According to Bernoulli's principle, as the velocity of a fluid increases, the pressure within the fluid decreases.

During the adiabatic expansion phase of the Carnot cycle, the working substance does work on the surroundings as it expands.

The efficiency of a Carnot cycle is given by the formula η = 1 - (T_c/T_h), where T_c is the temperature of the cold reservoir and T_h is the temperature of the hot reservoir.

The efficiency of a Carnot cycle is given by the formula η = 1 - (T_c/T_h), where T_c is the temperature of the cold reservoir and T_h is the temperature of the hot reservoir.

In a Carnot cycle, the hot reservoir must be at a higher temperature than the cold reservoir for the cycle to operate.

In a Carnot cycle, the isothermal process occurs during the heat absorption from the hot reservoir, where the temperature remains constant.

In a closed system, if the internal energy increases, it means that heat must be added or work must be done on the system.

The working fluid in a Rankine cycle is typically water, which is used to convert heat into work.

In an ideal gas, the internal energy increases with an increase in temperature.

Conduction is the transfer of heat through direct contact between materials.

Radiation is the mode of heat transfer that does not require a medium; it can occur through a vacuum.

Convection is the mode of heat transfer that involves the movement of fluid, where heat is carried by the fluid as it moves.

The Rankine cycle typically uses water as the working fluid due to its favorable thermodynamic properties.

The Rankine cycle typically uses water as the working fluid, which undergoes phase changes to absorb and release heat.

The second law of thermodynamics states that the entropy of the universe tends to increase, indicating the direction of spontaneous processes.

Entropy is defined as a measure of disorder or randomness in a system, reflecting the number of microscopic configurations that correspond to a thermodynamic system's macroscopic state.

The efficiency of a Carnot engine is given by the formula 1 - (T_c / T_h), where T_h is the temperature of the hot reservoir and T_c is the temperature of the cold reservoir.

The main advantage of using a Carnot engine is that it operates at maximum efficiency, as it is an idealized engine.

The main function of a heat exchanger is to transfer heat between two or more fluids without mixing them.

The efficiency of a Carnot engine is given by the formula η = 1 - (T_C/T_H), where T_H is the temperature of the hot reservoir and T_C is the temperature of the cold reservoir.

The maximum efficiency of a Carnot engine is given by the formula η = 1 - (T_c/T_h), where T_c is the cold reservoir temperature and T_h is the hot reservoir temperature.

The primary function of a heat exchanger is to transfer heat between two or more fluids without mixing them.

Conduction is the primary mechanism of heat transfer that occurs through direct contact of particles in a solid material.

The primary purpose of a heat engine is to convert heat energy into mechanical work by utilizing the temperature difference between two reservoirs.

The primary purpose of a heat exchanger is to transfer heat between two fluids without mixing them.

The primary purpose of the Rankine cycle is to convert thermal energy into mechanical work, typically used in power generation.

In heat transfer basics, the rate of heat transfer is directly proportional to the temperature difference between two bodies, as described by Fourier's law.

The second law of thermodynamics is concerned with the direction of heat transfer and the concept of entropy, stating that heat cannot spontaneously flow from a colder body to a hotter body.

The second law of thermodynamics states that heat cannot spontaneously flow from a colder body to a hotter body, which defines the direction of heat transfer.

The Carnot cycle is significant because it represents the maximum possible efficiency that any heat engine can achieve operating between two temperatures.