Appendix F: Modeling VRF systems

While work has begun on this, the VE does not yet include an explicit model for Variable Refrigerant Flow (VRF) systems, also referred to as Variable Refrigerant Volume (VRV). The condenser heat recovery facility in ApacheHVAC, however, can be used to reasonably approximate the thermodynamic performance of such systems. This assumes that the system is configured and controlled the move heat, via a common refrigerant loop, from zones in cooling mode to those in heating mode when these modes overlap.
1. Start with a multiplexed prototype system that best represents the configuration for the actual project—e.g., PTAC, packaged single-zone, or DOAS with Fan-coil units.
2. Use a part-load-curve chiller component for the cooling mode.
The part-load-curve chiller component is used to represent the cooling mode for six reasons:
3. Use a Generic heat source component for the heating mode.
Depending upon whether heating mode performance varies more significantly with load fraction or outdoor temperature, the part-load-curve Heating equipment inputs or Air-source heat pump (both accessed from within the Generic heat source dialog) can be used to model the heating mode (addressing heating loads when rejected heat from cooling-mode operation is not available).
In a warm climate where the variation of outdoor source temperature does not significantly influence capacity and COP, the ability to model COP variation with part-load fraction may be most valuable. Efficiency values (which can be in excess of 100%—e.g., 350% to represent a COP of 3.5) in the Part load curve heating plant dialog are used to indicate up to 10 part-load COP values. If there is backup electric resistance heating, this can be represented by a 100% efficiency value in the last (bottom) row, with the 9th data point representing the heat pump function a maximum output. There should be very small increment for the load range between the 9th and 10th data points so that the model makes a very steep transition rather than smooth ramp of the COP value between these point.
When outdoor temperature is the primary driver for heating mode performance (after using recovered heat when there is simultaneous heating and cooling), the Air-source heat pump (ASHP) may be the preferable option when outdoor temperature is the primary driver for heating mode performance (after using recovered heat when there is simultaneous heating and cooling). The reasons for this are that the ASHP model varies according to outdoor temperature (and thus thermal lift) and also has a setting for the Minimum source temperature below which the unit will cease to operate and will depend fully upon the backup heat source.
The ASHP model can still account in some respect for variation of COP with load fraction; however, this must be entered as data points on a single composite curve that indicates both the COP and heat output available for each outdoor temperature. The curve is once again represented by up to 10 data points. For each point, users need to indicate the outside-air source temperature, COP, and heat output available at that temperature. While there are benefits in accounting for variation of performance with outdoor temperature, some analysis may be required to determine appropriate part-load adjustments to the otherwise full-load COP with relatively higher outdoor source temperatures. In other words, the user must first determine how much, assuming otherwise typical operation of the building, the heating load will be reduced from the full-load condition as outdoor temperatures rise. This can then be used to adjust COP according to load fraction for data points associated warmer outdoor temperatures.
When using the ASHP, the Part load curve heating plant (see Heating equipment Edit button) within the Generic heat source dialog can be used to represent just the backup heat source. Typically this will be electric resistance heat (efficiency = 100%).
4. Distribution losses associated with refrigerant lines can be accounted for in the Heat source dialog. Airside distribution losses are better accounted for by using the Ductwork heat pickup (heat gain/loss) component on the HVAC network.
5. In the cooling source (part-load curve chiller model), you can specify COP values dependent upon both load and OA dry-bulb conditions. Set the pump and tower fan power to zero.
6. The Condenser Heat Recovery percentage in the part-load curve chiller dialog should be 100% (indicating that all of the heat extracted from zones in cooling can be rejected to zones in heating) and the CHR recipient should point to the Generic heat source you have set up for the heating mode.
7. In the Part-load curve heating plant dialog for the Generic heat source (when using this rather than the ASHP to model heating mode) COP values will be expressed as efficiency values—e.g., 350% to indicate a COP of 3.5).
8. In the Generic heat source dialog, leave the tick box for “Use water source heat pump?” unticked, as you will already have determined the electrical energy needed to extract this recovered heat on the cooling side. Set the Heating plant type to “Other heating plant” to keep energy consumption results separate from boilers or DHW heat sources, if any, in the project. The heat load will be apportioned in the following sequence:
 
This method can account for the benefits of moving heat from one zone to another and variation of COP with both load and outdoor temperature (it will account for the degradation of COP and heating capacity with low outdoor temperatures only if the ASHP is used for the heating mode).
The graph below shows results for a modest 25-zone office building on a day where heating and cooling loads overlap. There is one air-source heat pump (ASHP) acting as the heating mode of the VRV system and one part-load-curve “chiller” as the cooling mode of the VRV. These components within ApacheHVAC are permitted to serve multiple heating and cooling coils, as would be the case in a VRV system.
In the illustrated example, the ASHP and part-load cooling sources are coupled to heating and cooling coils in a multiplexed stack of 25 packaged single-zone systems for the individual zones. These are created from either the prototype Packaged single-zone system 04 or prototype Packaged terminal heat pump system 02, as provided in pre-defined configuration. With just two exceptions, the pre-defined configurations remain unchanged:
The condenser heat recovery (CHR) acts as the common refrigerant loop to pass heat from the zones in cooling mode to those requiring heat. The CHR points to a Generic heat source representing the VRV heating mode (via options described above) and electric-resistance backup heat.

The ER backup is third in line to meet heating loads after the CHR and VRV heating mode (part-load-curve or ASHP) capacity are fully used. Because the backup heat source will always have an infinitely expandable capacity, any limitation of heating capacity needs to be specified in terms of the capacity of the each heating coils. Maximum cooling capacity is similarly limited by the capacity specified for each “simple” cooling coil (advanced coils, water loops, and detailed chiller models must be used to model the cooling performance of under-served coils in the case of intentionally constrained plant equipment capacity).

The graphs below for two different VRV examples show the recovered heat from the cooling mode (green line) taking precedence over the ASHP (VRV heating mode) to meet heating load. When energy values for the “chillers” and “heat pumps” variables are added in the second graph, these result also show that the cooling system is accounting for the energy required to extract this heat via an evaporator coil in zones where cooling is taking place and then pumping it to the heating side. Thus the electrical energy consumption for this extraction of heat from zones in cooling mode does not need to be counted separately on the heating side.

In working out the these methods, our observation is that for many building types and configurations, if the systems are suitably controlled, there should be very little temporal overlap of heating and cooling modes in a building effectively served by a large number of single-zone systems sharing a common outdoor component. It would therefore appear that, in many applications, much of the efficiency (or perhaps better referred to as efficacy) of VRV/VRF systems stems from their avoidance of the “one-size-fits-all” plus re-heat outcome typical of a multi-zone packaged VAV system.  In other words, the common-loop aspect of the configuration often seems to be secondary, in terms of providing reduced energy consumption, to other aspects of VRV, such as obviating the need for re-heat.
The table of results below shows another means of confirming the transfer of recovered heat from zones in cooling mode to zones in heating mode: When there is a cooling load present and the cooling load (total for all zones presently in cooling mode) times the cooling COP—i.e., the amount of heat that needs to be rejected by the VRV system in cooling mode—is equal to or greater than the heating coils load (total for all zones presently in heating mode), then the part-load heat source or heat pump load should go to zero, as should the backup heat source if using the ASHP with backup electric heat.
 
The two graphs on the next page show additional examples of results variables that can be examined to analyze the performance of VRV performance for particular project. Results such as these can be used as a quick reality check to see that the system is behaving as expects. They can also be used to provide more detailed analysis of what sort of performance might be expected under various conditions.