- Residential Market
- Light Commercial Market
- Commercial Market
- Indoor Air Quality
- Components & Accessories
- Residential Controls
- Commercial Controls
- Testing, Monitoring, Tools
- Services, Apps & Software
- Standards & Legislation
- EXTRA EDITION
However, to be a good troubleshooter, a technician must use the proper instrumentation and, more importantly, have certain organizational skills. Organizational skills will help the technician more quickly solve even the toughest problems he may encounter in the field. One of the best-known ways for a service technician to organize thoughts is through the use of a service checklist, a sample of which is shown in Table 1.
By simply measuring and recording those temperatures required in Table 1 using thermistors or thermocouples, getting the low- and high-side pressure readings using a gauge manifold set, and reading the compressor's voltage and amperage, a technician will be able to troubleshoot any refrigeration system, thoroughly and quickly. These six temperatures and two pressures give the technician evaporator superheat, compressor superheat, condenser subcooling, and the condenser split for the system.
Take a look at the system checklist in Table 2. With those figures in hand, a technician could analyze the system for faster systematic troubleshooting.
Medium to high compressor discharge temperature: This temperature is very high compared to normal system operations. The 220°F discharge temperature is caused by the evaporator and compressor running high superheat along with high compression ratios.
When undercharged, do not expect the TXV to control superheat. The TXV may be seeing vapor and liquid at its entrance. The evaporator will be starved of refrigerant and running at high superheat. The compressor now sees high superheat coming to it, and with the compression stroke will superheat the vapors even more.
Compression ratios also will be elevated, giving the system a higher-than-normal heat of compression. Compression ratios will be high due to low evaporator pressures. This will give the system very low volumetric efficiencies and cause unwanted inefficiencies with low refrigerant flow rates.
The compressor will now have to compress much lower pressure vapors coming from the suction line to the condensing pressure. This requires a greater compression range and a higher compression ratio.
This greater compression range from the lower evaporator pressure to the condensing pressure is what causes more compression work and generates more heat of compression. This increased heat may be seen by the high compressor discharge temperature.
In conclusion, higher compression ratios and higher superheats are what cause the discharge temperature to be high. Remember, the discharge line sees all of the superheat coming to the compressor, the electric motor heat generated, and the heat of compression.
The absolute limit that any discharge temperature should be measured about three inches from the compressor on the discharge line is 225°. The back of the discharge valve is usually about 50° to 75° hotter than this point on the discharge line. This would make the back of the discharge valve about 275° to 300°. This temperature could vaporize oil around the cylinders and cause excessive wear. At 350°, oil will break down. Overheating of the compressor will soon occur.
Compressor overheating is one of today's most serious field problems. Try to keep your discharge temperatures below 225° for longer compressor life.
High evaporator superheats: Because the TXV and evaporator are starved of refrigerant from the undercharge, evaporator superheats will be high. This, in turn, will lead to high compressor (total) superheats. The receiver is not getting enough liquid refrigerant from the condenser because of the shortage of refrigerant in the system. This will starve the liquid line and may even bubble a sight glass if the condition is severe enough. The TXV is not seeing normal pressures and may even be trying to pass a liquid and vapor mixture from the starved liquid line. The TXV cannot be expected to control evaporator superheat under these conditions.
Low condenser subcooling: In TXV systems, the compressor is seeing much warmer vapors from the high superheat readings. The gases entering the compressor will be very expanded and have a low density. The compression ratio will be high from the low suction pressure, causing low volumetric efficiencies. The compressor is simply not pumping much refrigerant.
All components in the system will be starved of refrigerant. The 100 percent saturated liquid point in the condenser will be very low. This will cause low condenser subcooling. The condenser is simply not receiving enough refrigerant vapor to condense it to a liquid and feed the receiver. Condenser subcooling is a good indicator of how much refrigerant charge is in the system. Low condenser subcooling can mean a low charge. High condenser subcooling can mean an overcharge, but not always.
This is not true for capillary tube systems; the majority of them have no receiver. A cap tube system can run high subcooling simply from a restriction in the capillary tube or liquid line. The excess refrigerant will accumulate in the condenser, causing high subcooling and high head pressures.
If a TXV receiver system is restricted in the liquid line, most of the refrigerant will accumulate in the receiver (with a bit in the condenser), causing low to normal subcooling and low head pressure.
Low compressor amps: High superheats cause compressor inlet vapors to be very expanded from the suction line. This will decrease their density. Low-density vapors entering the compressor mean low refrigerant flow through the compressor. This causes a low amp draw because the compressor doesn't have to work as hard compressing the low-density vapors. Low refrigerant flow will also cause refrigerant-cooled compressors to overheat.
Low evaporator pressure: Low evaporator pressure is caused by the compressor being starved of refrigerant. The compressor is trying to draw refrigerant into its cylinders, but there isn't enough refrigerant to satisfy it. The entire low side of the system will experience low pressure.
Low condensing pressure: Because the evaporator and compressor are being starved of refrigerant, the condenser will also be starved. Starving the condenser will reduce the heat load on the condenser because it isn't seeing as much refrigerant to reject any heat. With not as much heat to accept and thus reject from the compressor, the condenser will be at a lower temperature. This lower temperature will cause a lower pressure in the condenser because of the pressure-temperature relationship at saturation.
The equation for this is:
Condensing Temperature - Ambient Temperature = Condenser Split
As the condenser sees less and less heat from the evaporator and compressor because they are both being starved of refrigerant from the undercharge, the condenser split will decrease. No matter what the ambient temperature is, the condenser split - the difference between the condensing temperature and the ambient - will remain the same if the load remains the same on the evaporator.
Condenser split will change if the load on the evaporator changes. Some common condenser splits for refrigeration applications are listed in Table 3. Box temperatures will tell the technician what evaporator load the system is under. A low box temperature means a low load; high box temperature means a high load.
CONCLUSIONAs you can see, systematic troubleshooting requires a thorough knowledge of the refrigeration system and its components. How and why temperatures and pressures respond the way they do when something goes wrong with the system can be understood with a thorough analysis of a system checklist. System checklists let the service technician organize his thoughts and help him find tough problems faster.
John Tomczyk is a professor of HVACR at Ferris State University, Big Rapids, Mich. He can be reached by e-mail at firstname.lastname@example.org.
Publication date: 01/09/2006