Basic Thermodynamic Formulas (Exam Equation Sheet) Control Mass (no mass flow across system boundaries) Conservation of mass: = Equations for Work Done in Various Processes 3. stream << /Type /XObject /Subtype /Form /FormType 1 /PTEX.FileName (./thermodynamics.pdf) /PTEX.PageNumber 1 /PTEX.InfoDict 48 0 R /BBox [ 0 0 864 1296 ] /Group 49 0 R /Resources << /Font << /F1 50 0 R /F2 51 0 R /F4 52 0 R /F5 53 0 R /F14 54 0 R >> /XObject << /Meta9 55 0 R /Meta18 56 0 R /Meta21 57 0 R /Meta28 58 0 R /Meta33 59 0 R /Meta38 60 0 R /Meta43 61 0 R /Meta58 62 0 R /Meta75 63 0 R /Meta86 64 0 R /Meta91 65 0 R /Meta100 66 0 R /Meta109 67 0 R /Meta122 68 0 R /Meta142 69 0 R /Meta149 70 0 R /Meta150 71 0 R /Meta151 72 0 R /Meta160 73 0 R /Meta161 74 0 R /Meta162 75 0 R /Meta165 76 0 R /Meta168 77 0 R /Meta173 78 0 R /Meta178 79 0 R /Meta185 80 0 R /Meta186 81 0 R /Meta189 82 0 R /Meta198 83 0 R /Meta211 84 0 R /Meta216 85 0 R /Meta217 86 0 R /Meta222 87 0 R /Meta235 88 0 R /Meta238 89 0 R /Meta241 90 0 R /Meta242 91 0 R /Meta243 92 0 R /Meta244 93 0 R /Meta250 94 0 R /Meta251 95 0 R /Meta252 96 0 R /Meta253 97 0 R /Meta254 98 0 R /Meta255 99 0 R /Meta256 100 0 R /Meta257 101 0 R /Meta258 102 0 R /Meta259 103 0 R /Meta260 104 0 R /Meta261 105 0 R /Meta262 106 0 R /Meta263 107 0 R /Meta264 108 0 R /Meta265 109 0 R /Meta266 110 0 R /Meta267 111 0 R /Meta268 112 0 R /Meta269 113 0 R /Meta270 114 0 R /Meta271 115 0 R /Meta274 116 0 R /Meta275 117 0 R /Meta276 118 0 R >> /ExtGState << /GS10 119 0 R /GS13 120 0 R >> /ProcSet [ /PDF /Text /ImageB /ImageC /ImageI ] >> /Length 11961 /Filter /FlateDecode >> The system is doing work on the surroundings. Mechanical and Thermodynamic Work 2. x��ZK��������heE��վu+�,����a��%��>H9ٱ�cX�!

Let us consider a battery and motor system . When the temperature changes, the values of the thermometric properties change proportionately. xڥ�MO1���s�=��i�3��Q�܌{# �P��1�{�~ ABLL�L�w�'��ZX��[sU��Xa��'CY�@Qj�:��p嬞۹�xSLQQ�( Copyright 10. The value of absolute zero on this scale is same as that given by Absolute temperature scale i.e., – 273.16°C. Traffic: Volume Studies, Flow Characteristics and Forecasting | Engineering, Unconventional Machining Processes: AJM, EBM, LBM & PAM | Manufacturing, Material Properties: Alloying, Heat Treatment, Mechanical Working and Recrystallization, Design of Gating System | Casting | Manufacturing Science, Forming Process: Forming Operations of Materials | Manufacturing Science, Generative Manufacturing Process and its Types | Manufacturing Science, Equations for Work Done in Various Processes, Thermometers and Measurement of Temperature. Thermodynamic Work: Equations, PdV-Work, Heat, Pressure and Temperature Measurement. << /Type /XObject /Subtype /Form /BBox [ 0 0 767 1189 ] /FormType 1 /Matrix [ 1 0 0 1 0 0 ] /Resources 46 0 R /Length 37 /Filter /FlateDecode >> Revision : Electricity. ?�÷�y�N:b'm�-�G��S��������rr��?�_�/?���r�������O��/��á^��٨N1�5'���q-0����. Keywords Print pdf and hang near your desk for quick reference. In a constant volume gas thermometer, gas will be used as the working substance and as all the gases behave as ideal gases at low pressure, thus scale is known as Ideal gas temperature scale. my thermodynamics cheat sheets Nasser M. Abbasi Sumemr 2004 Compiled on May 23, 2020 at 4:09am 1. all of theormodynamics in one sheet. %%EOF Also includes the value of Physical Constants. x��=]�G����Q������l�����l�C��l����k�Xܿ��w$�[j��R��5A�Z�n�X$�d�����VW���ɓ��W�����e�����/�|���/���柮n竫���gՋW/��{��{Q Y����#Q5���������5�'��o�=�yV���z��w�^Ã��/�����jy�n������� �����] �^�]���/��˳s=���/���3!gs��������*��8[��_a:��T�M-�P��B§��s����?�R���� Work is a Path Function and Properties are Point Functions: It is possible to take a system from state (1) to state (2) by following many quasi-static paths such as A, B, C etc: Now if we consider the path 1-A-2, then the work done during the process 1-A-2 will be equal to the area under the curve 1-A-2 and if we consider path 1-B-2, then the work done during the path 1-B-2 will be equal to the area under the curve 1-B-2. endobj If the pressure of the system is less (i.e., s -ve pressure) than the atmo­spheric pressure, its gauge pressure is –ve and it is known as vacuum and. The anal-ysis of thermal systems is achieved through the application of the governing conservation equations, namely Conservation of Mass, Conservation of Energy (1st law of thermodynam-ics), the 2nd law of thermodynamics and the property relations. (a) PDF (b) image 2. polytropic process diagrams (a) PDF (b) image 3. first and second laws diagrams (a) PDF (b) image 4. Thus from this equation, we can construct a scale and calibrate it to give us direct temperature readings.

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