Theory
Rankine thermal efficiency:$\eta_{th}= \dfrac{w_{net}}{q_{in}}= \dfrac{(h_3-h_4)-(h_2-h_1)}{h_3-h_2}$
Turbine isentropic efficiency:
$\eta_t = \dfrac{h_3-h_4}{h_3-h_{4s}}$
| State | T (°C) | P (MPa) | h (kJ/kg) | s (kJ/kg·K) | Description |
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Visualize steam power (Rankine) and refrigeration cycles on T-s and P-h diagrams in real time. Automatically calculate thermal efficiency, COP, and state properties.
| State | T (°C) | P (MPa) | h (kJ/kg) | s (kJ/kg·K) | Description |
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The core performance metric for the Rankine power cycle is its thermal efficiency. It's the ratio of the net work output (turbine work minus pump work) to the heat input from the boiler.
$$\eta_{th}= \frac{w_{net}}{q_{in}}= \frac{(h_3-h_4)-(h_2-h_1)}{h_3-h_2}$$Here, $h$ is specific enthalpy (kJ/kg). Points 1, 2, 3, and 4 correspond to the states at the pump inlet, boiler inlet, turbine inlet, and condenser inlet, respectively, on the cycle diagram. The simulator calculates these enthalpies using the pressures and efficiencies you set.
For the refrigeration cycle, the equivalent metric is the Coefficient of Performance (COP). For cooling, it's the ratio of the desired heat removal from the cold space to the work input required by the compressor.
$$COP_{R}= \frac{q_{in}}{w_{in}}= \frac{h_1 - h_4}{h_2 - h_1}$$Here, $q_{in}$ is the refrigeration effect (heat absorbed in the evaporator), and $w_{in}$ is the compressor work. Points 1, 2, and 4 are at the compressor inlet, compressor outlet, and evaporator inlet. A higher COP means a more efficient refrigerator or air conditioner.
Coal/Nuclear Power Plants: These use large-scale Rankine cycles. The boiler pressure (P_high in the simulator) is supercritical in advanced plants, exceeding 22 MPa, to achieve thermal efficiencies over 45%. Engineers use CAE tools to optimize every component, from the feedwater pump (η_p) to the last turbine stage (η_t).
Geothermal Power Generation: Uses the Rankine cycle with organic working fluids (like pentane) that boil at lower temperatures than water. This allows them to generate electricity from lower-grade heat sources. The simulator's pressure and temperature parameters are critical for designing these Organic Rankine Cycles (ORCs).
Household Refrigeration: Your fridge runs on the vapor-compression cycle. The evaporating temperature (T_evap) is set below your fridge's interior temperature to absorb heat. The compressor efficiency (η_c) directly impacts your electricity bill. CAE simulation helps design more efficient compressors and select optimal refrigerants.
HVAC & Heat Pumps: An air conditioner is a refrigeration cycle. A heat pump is the same cycle, but used for heating—its COP is even more critical. By adjusting the condensing and evaporating temperatures (T_cond & T_evap) in the simulator, you can model how a heat pump's performance changes between a mild fall day and a cold winter night.
First, there is a pitfall in the idea that "thermal efficiency or COP is simply better the higher it is." While drastically increasing boiler pressure in the simulator does improve thermal efficiency, in a real plant, material strength limits and costs skyrocket. For example, supercritical pressure power plants are highly efficient but require expensive special steels for piping and boilers. A design that pursues only efficiency is not realistic.
Next, a misconception regarding the "evaporation temperature" setting in refrigeration cycles. Raising the evaporation temperature does indeed improve COP, but this assumes "the temperature of the space you want to cool can be set higher." If a refrigerator requires -20°C, forcibly setting the evaporation temperature to -5°C drastically reduces cooling capacity, failing to achieve the objective altogether. It's crucial to understand the trade-off between COP and the required cooling capacity.
Finally, do not mistake "100% turbine efficiency" or "isentropic processes" for real-world targets. Setting it to 100% in the simulator is to create an ideal reference benchmark. In actual turbines, losses inevitably occur due to friction at blade tips, leakage, etc., with even large ones maxing out around 90%. Use this tool to experience how much output drops when you lower efficiency, and understand that "how to minimize losses" is the essence of engineering.
The calculations handled by this simulator are the very fundamentals of thermal fluid dynamics (CFD). For instance, detailed CFD simulations of the complex flows inside turbines and compressors are used to more accurately predict the values for "isentropic efficiency" dealt with here or to elucidate loss mechanisms.
They are also deeply connected to materials engineering and strength design. Materials for high-pressure boilers and high-temperature turbines must withstand high temperatures and pressures over long periods. Changing the "boiler pressure" in the simulator is the first step in considering the stress on materials and creep phenomena (where materials deform over time).
Furthermore, renewable energy technologies can be mentioned as application areas. For example, Ocean Thermal Energy Conversion (OTEC) operates a Rankine cycle using the temperature difference between warm surface seawater and cold deep seawater, but this difference is small, around 20–25°C. By experimenting in the simulator with what happens to thermal efficiency when you set the condenser temperature high and the evaporator temperature low, you can intuitively understand the challenges of this technology (low efficiency, large scale).
The first next step is to study the "wet steam" region in detail. The inside of the simulator's dome is the wet steam region, where state properties are determined by a parameter called dryness fraction (x). For example, enthalpy can be expressed as $h = h_f + x \cdot h_{fg}$. Here, $h_f$ is the enthalpy of saturated liquid and $h_{fg}$ is the latent heat of vaporization. Understanding this relationship will enable you to perform calculations yourself for when the turbine outlet is in the wet region.
Regarding the mathematical background, try exploring the partial derivatives of state properties and thermodynamic relations (like Maxwell's relations). If T-s or P-h diagrams are "maps," these equations are their "drawing rules." For example, understanding from these equations why isotherms slope the way they do in the vapor region on a P-h diagram will change how you view the charts.
Finally, once you've grasped the basics with this tool, I recommend moving on to learning about more complex cycles. Specific examples include the "regenerative cycle," which recovers heat discarded in the condenser; the "combined cycle," which pairs it with a gas turbine; and "cogeneration (combined heat and power)," which simultaneously provides refrigeration and power generation. All of these are essentially combinations and optimizations of the basic Rankine and refrigeration cycles you are now operating as building blocks.