, near its Curie temperature, a ferromagnetic body disposed in a magnetic field, the body being geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, the body being rotatable about an axis perpendicular to the field, an internal heat exchange fluid containing regenerator slidably positionable over the body, along the axis between a bottom position and a top position, the method comprising the steps of: (a) positioning the body within the field at a temperature of essentially T H with the body disposed in a substantially magnetized orientation; (b) rotating the body within the field to a substantially demagnetized orientation while transferring heat to a first external two-phase fluid or a first very large thermal mass, resultring in isothermal demagnetization of the body; (c) cooling the body with the internal regenerator fluid, thereby causing it to reach a temperature of essentially T C with the body still in the substantially demagnetized orientation; (d) rotating the body to a substantially magnetized orientation while transferring heat to a second external two-phase fluid or second very large thermal mass so that the body remains essentially at temperature T C ; (e) increasing the temperature of the body from essentially T C to essentially T H by moving the regenerator from its bottom position to its top position.

Claim 7

A method of refrigeration approximating an Ericsson cycle utilizing, near its Curie temperature, a ferromagnetic body disposed in a magnetic field, the body being geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, the body being rotatable about an axis perpendicular to the field, an internal heat exchange fluid containing regenerator slidably positionable over the body, along the axis between a bottom position and a top position, the method comprising the steps of: (a) positioning the body within the field at a temperature of essentially T H with the body disposed in a substantially magnetized orientation; (b) rotating the body within the field to a substantially demagnetized orientation while transferring heat to a first external two-phase fluid or a first very large thermal mass, resultring in isothermal demagnetization of the body; (c) cooling the body with the internal regenerator fluid, thereby causing it to reach a temperature of essentially T C with the body still in the substantially demagnetized orientation; (d) rotating the body to a substantially magnetized orientation while transferring heat to a second external two-phase fluid or second very large thermal mass so that the body remains essentially at temperature T C ; (e) increasing the temperature of the body from essentially T C to essentially T H by moving the regenerator from its bottom position to its top position.

Claim 9

A method of refrigeration approximately a Stirling cycle utilizing, near its Curie temperature, a ferromagnetic body which is geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, the body being rotatable about an axis perpendicular to the field, an internal heat exchange fluid containing regenerator slidable disposed about the body, the regenerator being slidable over the body along the axis between a bottom position and a top position, the method comprising the steps of: (a) positioning the body at a first temperature of essentailly T H at an orientation partially rotated from a substantially demagnetized orientation so that it is partially magnetized; (b) rotating the body to a substantially magnetized orientation and transferring heat from the body to a first external two-phase fluid or first very large thermal mass; (c) cooling the body with the internal regenerator fluid to a temperature of essentially T C as it is rotated to maintain constant magnetization; (d) utilizing a second external two-phase fluid or second very large thermal mass to cause an isothermal substantially complete demagnetization of the body as it is rotated to an orientation of complete demagnetization; (e) utilizing the regenerator fluid to warm the body to a temperature of essentially T H ; and (f) partially rotating the body to maintain constant magnetization, thereby bringing the body to essentially temperature T H .

Claim 10

A method of refrigeration approximately a Stirling cycle utilizing, near its Curie temperature, a ferromagnetic body which is geometrically structured to undergo magnetization and demagnetization in accordance with its orientation in a magnetic field, the body being rotatable about an axis perpendicular to the field, an internal heat exchange fluid containing regenerator slidable disposed about the body, the regenerator being slidable over the body along the axis between a bottom position and a top position, the method comprising the steps of: (a) positioning the body at a first temperature of essentailly T H at an orientation partially rotated from a substantially demagnetized orientation so that it is partially magnetized; (b) rotating the body to a substantially magnetized orientation and transferring heat from the body to a first external two-phase fluid or first very large thermal mass; (c) cooling the body with the internal regenerator fluid to a temperature of essentially T C as it is rotated to maintain constant magnetization; (d) utilizing a second external two-phase fluid or second very large thermal mass to cause an isothermal substantially complete demagnetization of the body as it is rotated to an orientation of complete demagnetization; (e) utilizing the regenerator fluid to warm the body to a temperature of essentially T H ; and (f) partially rotating the body to maintain constant magnetization, thereby bringing the body to essentially temperature T H .