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CHAPTER 4: Manufacturing and Experimental Testing of the Developed Compressed Air RIT uncorrelated and also that there are no systematic errors. If the calculated quantity (Y) is a function of k measurements (x1 to xk) each with its own uncertainty (ΞΆπ₯1 to ΞΆπ₯π ), then the uncertainty in Y(ΞΆπ¦) can be divided into its elemental uncertainties due to each of measured variables as following: π = π(π₯1,π₯2,π₯3,....,π₯π) Equation 4-4 ππ,π₯ = ππ ππ₯ Equation 4-5 π ππ₯π π The elemental uncertainties are combined to provide the total uncertainty in Y as below: β πΏπ 2 πΏπ 2 πΏπ 2 Equation4-6 ππ¦ = (πΏπ₯ ππ₯1) +(πΏπ₯ ππ₯2) +β―+(πΏπ₯ ππ₯π) 12π 4.3.5.1. Uncertainty propagation in temperature measurements As previously mentioned, T-type thermocouples were used in the current test rig and they were all calibrated against PT100 RTD thermocouple with the accuracy of Β±0.04 ΜC (refer to Appendix A). Table 4-1 summarizes the calibration curve formulas for all thermocouples and their associated uncertainty. Details of the uncertainty calculation for thermocouples based on the discussion in section 4.3.5 are presented in Appendix A. According to Table 4-1 average uncertainty of the thermocouples was found to be Β±0.699 ΜC. 140 | P a g ePDF Image | SMALL-SCALE RADIAL INFLOW TURBINE FOR WHR ORC
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