ADVANCED THERMODYNAMICS ENGINEERING phần 9 pdf

ADVANCED THERMODYNAMICS ENGINEERING phần 9 pdf

ADVANCED THERMODYNAMICS ENGINEERING phần 9 pdf

... 361 .93 0. 097 6 17.1488 0.14088 Nitric Oxide NO 30.01 180 65 0.252 0.058 0.588 1 09. 5 121.4 76.7 460.5 19. 76 0.0 199 1.45357 0.02878 Nitrogen N 2 28.02 126.2 33 .9 0.2 89 0.0 895 0.0 39 63.3 77.4 25.7 199 .2 ... 144.45 0.0 394 6.86 798 0.05682 Sulfur trioxide SO 3 80.06 490 .9 82.07 0.256 0.1271 0.422 290 .0 317 .9 24.6 502.5 192 .24 0.0431 8.5626 0.06216 Sulfuric acid H 2 SO 4 98 .0...
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ADVANCED THERMODYNAMICS ENGINEERING phần 3 pdf

ADVANCED THERMODYNAMICS ENGINEERING phần 3 pdf

... P 3 /P 2 = T 3 /T 2 = 90 0÷574 , i.e., P 3 = 15.68 atm, and s 3 = 2.8 49 – 0.287 ln (15.68÷1) = 2.0 59 kJ kg –1 K –1 . Therefore, 2.0 59 – 1.702 – (2 89/ 1000) – (– 29/ 298 ) = σ so that σ = 0.165 ... ln(350 ÷ 273) = 1.0 395 kJ K –1 . Similarly, at temperatures of 3 49. 5, 3 49, 348.5, , K, S W = 1.0336, 1.0276, , kJ K –1 . For a 0.5 K temperature drop dS W = 1.0336 – 1.0 395 = –0....
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Software Engineering (phần 9) pdf

Software Engineering (phần 9) pdf

... River. NJ, 199 5. 1 (Bowen and Hinchev, 1 99 5a1 J. P. BOwEN AND M. G. HINCHEY, ifrlkn Commandments Of .j 'e '' ' ; Formal Methods,'' IEEE Computer 28 (April 1 99 5). pp. ... Electric Re- Jonsson, and Overgaard, 199 21 in Sweden, starting in i search and Development Center in Schenectady, New 1 96 7. Version 1.0 of UM L was published in 199 7. lt ' ! !Yo...
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ADVANCED THERMODYNAMICS ENGINEERING phần 1 ppt

ADVANCED THERMODYNAMICS ENGINEERING phần 1 ppt

... in –2 0.1450 PE potential energy kJ BTU 0 .94 78 pe specific potential energy Q heat transfer kJ BTU 0 .94 78 q heat transfer per unit mass kJ kg –1 BTU lb –1 0.4 299 q c charge R gas constant kJ kg –1 ... R –1 0.2388 T temperature °C, K °F, °R (9/ 5)T+32 T temperature °C, K °R 1.8 t time s s U internal energy kJ BTU 0 .94 78 u specific internal energy kJ kg –1 BTU lb –1 0.4 299 u interna...
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ADVANCED THERMODYNAMICS ENGINEERING phần 2 ppsx

ADVANCED THERMODYNAMICS ENGINEERING phần 2 ppsx

... Air Composition Species Mole % Mass % Ar 0 .93 4 1.288 CO 2 0.033 0.050 N 2 78.084 75.521 O 2 20 .94 6 23.1 39 Rare gases 0.003 0.002 Molecular Weight: 28 .96 kg kmole –1 . 2. Proof of the Euler Equation Assume ... ∂∂∂∂ (92 ) The LHS of Eq. (94 ) is a vector called curl r F . If rr ∇×F = 0, then the two are parallel to each other, i.e., the vector field is irrotational. Assume that r F =...
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ADVANCED THERMODYNAMICS ENGINEERING phần 4 potx

ADVANCED THERMODYNAMICS ENGINEERING phần 4 potx

... –T 0 ) = 4 .97 . = 6203 – 298 × (205.0 – 8.314 × ln (0.21/1)) + 100 × (0.08314 × 298 /0.21) = –4 698 1 kJ kmole –1 . Likewise, φ N 2 ,∞ (T 0 ,p N2 , ∞ ) = 6 190 – 298 × ( 191 .5 – 8.314 × ln (0. 79/ 1)) + ... =1 × 673 – 298 × (1 × ln (673/ 298 )) = 430.2 kJ kg –1 , ψ a,e = 473 – 298 × 1 × ln (473/ 298 ) = 335.3 kJ kg –1 , ψ w,i = 4 19 – 298 × 1.31 = 28.6 kJ kg –1 , and ψ w,e = 2676.1 –...
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ADVANCED THERMODYNAMICS ENGINEERING phần 5 potx

ADVANCED THERMODYNAMICS ENGINEERING phần 5 potx

... and used in Eq. ( 69) to determine ω. ii. Empirical Relations Empirical relations are also available, e.g., ω = (ln P R sat – 5 .92 714 + 6. 096 4/T R,BP +1.28862 ln T R,BP – 0.1 693 5 T R,BP )/ (15.2578 ... R–134a, c f = 1.464 kJ kg –1 K –1 , and c p,o at 298 K = 0.851 kJ kg –1 K –1 . Using the values for P = 690 kPa, R = 0.081 49 kJ kg –1 K –1 , c vo = 0.7 697 kJ kg –1 K –1 , v f...
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ADVANCED THERMODYNAMICS ENGINEERING phần 6 ppt

ADVANCED THERMODYNAMICS ENGINEERING phần 6 ppt

... 2501.3 233.18 13 89. 0 215.188 524.534 1 69. 59 A o 30.54 22.54 16.778 17.2 29 29. 75 28.58 29. 15 19 26.765 † B o 0.01030 0.1141077 0.2865 0.4757 .025 .00377 –.001573 0.17 594 † C o 0.0 130 196 .35 0 0 –154808. ... subscript “o” µ N 2 , .mix = µ N 2 ( 298 , 2 bar) + RT ln X N 2 = 298 – 298 ×(ln( 298 ÷273) – 0. 297 ×ln(2÷1)) + 0. 297 × 298 ln(0.6) A mixture contains 60% N 2 and 40% O 2...
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ADVANCED THERMODYNAMICS ENGINEERING phần 7 ppt

ADVANCED THERMODYNAMICS ENGINEERING phần 7 ppt

... liquid) (cf. Figure 11), σ = ( 95 30.5 – ( 97 76.2))÷ 593 = 0.414 kJ kmole -1 K -1 , while for a change from D to the metastable vapor state K, σ = ( 95 30.5 – ( 96 38.8)) ÷ 593 = 0.183 k kmole -1 K - . -4000 -3500 -3000 -2500 -2000 -1500 -1000 -500 0 500 1000 0 ... ¯s = 1 49. 83 kJ kmole –1 . The state is represented by point D in the figure, and the extensive 146 146.5 147 147.5 148 1...
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ADVANCED THERMODYNAMICS ENGINEERING phần 8 doc

ADVANCED THERMODYNAMICS ENGINEERING phần 8 doc

... Hence, p O 2 = X O 2 P = (50– 0.0005) ÷(0.001+(50–0.0005)) = 0 .99 99 P = 0 .99 99 bar. Therefore, s O 2 = 205.03 – 8.314 × ln 0 .99 99 = 205.03 kJ K –1 kmole –1 , i.e., -6.0E+05 -5.0E+05 -4.0E+05 -3.0E+05 -2.0E+05 -1.0E+05 0.0E+00 0.0 ... h HO 2 – T s HO 2 = –285830 – 298 × 69. 95 = –306675 kJ kmole –1 of H 2 O(l) , g CO o = –110530 – 298 × 197 .56 = –1 694 03 kJ kmole –1 of CO,...
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