In Polytropic process the product of Pressure and Volume (PV) power 'n' is constant
where,
'n' is polytropic index
Polytropic work refers to the work done in a process where the relationship between pressure and volume follows a specific power-law equation (P*V^n = constant). It is commonly encountered in compressible flow systems and is expressed as the area under the curve on a P-V diagram for a polytropic process.
The polytropic index in thermodynamics is a measure of how a gas behaves during a polytropic process, where pressure and volume change. It indicates the relationship between pressure and volume changes in the process. The value of the polytropic index affects the efficiency and work done in the process. A higher polytropic index means more work is done, while a lower index means less work is done.
A polytropic process is a process where ( P ) ( V )^n is maintained throughout the process; commonly a compression or an expansion. The n is called the polytropic exponent and is often between 1.0 and k , the specific heat ratio. For a reversible, polytropic, and nonflow process : WB = [ ( P2 ) ( V2 ) - ( P1 ) ( V1 ) ] / [ 1 - n ] or WB = [ 1 / 1 - n ][ ( P1 ) ( V1 ] [ ( P2 / P1 )^B - 1 ] B = ( n - 1 ) / ( n ) For a reversible, polytropic, and steady flow process : WSF = [ n / 1 - n ] [ ( P1 ) ( V1 )] [ ( P2 / P1 )^B - 1 ] B = ( n - 1 ) / ( n )
An example problem of a polytropic process is when a gas undergoes compression or expansion while its pressure and volume change, following a specific mathematical relationship known as a polytropic equation.
The value of the polytropic exponent 'n' in a reversible polytropic process typically varies between 0 and ∞. However, common values for n are between 0 (isobaric process) and 1 (isothermal process) for ideal gases.
the value of polytropic exponent "n" in reversible process will vary from 1 to adiabatic constant "gamma"
Polytropic work refers to the work done in a process where the relationship between pressure and volume follows a specific power-law equation (P*V^n = constant). It is commonly encountered in compressible flow systems and is expressed as the area under the curve on a P-V diagram for a polytropic process.
The polytropic index in thermodynamics is a measure of how a gas behaves during a polytropic process, where pressure and volume change. It indicates the relationship between pressure and volume changes in the process. The value of the polytropic index affects the efficiency and work done in the process. A higher polytropic index means more work is done, while a lower index means less work is done.
A polytropic process is a process where ( P ) ( V )^n is maintained throughout the process; commonly a compression or an expansion. The n is called the polytropic exponent and is often between 1.0 and k , the specific heat ratio. For a reversible, polytropic, and nonflow process : WB = [ ( P2 ) ( V2 ) - ( P1 ) ( V1 ) ] / [ 1 - n ] or WB = [ 1 / 1 - n ][ ( P1 ) ( V1 ] [ ( P2 / P1 )^B - 1 ] B = ( n - 1 ) / ( n ) For a reversible, polytropic, and steady flow process : WSF = [ n / 1 - n ] [ ( P1 ) ( V1 )] [ ( P2 / P1 )^B - 1 ] B = ( n - 1 ) / ( n )
An example problem of a polytropic process is when a gas undergoes compression or expansion while its pressure and volume change, following a specific mathematical relationship known as a polytropic equation.
The value of the polytropic exponent 'n' in a reversible polytropic process typically varies between 0 and ∞. However, common values for n are between 0 (isobaric process) and 1 (isothermal process) for ideal gases.
Thermodynamic polytropic processes are processes that can be described using the polytropic equation ( PV^n = C ), where ( P ) is pressure, ( V ) is volume, ( N ) is the polytropic exponent, and ( C ) is a constant. These processes can encompass a range of behaviors, from isobaric to isothermal to adiabatic processes, depending on the value of the polytropic exponent.
The term "polytropic" refers to a thermodynamic process that follows the equation (PV^n = \text{constant}), where (P) is pressure, (V) is volume, and (n) is the polytropic index. This index can take on various values, allowing the process to represent different thermodynamic behaviors, including isothermal ((n = 1)) and adiabatic ((n = \gamma)) processes. Polytropic processes are often used in engineering to model the behavior of gases in compression and expansion processes.
A polytropic process, characterized by the relationship ( PV^n = \text{constant} ), offers several advantages, such as the ability to model various thermodynamic processes (isothermal, adiabatic, etc.) by adjusting the polytropic index ( n ). This flexibility makes it useful in engineering applications where different behaviors of gases are observed. However, disadvantages include the complexity of calculating work done and heat transfer, as it often requires specific values of ( n ) that may not be easily determined in practice. Additionally, assuming a polytropic process may oversimplify real gas behavior, leading to inaccuracies in predictions.
In a reversible polytropic process, the work done can be calculated using the formula ( W = \frac{P_2 V_2 - P_1 V_1}{n - 1} ), where ( P_1 ) and ( P_2 ) are the initial and final pressures, ( V_1 ) and ( V_2 ) are the initial and final volumes, and ( n ) is the polytropic index. Alternatively, it can also be expressed as ( W = \frac{P_1 V_1}{n} \left( \left( \frac{V_2}{V_1} \right)^{n} - 1 \right) ) if the volume ratios are known. This work is determined by integrating the pressure-volume relationship for a polytropic process, represented by ( PV^n = \text{constant} ).
See wikipedia article on polytropic processes.
In a polytropic process, the net heat change depends on the specific conditions of the process (e.g., if it is adiabatic or not, reversible or irreversible). In general, the net heat change can be calculated by comparing the heat added or removed during the process with the work done by the system.