The rating condition for high-pressure refrigerants (such as R-404A, -507 or -22) is a 40 degree evaporator temperature, 100-pounds delta P across the valve port, and 100 degrees liquid temperature. If the actual conditions are different than the nominal rating condition, then the actual valve capacity will be different than the nominal capacity.
The delta P across the TEV port is not simply the difference between liquid pressure and evaporator pressure. If there is a refrigerant distributor in the circuit, its delta P must be considered in the equation as well. The typical refrigerant distributor/tube assembly (in a high pressure refrigerant system), when correctly sized, will provide approximately a 35-pound delta P. The TEV delta P is calculated as follows: 226 pounds (liquid pressure) minus 45 pounds (the sum of 35 pounds distributor/tube assembly delta P plus 10 pounds evaporator inlet pressure), equals a 181-pound delta P across the TEV port. As the head pressure lowers, the available delta P across the TEV port is also lowered.
While lowering the head pressure results in a delta P reduction (which will decrease TEV capacity), this is accompanied by a lower liquid temperature (a result of the lower condensing temperature) which will increase the TEV capacity. The effect of lower delta P (reduced valve capacity) and lower liquid temperatures (increased valve capacity) will tend to negate each other without any significant change in TEV capacity.
While the lower head pressure yields reduced motor current and increased compressor efficiency, if lowered too far, eventually the TEV capacity would not be able to meet the demands of the evaporator load.
When this occurs, a portion of the evaporator will cease to transfer heat effectively, as liquid refrigerant would no longer be available to feed it. This will be evidenced by the higher superheat at its outlet. That portion of the evaporator that only sees refrigerant vapor essentially has become an extension of the suction line; it performs no useful work at all.
Reducing the TEV capacity, which leads to a starving evaporator, has, in effect, reduced the evaporator capacity. The end result is increased discharge air temperatures.