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Specific Work Turbo Machines

Reference data and engineering information about specific work turbo machines for dynamics applications.

specificworkturbomachines

Overview

Engineering reference data for Specific Work Turbo Machines in dynamics.

Key Formulas

Newton's Second Law

F=maF = ma

Force = mass × acceleration.

Kinetic Energy

Ek=12mv2E_k = \frac{1}{2}mv^2

Energy of motion.

Momentum

p=mvp = mv

Mass × velocity.

Work

W=FdcosθW = Fd\cos\theta

Force × displacement × cos(angle).

Variables

Symbol Description Unit
FF Force N
mm Mass kg
aa Acceleration m/s²
vv Velocity m/s
EkE_k Kinetic energy J

Calculations

Pump and Fan (Incompressible Fluid)

Specific work of a pump or fan: w=p2p1ρ(1)w = \frac{p_2 - p_1}{\rho} \quad \text{(1)} where ww is specific work (J/kg), pp is pressure (Pa), and ρ\rho is fluid density (kg/m³).

Turbine (Incompressible Fluid)

Specific work of a turbine: w=p1p2ρ(2)w = \frac{p_1 - p_2}{\rho} \quad \text{(2)}

Compressor (Isentropic Process)

For a compressor working with a compressible fluid under isentropic conditions: p1v1κ=p2v2κ(3)p_1 v_1^\kappa = p_2 v_2^\kappa \quad \text{(3)} The specific work can be calculated as: w=κκ1RT1((p2p1)κ1κ1)(4)w = \frac{\kappa}{\kappa - 1} R T_1 \left( \left(\frac{p_2}{p_1}\right)^{\frac{\kappa-1}{\kappa}} - 1 \right) \quad \text{(4)} where RR is the individual gas constant (J/kg·K), T1T_1 is absolute inlet temperature (K), and κ=cp/cv\kappa = c_p/c_v.

Gas Turbine (Isentropic Expansion)

Specific work for a gas turbine: w=κκ1RT1(1(p2p1)κ1κ)(5)w = \frac{\kappa}{\kappa - 1} R T_1 \left( 1 - \left(\frac{p_2}{p_1}\right)^{\frac{\kappa-1}{\kappa}} \right) \quad \text{(5)}

Head Conversion

Specific work relates to head via the energy equation: w=gh(6)w = g h \quad \text{(6)} h=wg(7)h = \frac{w}{g} \quad \text{(7)} where hh is head (m) and gg is acceleration due to gravity (m/s²).

Worked Examples

Example: Water Pump

A water pump increases pressure from 1×1051 \times 10^5 Pa to 10×10510 \times 10^5 Pa. For water (ρ=1000\rho = 1000 kg/m³): w=(10×105)(1×105)1000=900 J/kgw = \frac{(10 \times 10^5) - (1 \times 10^5)}{1000} = 900 \text{ J/kg} hwater=9009.81=91.74 mh_{\text{water}} = \frac{900}{9.81} = 91.74 \text{ m}

Example: Air Compressor

An air compressor compresses air at 20°C20°C (293293 K) from 1 bar to 10 bar. Using air properties (κair=1.4\kappa_{\text{air}} = 1.4, Rair=286.9R_{\text{air}} = 286.9 J/kg·K): w=1.41.41286.9293((10×1051×105)0.41.41)=273,826 J/kgw = \frac{1.4}{1.4 - 1} \cdot 286.9 \cdot 293 \left( \left(\frac{10 \times 10^5}{1 \times 10^5}\right)^{\frac{0.4}{1.4}} - 1 \right) = 273,826 \text{ J/kg} hair=273,8269.8127,951 mh_{\text{air}} = \frac{273,826}{9.81} \approx 27,951 \text{ m}

References