PVT and Flow course - Flash Calculations
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Flash Calculations (Part 1 of 2)
A lecture over Flash Calculations and their applications to equations of state. Information from chapter 4 of "Phase Behavior" SPE Monograph (Whitson and Brule)
PDF of notes available here: http://www.ipt.ntnu.no/~curtis/courses/YouTube/Video-Notes/Whitson-PVT-Flow-20120921-Flash-Calc.pdf
We are going to talk about a phase equilibrium calculation. It's usually referred to as the isothermal flash calculation.
The problem statement is that we have a system at fixed (or known or specified) pressure and temperature, and you have the the known composition inside. This might be a some little place inside the reservoir, the production tubing or a production separator, at the surface, it can be really anywhere in the production system.
What we're interested in is finding out:
- how many phases exist (1 or 2).
- how much of each phase. And that will be done in terms of moles or, more typically mole fraction.
- the molar composition of each phase (y_{i} for gas and x_{i} for liquid).
Note: * if it is two phases - they are gas ang liquid (or gas and oil) * if it is one phase, it can either be: ** saturated (in a sense it's two phases but you've got one is one minus epsilon and the other is epsilon, so it's like single phase but there's this like little bubble trying to appear or a little drop trying to appear. So it's a single phase but epsilon you don't see, in a sense the second phase is just it's kind of there) ** undersaturated - where there is just one phase but we can't formally say whether it's gas or liquid. We can only say it behaves like a gas or behaves like liquid.
The solution requires in addition to the pressure, temperature and composition Z_{i}, it requires an estimate of the ratio which we call the equilibrium ratio component K_{i}.
K_{i} = y_{i} / x_{i} - equilibrium ratio
Component material balance says that total moles is equal to the moles of component i in the liquid plus the number of moles of component i in the vapor. we don't let in those component i disappear:
n_{i} = n_{LI} + n_{Vi}
We have a total material balance that we don't lose any moles altogether. So the total moles is equal to total moles in the liquid plus the total moles in the vapor:
n = n_{L} + n_{V}
n = Σn_{i}; n_{L} = Σn_{LI}; n_{V} = Σn_{Vi}
Define:
z_{i} = n_{i}/n y_{i} = n_{Vi}/n_{V} x_{i} = x_{Li}/n_{L} f_{v} = n_{v}/n - mole fraction of vapor is the moles of vapor over the total moles f_{L} = n_{L}/n - mole fraction of the phase liquid f_{L} = 1 - f_{v}
And also:
Σz_{i} = 1 = Σy_{i} = Σx_{i}
Let's rewrite the equations:
z_{i} = f_{v}*y_{i} + (1 - f_{v})*x_{i} z_{i} = f_{v}*(K_{i}*x_{i}) + (1 - f_{v})*x_{i}
Let's solve this for x_{i} and y_{i}:
x_{i} = z_{i} / [f_{v}*(K_{i}-1) + 1] y_{i} = K_{i}*x_{i} = [z_{i}*K_{i}] / [f_{v}*(K_{i}-1) + 1]
In 1949 Muscat and his colleague McDowell published the first paper in the Society of petroleum engineers about using a computer and they had to solve this problem in connection with that and so they did. But later, Rachford and Rice published a 3 or 4 page paper in the Society of petroleum engineers, they gave this whole development we've done and they came up with this final equation, a little bit further than that. And they became famous. But in fact Muscat and McDowell in 1949 paper in a small footnote and the text of the paper gave exactly the equation. And Rachford and Rice did not refer to what was Morris Muskets last publication.
Σ(y_{i} - x_{i}) = 0 Σ {[z_{i}*K_{i} - 1] / [f_{v}*(K_{i}-1) + 1]} = 0 - that is so called Rachford-Rice equation.
The only thing in that equation we don't know is f_{V}. You define this function:
h(f_{V}) = Σ {[z_{i}*K_{i} - 1] / [f_{v}*(K_{i}-1) + 1]} = 0
The only thing you have to do to solve this problem to solve this equation. You have to find which f_{V} drives this summation to 0.
Watch the full video
Flash Calculations (Part 2 of 2)
Let's look at the equation and see what are the characteristics of this of this function"
h(f_{V}) = Σ {[z_{i}*K_{i} - 1] / [f_{v}*(K_{i}-1) + 1]} = 0
- h(f_{V}) is a monotonic function, that should mean that a Newton Rapson type solution should work efficiently, we can take the analytical derivative and use that in a Newton Rapson solution.
- (N-1) solutions for N components. But luckily only one of these yields physical solution. And by physical solution what we mean is that both the calculated x_{i} are positive for all components and the calculated y_{i} for all components are positive.
0 > 1/(1-K_{max}) = f_{Vmin} < f_{V} < f_{Vmax} = 1 / (1-K_{min}) > 1
You just have to search all the K values and you find the minimum and you find the maximum and that will immediately tell you what is f_{Vmin} and f_{Vmax}. And in between those two numbers there's only one solution and only that solution will guarantee this: x_{i}>0 and y_{i}>0. So, even though there are n minus 1 solutions we can immediately identify the bounds of the one we want.
0 ≤ f_{V} ≤ 1 - two phase solution, liquid + vapor f_{V} = 0 - saturated single phase solution, liquid f_{V} = 1 - saturated single phase solution, vapor f_{V} < 0 - undersaturated single phase, liquid-like solution f_{V} > 1 - undersaturated single phase, vapor-like solution
The general setup for solution is that you know basically pressure, temperature and composition:
- Estimate K_{i}(P,T,p_{k})
- Setup a table:
Guess: f_{V}
Calc: f_{Vmin}
and f_{Vmax}
i | z_{i} | K_{i} | c_{i} | Term_{i} | y_{i} | x_{i} |
1 | ||||||
2 | ||||||
3 | ||||||
... | ||||||
N | ||||||
h |
Changing f_{V}
try to achieve h = 0.
There are special cases of the flash calculation. To learn more, watch the full video.
Watch the full video
Flash Calculation Example (Part 1 of 3)
An example using Flash Calculations. Information from chapter 4 of "Phase Behavior" SPE Monograph (Whitson and Brule)ю
PDF of notes available here: http://www.ipt.ntnu.no/~curtis/courses/YouTube/Video-Notes/Whitson-PVT-Flow-20120925-Flash-Example.pdf
Flash Calculation Example (Part 2 of 3)
Flash Calculation Example (Part 3 of 3)
Other lectures from the PVT and Flow course
- Blog:PVT and Flow course - Gas or Oil Reservoir?
- Blog:PVT and Flow course - Single Component Vapor Pressure.
- Blog:PVT and Flow course - Two-Component Phase Behavior
- Blog:PVT and Flow course - Multi-Component Phase Diagrams
- Blog:PVT and Flow course - K Values
- Blog:PVT and Flow course - Flash Calculations
- Blog:PVT and Flow_course - Surface Separation Processing
- Blog:PVT and Flow course - Sampling
- Blog:PVT and Flow course - PVT Lab Tests
- Blog:PVT and Flow course - OBM Decontamination
- Blog:PVT and Flow course - Lab PVT Tests CCE
- Blog:PVT and Flow course - LAB PVT Tests Multistage SEP
- Blog:PVT and Flow course - Lab PVT Tests DLE
- Blog:PVT and Flow course - Lab PVT Tests CVD
Class notes developed during lectures are available as PDF files, named with the format yyyymmdd.pdf located on: http://www.ipt.ntnu.no/~curtis/courses/PVT-Flow/2016-TPG4145/ClassNotes/
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