REAL-TIME MEASUREMENT OF TWO-PHASE MASS FLOW RATE AND ENTHALPY USING PRESSURE DIFFERENTIAL DEVICES

Abstract

The methods and instrumentations for measuring in real-time the two-phase mass flow rate and the enthalpy from the geothermal wells and large diameter pipelines can be used in memory and on-line to measure the mass flow rate and enthalpy when the two-phase pipeline is in operation or during testing. This measuring instrument consists of primary, secondary and multi-tapping components. The primary component can be a concentric orifice plate, a top eccentric orifice plate, a bottom eccentric orifice plate, a segmental orifice plate, Nozzle or Venturi tube. The secondary component is a transmitters-transducers. The multi tapping used are radius (ID and ID/2), flanges, corners and other arrangement or different combinations. On this device system, the data signal of upstream pressure, downstream and the pressure difference of the multi tapping is recorded and transmitted or recorded by the transmitters-transducers to the computer machine.

Claims

1. A method of calculation of mass flow rate and enthalpy for two-phase fluid, consisting of: measurements of transmitter signal of upstream pressure, downstream pressure and pressure differences during the operation of the two-phase fluid flow in the pipeline; reception of signals from transmitters within the transducer which is in the form of electrical or pneumatic signals; the signal is recorded and converted into pressure units; computation of enthalpy, in real-time, using the pressure data input of the transducer whose varies in time units; and computation of mass flow rate, in real-time, using enthalpy real-time input and the pressure data of the transducer simultaneously and continuously.

2. The method of claim 1, where the two-phase fluid is a mixture of steam and water or other liquid and gas.

3. The method of claim 1, where real-time measurement of mass flow rate and enthalpy can be carried out on-line in production without having to stop the operation.

4. The method of claim 1, where real-time measurement of mass flow rate and enthalpy can be used on geothermal wells or other pipelines in operation and supplying steam to the plant and or on the geothermal wells or pipelines that are in production or during testing.

5. The method of claim 1, where the frequency of data acquisition can be adjusted according to the requirements.

6. The method of claim 1, where the attenuation of signal strength sent by the transmitter to the transducer, will follow the pressure changes that occur in the pipeline.

7. The method of claim 3, a measured real-time signal of the upstream and downstream sides of two or three tapping, of these tapings are obtained two or three values of upstream pressure and two or three values of downstream pressure.

8. The method of claim 4, the pressure difference value of the all pressure tapings is calculated by a subtracting the upstream pressure from the downstream pressure.

9. The method of claim 1, two values of upstream pressure, two values of pressure difference, and the diameter ratio () is used to obtain the steam mass fraction or the dryness fraction.

10. The method of claim 1, the value of pipe inside diameter is used to determine the enthalpy correction factor.

11. The method of claim 1, the upstream pressure value, steam mass fraction and enthalpy correction factor are used to calculate the real-time enthalpy.

12. The method of claim 7, to acquire real-time enthalpy with minimum noise, the calculation results of real-time enthalpy is optimized using the Kalman filter technique in which this technique requires one initial input value (estimation) of enthalpy into the iteration algorithm.

13. The method of claim 1, the pipe inside diameter is used to determine the mass flow rate correction factor.

14. The method of claim 1, one upstream pressure value, one pressure difference value and flow rate correction factor are used to calculate the real-time mass flow rate.

15. The method of claim 11, to acquire real-time mass flow rate with minimum noise, the calculation result of real-time mass flow rate is optimized using the Kalman filter technique where this technique requires one initial (estimated) input value for the iterations algorithm.

16. The method of claim 1, the calculation and iteration of the mass flow rate and enthalpy is carried out using the computation system where the process of algorithm model is designed specifically so that the measurements are obtained in real-time and simultaneous in the given measurement range continuously.

17.39. (canceled)

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0012] To facilitate presentation of the inventions, the images related to this invention follow:

[0013] FIG. 1 is a simple schematic diagram of the two-phase fluid utilization from a geothermal well.

[0014] FIG. 2 is a flowchart of the method of measuring mass flow rate and enthalpy of two-phase fluid of a geothermal well or a pipeline in real-time.

[0015] FIG. 3 is a top view schematic diagram of the measuring instrument of mass flow rate and enthalpy of geothermal well or a pipeline wo-phase fluid flow with the multi-taping orifice plate type.

[0016] FIG. 4 is the orifice plate type: (a) concentric, (b) bottom eccentric, (c) top eccentric, and (d) segmental designs.

[0017] FIG. 5 is a top view schematic diagram of the measuring instrument of mass flow rate and enthalpy of geothermal well or a pipeline two-phase fluid flow with the multi-taping Nozzle type.

[0018] FIG. 6 is a top view schematic diagram of the mass flow rate and enthalpy of two-phase fluid flow of geothermal well or a pipeline with the Venturi tube multi-taping type.

[0019] FIG. 7 is a comparison of the measurement results using the measuring instrument of mass flow rate gauge and enthalpy with real-time field data.

DETAILED DESCRIPTION

[0020] The measuring instruments (6, 7) of mass flow rate which is often used in the industry employ a method which measures the difference between upstream (3) and downstream pressures (4). The principle of this measuring instrument (6, 7) refers to the energy conversion theory in the fluid flowing inside the closed pipeline (5). The measuring instruments (6, 7) of pressure difference device consist of two components, primary and secondary. The primary component is installed in the pipeline (5) for restricting flow and will cause the pressure difference between upstream (3) and downstream (4). The value of pressure difference from the measuring instrument (6, 7) is used to calculate the fluid mass flow rate (14) by applying the Bernoulli law. The secondary component is connected to the measuring instrumentation to provide information on the calculation variable of mass flow rates, such as pressure and temperature. Both the primary and secondary components can be installed as one unit or separated from the measuring instrument system (6).

[0021] Real-time measurement techniques of geothermal two-phase fluids are developed based on the design of pressure differential devices (6, 7). In this invention, the measuring instrument of pressure difference includes orifice plates (FIGS. 3-4), Nozzle (FIG. 5) and Venturi tube (FIG. 6). The installation of pressure difference measuring instruments (6, 7) on the pipeline (1, 5) can be seen in FIG. 1. The recommended installation for the measuring instruments (1) is that it is installed on a straight, unhindered pipe (5) with a minimum distance of 20 times the pipe inside diameter (26) on the upstream side (3) and 7 times the pipe inside diameter (26) on the downstream side (4). The longer the straight pipe distance (5) the smaller the error in the measurement results because the flow disturbance effects caused by pipefittings, such as valve, reducer and elbow can be minimized.

[0022] The multi pressure tapings (16-21, 32-37, 42-47) are installed into a single unit with the measuring instrument (6, 7). When the geothermal two-phase fluid flows towards the primary component (25, 41, 52) inside the pipe (5), then the pressure at that point is referred to as the upstream pressure (16-18, 32-34, 42-44). The two-phase fluid velocity will increase due to the narrowing area at the primary component (25, 41, 52) so that it causes the pressure decrease in the downstream side (19-21, 35-37, 45-47). This occurs due to increased friction between the fluid and the walls of the primary components (25, 41, 52) and also because of the flashing effect, namely the change of the liquid phase to steam in the two-phase fluid due to pressure drop. The difference between the upstream (16-18, 32-34, 42-44) and downstream pressures (19-21, 35-37, 45-47) is called as a pressure difference, which is measured by the pressure transducer or gauge. The pressure difference will increase and decrease following the change in the mass flow rate (14) and enthalpy (12) in the pipeline (5). In this invention, there are three upstream pressure values (16-18, 32-34, 42-44), three downstream pressure values (19-21, 35-37, 45-47), and three pressure difference values (22-24, 38-40, 48-50) that are recorded simultaneously. The system is called as multi-tapping. All measured values of the multi-tapping (upstream pressure, downstream pressure, and pressure difference) are correlated with enthalpy (12) and mass flow rate (14). Signals of multi-tapping pressure difference (22-24, 38-40, 48-50) are measured by the transmitters from the primary components (25, 41, 52). Then the signal from the transmitters is converted into electrical signals which are processed and calculated in a computer to get the enthalpy. The noise of the resulting enthalpy is reduced by adding an input of enthalpy estimate value (11) and is reduced using the Kalman filter technique. From the results, the real-time enthalpy (12) is obtained and optimized. The real-time enthalpy (12) and the real-time data of multi-tapping pressure differences (22-24, 38-40, 48-50) are used to calculate the mass flow rate. Noise in the measured mass flow rate is also reduced by using the Kalman filter technique. The algorithm of real-time measurement process of enthalpy (12) and mass flow rate (14) are presented in the flowchart shown in FIG. 2.

[0023] Measuring instruments (6, 7) of the pressure difference with multi-tapping in this invention is applied to three types of measuring devices (6, 7) of pressure difference, namely orifice (FIG. 3), Nozzle (FIG. 5) and Venturi tube (FIG. 6). The multi-tapping design of orifice and Nozzle has similarities as seen in FIGS. 3 and 5. The first tapping position (17, 20, 33, 36) is placed vertically on the top of the pipe (5), while the second (16, 19, 32, 35) and the third tapping (18, 21, 34, 37) are placed horizontally on the flange (15). Other possible pressure tapping design and locations can also be applied to give similar outcome.

[0024] There are four types of orifice plates that can be used in the measuring instruments in this invention, namely concentric (FIG. 4a), bottom eccentric (FIG. 4b), top eccentric (FIG. 4c), and segmental (FIG. 4d). The location of orifice holes (28) is placed in the middle of the pipe inside diameter (26) on the concentric type, while the position of orifice holes can be shifted to the lower position (29) or upper position (30) of the pipe inside diameter (26) for the eccentric type. In a segmental type orifice plate, the orifice holes (31) are placed at the lower position of the pipe inside diameter (26) with a segmented hole shape (31). Other possible orifice plate design (type) can also be used to give similar outcome. For the measuring instruments (6, 7) which use Nozzle type, the configuration and location of the tapping follow that of the orifice type. The Nozzle installation direction (41) must be installed correctly and must be associated with the direction of the two-phase fluid flow (2) (FIG. 5).

[0025] The location of tapping on the Venturi tube type differs from the orifice and Nozzle, where the first (43, 46), the second (42, 45) and the third (44, 47) tapping are installed in accordance with FIG. 6. The position of the tapping holes on the flange (42, 44, 45, 47) is separated by the Venturi tube, the length of which is adjusted to the body of Venturi tube (52). The diameter of Venturi tube (51) is smaller than the pipe inside diameter (26) to produce a disturbance effect and resistance to the two-phase fluid flow.

[0026] The three alternative types of measuring instruments (6, 7) of real-time mass flow rate (14) and enthalpy (12) of two-phase fluids are designed and adapted to the application (FIGS. 3, 5, and 6). At the process design stage, attention should be paid to the physical parameters, including the desired range of pressure difference, the desired range of enthalpy and mass flow rate, the anticipated accuracy and the prediction of total pressure drop of the measuring instrument.

[0027] In this invention, methods and measuring instruments (6, 7) of real-time enthalpy and mass flow rate of a two-phase fluid have been verified and validated on a series of field tests on several two-phase pipelines. These methods and measuring instruments (6, 7) have been tested for a varying range of pipe sizes (26), enthalpy (57), and mass flow rates (58). Comparison of the resulting measurement of the enthalpy and the mass flow rate of two-phase fluid from the measuring instrument (60, 62) in this invention with the field data (59, 61) is presented in FIG. 7. From FIG. 7 it appears that the relative error to the field flow test data of the four geothermal wells (53-56) is less than one percent. The field test results show that the methods and measuring instruments (6, 7) of this invention can be implemented and applied to the measurement of mass flow rate (14) and enthalpy (12) of two-phase fluid in real-time.