초록 ▼

A method of more accurately measuring the true surface temperature of metal alloy objects without contacting the same. The surfaces of the objects have unknown emissivities that change and that are less than unity. The method includes the step of providing objects having surfaces that radiate infrar

A method of more accurately measuring the true surface temperature of metal alloy objects without contacting the same. The surfaces of the objects have unknown emissivities that change and that are less than unity. The method includes the step of providing objects having surfaces that radiate infrared energy. The radiated energy is measured at two wavelengths, and a first measurement is provided that is a function of the ratio of the energies at the two wavelengths. The radiated energy is also measured at a single, narrow band wavelength, and a second measurement is provided that is a function of the radiated energy. The two measurements are then electrically combined to provide measurements of radiated energy and thus temperature measurements that are or at least are closer to the true temperature than either of the first or second measurements.

대표청구항 ▼

A method of measuring the surface temperature of heated metal objects having changing unknown emissivities that are less than unity, the method comprising the steps of: providing an object having a heated surface radiating infrared energy therefrom; determining true surface temperature of the object

A method of measuring the surface temperature of heated metal objects having changing unknown emissivities that are less than unity, the method comprising the steps of: providing an object having a heated surface radiating infrared energy therefrom; determining true surface temperature of the object by making an initial measurement thereof that is separate from measurements of infrared energy radiating from the object; measuring infrared energy radiated from a narrow selected portion of the surface at two different, but closely adjoining wavelengths; rationing the measurements of the energies at the two wavelengths to provide a first output signal that is a function of the ratio of the infrared energies radiating from the selected portion of the surface at the two wavelengths; simultaneous with the step of measuring the infrared energies at the two closely adjoining wavelengths, measuring infrared energy radiating from the same narrow selected portion of the surface at one of the wavelengths and providing therefrom a second output signal that is a function of the radiated infrared energy at the one wavelength; said first measurement and output signal containing errors in the amount of infrared energy radiated from the surface due to the changing emissivities thereof such that the first output signal represents a temperature value that is greater than the true temperature of the surface; said second measurement and second output signal containing errors in the amount of infrared energy radiated from the surface due to the changing emissivities thereof such that the second output signal represents a temperature value that is less than the true temperature of the surface, and by an amount that is considerably greater than the amount that the temperature value of the first output signal is different from the true temperature; correcting for the changing unknown emissivities that affect the amount of infrared energy radiated from the surface by electrically adding the output signals of the first or second measurements; selecting proportions of the output signals in a manner that allows use of the first or second measurement, or any combination thereof; and providing thereby means to adjust the output signal such that it represents the true surface temperature, as determined by the initial, separate measurement of true surface temperature.