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西安石油大学:《油藏物理(油层物理学)Petro-physics》精品课程教学资源(英文课件)Fluid 2.2 Phase state equation of hydrocarbons 油气系统的溶解与分离

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Phase state equation of hydrocarbons Xuanqi zhang Petroleum engineering college

Phase state equation of hydrocarbons Xuanqi zhang Petroleum engineering college

油藏物理学一油气系统的溶解与分离 2.平衡常数equilibrium constant K=y:/X:与P、T及组成有关。 y一在压力P下,组分在气相中的浓度;(摩 尔分数) x:一在压力P下,组分在液相中的浓度; K一平衡常数,在压力P下,组分在气相中的 分配比例。 特点:在T一定时,随P的增加,平衡常数K逐 渐收敛于等于1的一点。该点即为收敛压力。 收敛压力:Convergence pressure

2. 平衡常数equilibrium constant Ki=yi/xi 与P、T及组成有关。 yi—在压力P下,i组分在气相中的浓度;(摩 尔分数) xi —在压力P下,i组分在液相中的浓度; Ki—平衡常数,在压力P下,i组分在气相中的 分配比例。 特点:在T一定时,随P的增加,平衡常数Ki逐 渐收敛于等于1的一点。该点即为收敛压力。 收敛压力: Convergence pressure 油藏物理学——油气系统的溶解与分离

「油藏物理学一油气系统的溶解与分离 set phase state equation 866666 a. P,T 1 moL Ng Yi 动平衡 NL Xi when P and T attain balance for 1mol of oil,balance equation of i component is Ng+N=1 (1) Nix+Ngyi=ni (2) Ki=yi/x (3)

set phase state equation 油藏物理学——油气系统的溶解与分离 a. when P and T attain balance for 1mol of oil, balance equation of i component is i i i L i g i i g L K y x N x N y n N N / 1      (1) (2) (3)

油藏物理学一油气系统的磙解与分离 Phase state equation for i component ni n Ni+K:Ng K;-(K,-I)N or Kin; Kini N1+K Ng 1+(K;-1)Ng

Phase state equation for i component 油藏物理学——油气系统的溶解与分离 L i g i i i L i g i i N K N K n y N K N n x     i g i i i i i L i i K N K n y K K N n x 1 ( 1) ( 1)       or

油藏物理李一油气系统的磙解与分离 total phase state equation ∑x,=1 So ∑K-(K-N n =1 ∑y,=1 Kini =1 1+(K,-)Ng

total phase state equation 油藏物理学——油气系统的溶解与分离     1 1 i i y x 1 1 ( 1) 1 ( 1)         i g i i i i L i K N K n K K N n So

油藏物理李一油气系统的溶解与分离 application of equation 1.If we know ni,P and T,find Ne NLXi Y in the condition If there are m kinds of components for oil,we can got m equations n; x=K-(K:-1)N

application of equation 油藏物理学——油气系统的溶解与分离 1. If we know ni , P and T,find Ng、NL、Xi、 Yi in the condition. If there are m kinds of components for oil, we can got m equations i i L i i K K N n x  ( 1) 

油藏物理李一油气系统的磙解与分离 Because there are (m+1)unknown,we don't solve the equation.We use trial method We can choose NL n K,-(K,-1)N f ∑x=1 NL is true. ∑x,≠1 return

if 油藏物理学——油气系统的溶解与分离 xi 1 NL is true. xi  1 return Because there are (m+1) unknown, we don’t solve the equation. We use trial method. We can choose NL i i L i L i K K N n N x ( 1) Substitute     

油藏物理学一油气系统的溶解与分离 2 find Pp和Pd a,Pp: based on saturated vapour pressure curve,N-0, NL=1,X-ni 工工晨 nKi =∑K,n,=1 By trial method,we can choose ,T,aem→Ke→∑Kn ∑Kn,=1 Pb is true. ∑Kn,≠1 return

2 find Pb和Pd 油藏物理学——油气系统的溶解与分离 a, Pb : based on saturated vapour pressure curve, Ng=0, NL=1,xi=ni 1 1 ( 1)        i i i g i i i K n K N n K y By trial method, we can choose     i i checkdiagram substitute Pb ,Tf Ki K n K 1 1 i     i i i n K n Pb is true. return

油藏物理学一油气系统的溶解与分离 b.Pa based on dew point curve,NL-0,Ng=1,yini 2x-2张1 trial method like as above

b. Pd 油藏物理学——油气系统的溶解与分离    1 i i i K n x trial method like as above. based on dew point curve, NL=0,Ng=1,yi=ni

3.calculate phase state diagram If we can got corresponding P for T,we can got phase state diagram

If we can got corresponding P for T, we can got phase state diagram. 3. calculate phase state diagram

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