Hydraulic Machinery

Principles of pumps and turbines, power calculations, characteristic curves, and cavitation.

Concept Overview

Hydraulic machines convert fluid energy into mechanical energy (turbines) or mechanical energy into fluid energy (pumps).

Pumps

Pumps increase the pressure head of a fluid. The most common types are centrifugal (radial flow) and axial flow pumps.

Pump Power

Hydraulic pump power is analyzed in two ways:

  • Water Power (PwP_w): The power delivered to the fluid.
  • Brake Power (PbP_b): The power supplied to the pump shaft by the motor.

Water Power Formula

Calculates the useful fluid power delivered to the water by the pump.

Pw=γQHP_w = \gamma Q H

Variables

SymbolDescriptionUnit
kN/m3kN/m^3
QQDischargem3/sm^3/s
HHTotal dynamic head (TDH)m

Brake Power Formula

Calculates the input power required at the pump shaft from the motor, accounting for pump efficiency.

Pb=PwηP_b = \frac{P_w}{\eta}

Variables

SymbolDescriptionUnit
PwP_wWater powerkW
Pump efficiencydecimal

Total Dynamic Head (TDH)

The total head against which the pump operates, representing the net energy increase per unit weight of fluid.

Total Dynamic Head (TDH)

Calculates the total dynamic head by summing static heads, friction losses, and velocity head differences between discharge and suction.

H=hs+hd+hf+Vd22gVs22gH = h_s + h_d + h_f + \frac{V_d^2}{2g} - \frac{V_s^2}{2g}

Variables

SymbolDescriptionUnit
hsh_sStatic suction liftm
hdh_dStatic discharge headm
hfh_fFriction losses in suction and discharge pipesm
VdV_dVelocity in discharge pipem/s
VsV_sVelocity in suction pipem/s
ggAcceleration due to gravitym/s2m/s^2

Turbines

Turbines extract energy from fluid flow to generate mechanical power (e.g., hydroelectric dams).

Turbine Power

The output power of a turbine represents the mechanical power extracted from the fluid. The turbine efficiency (η\eta) accounts for hydraulic, volumetric, and mechanical losses.

Turbine Output Power

Calculates the mechanical power output generated by a hydraulic turbine from the available fluid power.

P=γQHηP = \gamma Q H \eta

Variables

SymbolDescriptionUnit
PPOutput powerW
Specific weight of fluidN/m3N/m^3
QQDischargem3/sm^3/s
HHNet headm
Turbine efficiencydecimal

Specific Speed

Specific speed is a dimensionless parameter used to classify and select the most efficient type of pump or turbine for a given application.

Pump Specific Speed (NsN_s)

Pump specific speed is defined as the speed in RPM at which a geometrically similar pump would deliver 1 unit of flow rate at 1 unit of head. It depends only on the design shape of the impeller, not its physical size or actual operating speed.

Impeller selection based on NsN_s:

  • Low NsN_s: Centrifugal (Radial flow). High head, low flow.
  • Medium NsN_s: Mixed flow.
  • High NsN_s: Axial flow (Propeller). Low head, very high flow.

Pump Specific Speed

Calculates the specific speed of a pump to classify the impeller type based on operational parameters at the Best Efficiency Point (BEP).

Ns=NQH3/4N_s = \frac{N \sqrt{Q}}{H^{3/4}}

Variables

SymbolDescriptionUnit
NNPump rotational speedRPM
QQDischarge at Best Efficiency Point (BEP)m3/sm^3/s
HHHead per stage at BEPm

Turbine Specific Speed (NsN_s)

For turbines, specific speed is defined based on power output (PP) rather than discharge (QQ), since generating power is the primary goal.

Turbine selection based on NsN_s:

  • Low NsN_s: Pelton Wheel (Impulse turbine). Very high head (>200 m> 200\text{ m}), low flow rate.
  • Medium NsN_s: Francis Turbine (Reaction turbine). Medium head (40 m400 m40\text{ m} - 400\text{ m}), medium flow.
  • High NsN_s: Kaplan Turbine (Reaction turbine, axial flow). Low head (<40 m< 40\text{ m}), high flow.

Turbine Specific Speed

Calculates the specific speed of a turbine to classify and select the optimal turbine type based on power output and head.

Ns=NPH5/4N_s = \frac{N \sqrt{P}}{H^{5/4}}

Variables

SymbolDescriptionUnit
NNRotational speedRPM
PPPower output at design pointkW
HHNet headm

Characteristic Curves

Performance curves plot Head (HH), Power (PP), and Efficiency (η\eta) against Discharge (QQ) for a constant speed (NN).

  • Head-Discharge Curve (H-Q): Typically drops as QQ increases.
  • Efficiency Curve: Increases to a peak (Best Efficiency Point - BEP) and then drops.
  • Power Curve: Increases with QQ.

Affinity Laws

Affinity laws are scaling rules to predict pump or turbine performance under different operating conditions.

Pump Affinity Laws

When testing a single pump (where impeller diameter DD is constant) at different rotational speeds, performance parameters scale predictably. These scaling laws assume that hydraulic efficiency remains constant between different speeds, which is highly accurate for moderate changes in rotational speed.

The scaling relationships are:

  • Discharge (QQ): Varies directly with the rotational speed.
  • Head (HH): Varies with the square of the rotational speed.
  • Power (PP): Varies with the cube of the rotational speed.

Affinity Law for Discharge

Scales the volumetric flow rate of a pump linearly with rotational speed.

Q1Q2=N1N2\frac{Q_1}{Q_2} = \frac{N_1}{N_2}

Variables

SymbolDescriptionUnit
Q1Q_1Initial dischargem3/sm^3/s
Q2Q_2Final dischargem3/sm^3/s
N1N_1Initial speedRPM
N2N_2Final speedRPM

Affinity Law for Head

Scales the developed head of a pump quadratically with rotational speed.

H1H2=(N1N2)2\frac{H_1}{H_2} = \left(\frac{N_1}{N_2}\right)^2

Variables

SymbolDescriptionUnit
H1H_1Initial headm
H2H_2Final headm
N1N_1Initial speedRPM
N2N_2Final speedRPM

Affinity Law for Power

Scales the required shaft power of a pump cubically with rotational speed.

P1P2=(N1N2)3\frac{P_1}{P_2} = \left(\frac{N_1}{N_2}\right)^3

Variables

SymbolDescriptionUnit
P1P_1Initial shaft powerkW
P2P_2Final shaft powerkW
N1N_1Initial speedRPM
N2N_2Final speedRPM

Cavitation and NPSH

Cavitation occurs when the absolute pressure at the pump inlet drops below the vapor pressure (PvP_v) of the liquid. Bubbles form and collapse violently, causing damage, pitting, vibration, and loss of efficiency.

Net Positive Suction Head (NPSH)

The absolute head at the pump inlet above the vapor pressure head of the liquid, serving as the margin of safety against cavitation.

Cavitation Prevention Criterion

The governing condition that must be met to ensure cavitation does not occur within the pump.

NPSHavailable>NPSHrequiredNPSH_{\text{available}} > NPSH_{\text{required}}

Variables

SymbolDescriptionUnit
Net Positive Suction Head available from the system installationm
Net Positive Suction Head required by the pump manufacturerm

NPSH Available (NPSHANPSH_A)

Calculates the Net Positive Suction Head available in a static suction lift installation.

NPSHA=PatmγhshfsPvγNPSH_A = \frac{P_{\text{atm}}}{\gamma} - h_s - h_{fs} - \frac{P_v}{\gamma}

Variables

SymbolDescriptionUnit
Atmospheric pressurekPa
Specific weight of the fluidkN/m3kN/m^3
hsh_sStatic suction lift (vertical distance from liquid level to impeller centerline)m
hfsh_{fs}Friction head loss in the suction pipingm
PvP_vVapor pressure of the liquid at operating temperaturekPa
Key Takeaways
  • Pumps add energy to a fluid system, increasing its total dynamic head (TDH).
  • Affinity Laws predict performance changes when altering pump speed: Flow scales linearly (QNQ \propto N), Head scales quadratically (HN2H \propto N^2), and Power scales cubically (PN3P \propto N^3).
  • Water Power (PwP_w) is the useful energy gained by the fluid, while Brake Power (PbP_b) is the total energy supplied by the motor. Brake power is always greater due to efficiency losses (η<1\eta < 1).
  • Turbines extract energy from a moving fluid to convert it into mechanical work, where efficiency (η\eta) is in the numerator since output power is less than input fluid power.
  • Specific Speed (NsN_s) is a design index used to select the optimal machinery type: centrifugal/impulse (low NsN_s), mixed/Francis (medium NsN_s), and axial/Kaplan (high NsN_s).
  • Cavitation is avoided when the available Net Positive Suction Head (NPSHANPSH_A) exceeds the required head (NPSHRNPSH_R).