A method and apparatus for accurately mapping the closed magnetic circuit demagnetisation curve to and from a open magnetic circuit demagnetisation curve. The method utilises open circuit data from a pulsed field magnetometer (PFM) and computer modelling of both the PFM (open circuit) and permeameter (closed circuit) apparatus. This method is more accurate than previous methods and can calculate the closed circuit curve within the precision of both the PFM and the permeameter apparatus.

A test and measurement instrument for determining magnetic core losses of a device under test during in circuit operation. The test and measurement instrument receives a primary current signal from a primary winding of a device under test and receives a primary voltage signal measured across a magnetic core of the device under test. Based on the primary electric current signal and the primary voltage signal, the test and measurement instrument determines a magnetic loss of the device under test. In some examples, the test and measurement instrument can use primary and secondary voltage and current inputs to determine the magnetic loss of the device under test. The magnetic loss of the device under test can be displayed on a display of the test and measurement instrument. The magnetic loss can include a total magnetic loss, a hysteresis loss, a copper loss, and/or other losses.

A test and measurement instrument for determining magnetic core losses of a device under test during in circuit operation. The test and measurement instrument receives a primary current signal from a primary winding of a device under test and receives a primary voltage signal measured across a magnetic core of the device under test. Based on the primary electric current signal and the primary voltage signal, the test and measurement instrument determines a magnetic loss of the device under test. In some examples, the test and measurement instrument can use primary and secondary voltage and current inputs to determine the magnetic loss of the device under test. The magnetic loss of the device under test can be displayed on a display of the test and measurement instrument. The magnetic loss can include a total magnetic loss, a hysteresis loss, a copper loss, and/or other losses.

A method for measuring a temperature of magnetic junction switchable using spin transfer. The magnetic junction includes at least one magnetic layer. The method includes measuring a temperature variation of at least one magnetic characteristic for the magnetic layer(s) versus temperature. The method also includes measuring a bias variation in the magnetic characteristic versus an electrical bias for the magnetic junction. This measurement is performed such that spin transfer torque-induced variation(s) in the magnetic characteristic(s) are accounted for. The temperature versus the electrical bias for the magnetic junction is determined based on the temperature variation and the bias variation.

A method for measuring a temperature of magnetic junction switchable using spin transfer. The magnetic junction includes at least one magnetic layer. The method includes measuring a temperature variation of at least one magnetic characteristic for the magnetic layer(s) versus temperature. The method also includes measuring a bias variation in the magnetic characteristic versus an electrical bias for the magnetic junction. This measurement is performed such that spin transfer torque-induced variation(s) in the magnetic characteristic(s) are accounted for. The temperature versus the electrical bias for the magnetic junction is determined based on the temperature variation and the bias variation.

A method for measuring a temperature of magnetic junction switchable using spin transfer. The magnetic junction includes at least one magnetic layer. The method includes measuring a temperature variation of at least one magnetic characteristic for the magnetic layer(s) versus temperature. The method also includes measuring a bias variation in the magnetic characteristic versus an electrical bias for the magnetic junction. This measurement is performed such that spin transfer torque-induced variation(s) in the magnetic characteristic(s) are accounted for. The temperature versus the electrical bias for the magnetic junction is determined based on the temperature variation and the bias variation.

A method for measuring a temperature of magnetic junction switchable using spin transfer. The magnetic junction includes at least one magnetic layer. The method includes measuring a temperature variation of at least one magnetic characteristic for the magnetic layer(s) versus temperature. The method also includes measuring a bias variation in the magnetic characteristic versus an electrical bias for the magnetic junction. This measurement is performed such that spin transfer torque-induced variation(s) in the magnetic characteristic(s) are accounted for. The temperature versus the electrical bias for the magnetic junction is determined based on the temperature variation and the bias variation.

The present invention relates to a device and a method for measuring a magnetic field and, more particularly, to a device and a method for measuring a magnetic field, wherein a spin current is in into a magnetic body that has magnetic anisotropy using a spin Hall effect occurring in a current applied to a conductor, and the degree of shift of hysteresis in the magnetic body is calculated while reversing the magnetization of the magnetic body by a spin torque such that an external magnetic field applied to the magnetic body can be measured precisely. The present invention provides a magnetic field measuring device for measuring a first magnetic field applied from the outside, the magnetic field measuring device comprising: a current applying means for applying a current to a conductor; a conductor that receives the current from the current applying means and forms a spin current therein; a magnetic body having magnetic anisotropy such that the spin current formed in the magnetic body injected therein; a magnetic field applying means for applying a second magnetic field to the magnetic body; and a control unit for deriving the degree of shift of hysteresis of the magnetic body following application of the first magnetic field, with regard to the hysteresis of the magnetic body while the first magnetic field has not been applied, and calculating the intensity of the first magnetic field using the same.

The present invention relates to a device and a method for measuring a magnetic field and, more particularly, to a device and a method for measuring a magnetic field, wherein a spin current is in into a magnetic body that has magnetic anisotropy using a spin Hall effect occurring in a current applied to a conductor, and the degree of shift of hysteresis in the magnetic body is calculated while reversing the magnetization of the magnetic body by a spin torque such that an external magnetic field applied to the magnetic body can be measured precisely. The present invention provides a magnetic field measuring device for measuring a first magnetic field applied from the outside, the magnetic field measuring device comprising: a current applying means for applying a current to a conductor; a conductor that receives the current from the current applying means and forms a spin current therein; a magnetic body having magnetic anisotropy such that the spin current formed in the magnetic body injected therein; a magnetic field applying means for applying a second magnetic field to the magnetic body; and a control unit for deriving the degree of shift of hysteresis of the magnetic body following application of the first magnetic field, with regard to the hysteresis of the magnetic body while the first magnetic field has not been applied, and calculating the intensity of the first magnetic field using the same.

A calculating method for ultimate demagnetization temperature of loudspeaker magnetic steel includes drawing a 2D or 3D geometric model view of the system; importing the performance parameter of magnetic steel and designing variables to be solved and formulas; establishing a finite element model for the system according to the imported performance parameter of magnetic steel, variables and formulas; solving and conducting a steady-state analysis of the finite element model for a coordinate (Hn, Bn), a loadline slope Pc value and an ultimate demagnetization temperature value of the operation point under 20 C. on BH curve by calculating; obtaining a demagnetization curve view with post-treatment. Thus, a value of loadline slope Pc is obtained, and the ultimate demagnetization temperature of loudspeaker magnetic steel can be obtained importing the variables and formulas into FEA simulation through the temperature coefficient of magnetic steel and by the solution and steady-state analysis using COMSOL Multiphysics software.