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TLC / ORC Process Comparison

Efficiency
An outsider might ask, “Why use the TLC process when established thermodynamic processes for low temperatures, such as the ORC and Kalina processes, are already available?”
A comparison of the TLC process with the widely known and utilized Organic Rankine Cycle (ORC process), based purely on efficiency, yields the following picture.

The ORC process (upper curve family) reaches higher efficiency across all temperature ranges, thus appearing clearly superior to the TLC process (lower curve family).
However, this is a misconception, as the following comparison demonstrates.


ORC Power Plant Structure


TLC Power Plant Structure


External Process View

The reason for this becomes clear from the external process view:
The pressurized liquid working fluid is first heated from the condensation temperature TCond to the evaporation temperature TSteam.
In the second step, the working fluid is evaporated and superheated.
However, only thermal energy with a temperature above the evaporation temperature can be used for evaporation and superheating. For evaporation, several times the amount of thermal energy is required per kilogram of working fluid compared to what is needed for heating the liquid working fluid per kilogram.
A large portion of thermal energy below the evaporation temperature remains unused.
This means that in the ORC process, losses occur in two areas:
1. – Exergetic losses due to “cooling down” the external thermal energy from a higher temperature to the lower evaporation temperature
2. – Incomplete absorption of thermal energy below the evaporation temperature

In contrast, the TLC process only involves heating the liquid, pressurized working fluid without evaporation. Therefore, the working fluid can absorb the entire thermal energy from the condensation temperature TCond up to TMax.
This is shown in both the internal and external process view.


Internal Process View


External Process View

Calculations
The significance of the differences in heat absorption, and thus the losses in the ORC process, can also be mathematically shown.

The following two scenarios were chosen for a direct process comparison:
The heat from 100 m³ of flue gas (e.g., engine exhaust) with a maximum temperature TMax of 300°C or TMax of 200°C is to be converted into mechanical energy in an ORC or TLC process.
Simple alcohol (ethanol) will be used as the working fluid in both processes.
The condensation of the resulting alcohol vapor occurs at a condensation temperature TCond of 50°C.

To compare both processes, the amount of heat absorbed before the conversion of thermal energy into mechanical and subsequently electrical energy is first calculated. For the ORC process, various evaporation temperatures are also considered to illustrate the influence of the evaporation temperature.
To facilitate understanding of the calculations, the formulas used are provided in the first column.
The calculations are based on the assumption of a completely lossless (unrealistic) conversion process.

Calculation with TMax = 300°C


Calculation with TMax = 200°C

Conclusion