A fast temperature measurement method based on magnetic nanometer magnetization-temperature curve
A magnetization, temperature curve technology, applied in thermometers, thermometers with electrical/magnetic components that are directly sensitive to heat, thermometers that give differences, etc., can solve the problem of low accuracy, slow temperature measurement, and no temperature given. Inversion methods and other issues to achieve high precision and reduce strength
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[0041] Based on this thinking, the embodiment of the present invention is as follows:
[0042] (1) Place the magnetic nano sample at the position to be tested
[0043] Modify the surface of magnetic nanoparticles to make them adsorbable and adsorb on the surface of the measured object, or mix the solid powder of magnetic nanoparticles with an adhesive and apply them to the surface of the measured object.
[0044] (2) Apply a suitable DC magnetic field in the area where the magnetic nanometer is located
[0045] A coil or a permanent magnet can be used to apply a DC magnetic field to the area where the magnetic nanoparticle sample is located, and the magnitude of the applied DC magnetic field can be selected according to the sensitivity of the magnetization to temperature under different DC excitation magnetic fields. figure 2 The derivatives of the magnetization to temperature under the excitation magnetic field of 100gauss, 500gauss, 900gauss and 1300gauss are respectively ...
example
[0058] In order to illustrate the above implementation steps in more detail, a simulation example of sample parameters using EMG1300 magnetic nanoparticles of Ferrotec Company is given below. The average particle size of EMG1300 is 10nm, and the saturation magnetization at room temperature is 50-70emu / g. In the simulation, M s =0.6T / μ 0 , the external magnetic field b=2.8E-5, a=1.65, the curve of magnetization intensity changing with temperature is as follows image 3 shown.
[0059] Using the double exponential function T(t)=A*(e -αt -e -βt )+T0 to simulate a temperature pulse, where the amplitude coefficient A is 100, the reciprocal of the wave tail time constant α is 1 / 300e-9, the front time constant β is 1 / 45e-9, T0 is 300K, t is time, temperature waveform like Figure 5 shown. Taking this temperature pulse as input, the normalized waveform of the coil induction signal obtained is as follows: Image 6 As shown, this signal is integrated and substituted into the ...
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