(1) Work and Energy Relations Wb = ∫ pdV EQUATIONS FOR MAE 3524 W= VI ∆t e ks 2 ( x2 − x12 ) 2 W= spring 2 Wrot = 2π nτ ΔKE = 1 m (V22 - V12 ) 2 wcv =− ∫ νdp + (V12 − V22 ) / 2 + g ( z1 − z2 ) 1 ΔPE = mg ( z2 - z1 ) Fspring = ks x (2) First Law Relations and Mass Conservation ∆Ε = ∆U + ∆KE + ∆PE = Q − W dEcv = Qcv - Wcv + ∑ m i ( h + V 2 / 2 + gz ) - ∑ m e ( h + V 2 / 2 + gz ) i e dt i e m = ρVA (3) dmcv = ∑ m i - ∑ m e dt i e ν 2 δ q ∆s =∫ ∫1 1 T int,rev Q j dScv = ∑ m i si − ∑ m e se + ∑ +σ cv dt i e j Tj 2 δ Q T + σ b Q dS = ∑ j + σ dt j Tj δQ = -σ ≤ 0 T b ∫ Pressure, Temperature and Energy Relations pabs = patm ± p gage pV = nRT pR = p / pc p − patm = ρgL = V ν m pV = mRT R=R M ν R =ν pc / RTc TR = T / Tc Pν =ZRT k = Cp /C v x = m g /(m f + m g ) y = (1 − x ) y f + xy g = y f + xy fg y fg = y g − y f h= u + Pv ∆u = ∫ c v dT ∆h = ∫ c p dT Cp - Cv = R ∆h = ∆u + ν∆p h (T,p ) ≅ h f (T )+ν f (T )[p - psat (T )] ν(T,p ) ≅ ν f (T ) s(T,p) ≅ s f (T) ∆u = ∫ cdT (5) V Second Law Relations = ∆S (4) m = u(T,p) ≅ u f (T) Entropy Relations (and Isentropic Processes) Tds = du + pd ν T ν = ∆s cv ln 2 + R ln 2 T1 ν1 Tds= dh − νdp T p = ∆s c p ln 2 − R ln 2 T1 p1 ∆s = s o2 − s1o − R ln(p 2 / p1 ) T2 / T1 =( p2 / p1 ) ( k −1)/ k =( ν1 / ν 2 ) ∆s = c ln(T2 / T1 ) k −1 (p 2 / p1 )s = p r 2 / p r1 ( ν 2 / ν1 )s =νr 2 / ν r1 (6) Device Efficiencies and Cycle Analyses w act w isen ηturbine = ηth = Wnet ,out COPR = Qin ηth ,rev = 1- TC TH = ε th η= II ,th (7) ηcompressor = ηpump = w isen w act Qin Wnet ,in COPR,rev = ηth ηth ,rev COPHP = TC TH - TC = ε R η= II , R COPHP,rev = mi m yi = ni nj j mfi ai and a ∑= p2 p1 m ma (10) in Rcond = ∆s = ηvol hˆ A Q hm = c (h∞ − hs ) c p ,m L kA j i =1 i pv pg T EER = Q cap W in Tdp = Tsat ( pv ) Btu W − hr L 1 1 1 = Rtot = + + UA hˆ1 A1 kA hˆ2 A2 Air-Cooled Condenser Analysis (Dry Coil Analysis) Q cond ε c m c ,a c p ,a (Tcond − Tca ,i ) ε c = 1 − e − Ntuc = Tc= Tca ,i + a ,o Q cond m ca c pa UAc = 1 1 1 + ˆh A η hˆ A r r o a a ∑n a =i 1 ∑ [ ∆s ] φ= Heat Transfer Fundamentals ˆ (T − T ) Q = hA conv s ∞ (11) p2 p1 Compressor Analysis η o , is j i i ∆si = si o,2 − si o,1 − R ln m act = ρ sucωVdisp mi ai ∑= ∑ya h= ha + ω hg m (h2, s − h1 ) = W j j M v pv pv pv = 0.622 = 0.622 M a pa pa p − pv hv ≅ hg j Ai ∑= =i 1 =i 1 Psychrometric Relationships ω= = v wturbine TC Q C = TH Q H rev COPHP = ε HP η= II , HP COPHP ,rev Extensive Properties: A = =i 1 =i 1 ∆s = s2o − s1o − R ln wpump TH TH - TC COPR COPR ,rev pi = yi p = Intensive Properties: a (9) BWR = Mixtures of Ideal Gases mfi = (8) Qout Wnet ,in Ntuc = UAc m a c p ,a h= h2 − 3 Rconv = Q cond m r T −T UAc ≅ −m a c p ,a ln 1 − ca ,o ca ,i Tcond − Tca ,i 1 ˆ hA i i Mass and Density UNITS CONVERSION TABLE FOR MAE 3524 1 kg = 2.20 lb m 3 3 1 g cm = 10 kg m 3 Length 1 lb = 0.454 kg m 3 1 g cm = 62.4 lb m 1 cm = 0.394 in ft 3 Volume 1 cm = 0.061 in 3 1 m = 35.3 ft 1 L = 10 −3 m Force 3 1 in = 16.4 cm 3 1 N = 1 kg ⋅ m s 3 1 gal = 0.134 ft 3 3 −3 1= gal 3.79 × 10 m 2 1 lb 2 = 1.45 × 10 1= Pa 1 N m 5 3 = 1 lb 32.2 lb ⋅ ft s f m f 1 bar = 10 N m 1 atm = 1.01 bar −4 lb f 2 Energy 1 J = 1 N ⋅ m = 0.738 ft ⋅ lb f and Specific = 1 kJ 737.56 ft ⋅ lb f Energy 1 kJ = 0.948 Btu Energy Transfer Rate 3 1 ft = 0.0283 m 3 1 N = 0.224 lb Pressure 3 3 1 L = 0.035 ft in 2 1 lb 1 lb f 2 = 4.45 N f f 2 in = 6894.8 Pa 2 in = 144 lb 1 atm = 14.7 lb 1 ft ⋅ lb f in f ft f 1.36 J = = 1 Btu 778.17 ft ⋅ lb f 1 Btu = 1.055 kJ 1 Btu lb = 2.326 kJ kg m 1 kcal = 4.19 kJ 1 W = 1 J s = 3.413 Btu h 1 kW = 1.341 hp 1 Btu h = 0.293 W 1= kJ kg ⋅ K 0.239 Btu lb m ⋅ R = ⋅ K 1 Btu lb ⋅ R 1 kcal kg m Universal Gas Constant 2 2 1 kJ kg = 0.43 Btu lb m Specific Heat 3 1 mile h = 1.61 km h 1 km h = 0.621 mile h 3 ft = 16.018 kg m 1 in = 2.54 cm 1 ft = 0.305 m 1 m = 3.28 ft Velocity 3 1 lb m 1 hp = 2545 Btu h 1 hp 550 ft ⋅ lb = f s 1 hp = 0.746 kW 1 ton =12,000Btu/h=3.517kW 1 Btu = lb R 4.19 kJ kg ⋅ K m 8.314 kJ / kmol ⋅ K o R= 1545 ft ⋅ lb f / lbmol ⋅ R o 1.986 Btu / lbmol ⋅ R Standard Acceleration of Gravity 9.81 m / s 2 g= 2 32.174 ft / s Standard Atmospheric Pressure 1.01bar 1 atm = 2 14.7 lb f / in Temperature Relations T(o R ) = 1.8T(K ) o T (= C ) T ( K ) − 273 T= (o F ) T (o R ) − 460