This application relates to a non-linear PID control algorithm that avoids a potential adverse condition in a vapor compression system.
Refrigerant cycles provide temperature change in a fluid to be treated. In general, a refrigerant cycle includes a compressor for compressing a refrigerant, a first heat exchanger receiving the compressed refrigerant, an expansion device downstream of the first heat exchanger, and a second heat exchanger downstream of the expansion device. Refrigerant flows from the compressor, through the first heat exchanger, through the expansion device, through the second heat exchanger, and back to the compressor. A fluid is heated or cooled at one of the heat exchangers. This basic system can have many uses such as providing hot water, providing air conditioning or providing a heat pump function, among others.
One type of refrigerant cycle is a transcritical cycle. In a transcritical cycle, operation is above the saturation pressure. Thus, there is a degree of freedom with regard to the achieved pressure.
One particular application recently developed by the assignee of this application is for a hot water heating system, wherein the first heat exchanger receives water to be heated. A water pump delivers the water through the first heat exchanger.
As disclosed in co-pending U.S. patent application Ser. No. 10/793,489, filed on even date herewith and entitled “Pressure Regulation in a Transcritical HVAC System,” a control may predict a desired discharge pressure to most efficiently achieve a hot water temperature. A control to achieve the efficient operation monitors a variable with regard to the hot water, and a variable with regard to the refrigerant discharge pressure. These variables are controlled in a manner disclosed in the U.S. patent application Ser. No. 10/793,542, filed on even date herewith and entitled “Multi-Variable Control of Refrigerant Systems.”
The control determines error correction factors for both water temperature and refrigerant discharge pressure, by looking at an error between a desired and actual water temperature and discharge pressure, and both the derivative and integral of these errors.
The basic system 20 is illustrated in
In a refrigerant system 35 operating in transcritical mode, there are two different steady state operational cycles available for a given set of ambient conditions. As one moves further to the right in the graph shown in
The present invention is directed to predicting and addressing when the control of the system would be moving to an inefficient mode. As will be shown below, an error correction algorithm for determining an error correction value looks at both the determined error and a derivative of that determined error. The control is modified under the teachings of this invention to utilize an alternative error calculation if both the error and its derivative are negative. In the disclosed embodiment, the control utilizes the error multiplied by the derivative of the error in the quadrant where the error and derivative of the error are negative. In all other quadrants, the error is not modified. This is illustrated in
These and other features of the present invention can be best understood from the following specification and drawings, the following of which is a brief description.
The system shown in
UEXV is an error correction factor for the expansion device, and UVSP is an error correction factor for the water pump. ep is the pressure error, i.e., the difference between actual and desired compressor discharge pressure. eT is the temperature error, i.e., the difference between actual and desired delivery water temperature. Kp11, Kp12, . . . etc., are numerical constants. The constants K are selected based upon the system, and also based upon the expected change that a particular change in water pump speed, for example, would have on the pressure. There are many methods for choosing the constants. The preferred method is the H∞ (“H infinity”) design method, as explained for example in the textbook “Multivariable Feedback Design” by J. M. Maciejowski (Addison-Wesley, 1989). Note that according to these equations, uEXV and uVSP depend both on the current pressure and the current temperature.
In the present invention, there is preferably an adjustment to provide for correction and avoiding a particular condition wherein both the error for water temperature, and the derivative of the error are negative. This algorithm essentially utilizes an error that is the multiple of the detected error multiplied by the derivative of the detected error when both are negative. In this way, an otherwise potentially inefficient condition can be avoided.
The disclosed embodiment adjusts for water temperature error by changing the volume of water flow from pump 30 through heat exchanger 28. As this flow decreases, the temperature at 26 should increase. As can be appreciated from
The present invention addresses this concern by utilizing a modified error factor for the evsp number if both evsp and the derivative of evsp are negative. Thus, the following equation is incorporated into the control strategy:
The alternative error provides the modified result as shown in
While this invention is illustrated in a particular application of a vapor compression cycle, the invention provides benefits for other vapor compression cycles operating transcritically.
Although a preferred embodiment of this invention has been disclosed, a worker of ordinary skill in this art would recognize that certain modifications would come within the scope of this invention. For that reason, the following claims should be studied to determine the true scope and content of this invention.
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| Number | Date | Country | |
|---|---|---|---|
| 20050193746 A1 | Sep 2005 | US |