4.3 Pump Selection, System Curves, NPSH & Cavitation

Key Takeaways

  • A pump's operating point is established at the exact intersection of the pump manufacturer head curve (Hpump(Q)H_{\text{pump}}(Q)) and the system head curve (Hsys(Q)=Hstatic+kQ2H_{\text{sys}}(Q) = H_{\text{static}} + k Q^2).

  • Pump Affinity Laws dictate that for speed variations (NN), flow scales linearly (Q∝NQ \propto N), head scales quadratically (H∝N2H \propto N^2), and brake horsepower scales cubically (P∝N3P \propto N^3).

  • In series configurations, pump heads add at constant flow (Htotal=H1+H2H_{\text{total}} = H_1 + H_2), whereas in parallel configurations, flows add at constant head (Qtotal=Q1+Q2Q_{\text{total}} = Q_1 + Q_2).

  • Specific speed Ns=NQH3/4N_s = \frac{N \sqrt{Q}}{H^{3/4}} dictates impeller geometry, progressing from radial flow (low NsN_s, high head) to mixed flow, to axial propeller flow (high NsN_s, high flow, low head).

  • To prevent destructive cavitation, Net Positive Suction Head Available (NPSHA=p0−pvγ±zs−hfsNPSHA = \frac{p_0 - p_v}{\gamma} \pm z_s - h_{fs}) must exceed Net Positive Suction Head Required (NPSHRNPSHR) with a safe engineering margin.

Last updated: August 2026

Pump Selection, System Curves, NPSH & Cavitation

Pumps add mechanical energy to fluids to overcome elevation differences, maintain pressure boundaries, and balance frictional head losses in piping networks. For mechanical engineers, sizing a pump requires analyzing pump performance and system curves, applying affinity laws for variable-speed drives (VFDs), selecting impellers via specific speed (NsN_s), and conducting rigorous Net Positive Suction Head (NPSH) calculations to prevent destructive cavitation.

+---------------------------------------------------------------------------------------------------+
|                         PUMP & PIPING SYSTEM INTERACTION MATRIX                                   |
|                                                                                                   |
|   [PUMP PERFORMANCE CURVES]         [SYSTEM HEAD CURVE]            [OPERATING POINT MATCH]        |
|   - H_pump vs Q (Manufacturer)      - H_sys = H_static + k*Q^2     - Intersection: H_pump = H_sys |
|   - Efficiency \eta vs Q            - Static Lift: \Delta z, \Delta P - Best Efficiency Point (BEP)|
|   - BHP = \gamma*Q*H / (550*\eta)   - Dynamic Friction: k*Q^2      - Series / Parallel Balancing  |
|                                              |                                                    |
|                                              v                                                    |
|                                     [CAVITATION GUARD]                                            |
|                                     - NPSHA = (p0 - pv)/\gamma +/- zs - h_fs                       |
|                                     - Design Requirement: NPSHA >= NPSHR + Margin                 |
+---------------------------------------------------------------------------------------------------+

1. Pump Classifications: Dynamic vs. Positive Displacement

+---------------------------------------------------------------------------------------------------+
|                                 PUMP CLASSIFICATION TAXONOMY                                      |
|                                                                                                   |
|   1. DYNAMIC (TURBOMACHINERY):                                                                    |
|      - Centrifugal (Radial Flow): High head, moderate flow (fluid enters axially, exits radially) |
|      - Mixed Flow: Medium head, medium flow (combined radial/axial discharge)                     |
|      - Axial Flow (Propeller): Low head (< 30 ft), high flow (> 10,000 gpm)                       |
|                                                                                                   |
|   2. POSITIVE DISPLACEMENT (PD):                                                                  |
|      - Reciprocating: Piston, Plunger, Diaphragm (High pressure, pulsating, constant volume)      |
|      - Rotary: Gear, Screw, Lobe, Vane (Viscous oils, constant non-pulsating discharge)          |
|      - Key Feature: Delivers constant flow regardless of discharge head; requires PRVs!           |
+---------------------------------------------------------------------------------------------------+

Power & Efficiency Formulations

+---------------------------------------------------------------------------------------------------+
|                             PUMP POWER CALCULATION FORMULAS                                       |
|                                                                                                   |
|   US CUSTOMARY UNITS:                                                                             |
|   - Water Horsepower (Hydraulic Power):    WHP = \frac{Q (\text{gpm}) \times H (\text{ft}) \times SG}{3960}  |
|   - Brake Horsepower (Shaft Power):        BHP = \frac{WHP}{\eta_{\text{pump}}} = \frac{Q \times H \times SG}{3960 \times \eta_{\text{pump}}} |
|   - Motor Input Electrical Power:          P_{\text{in}} = \frac{BHP \times 0.7457}{\eta_{\text{motor}}} \; [\text{kW}] |
|                                                                                                   |
|   SI METRIC UNITS:                                                                                |
|   - Hydraulic Power:                       P_{\text{hyd}} = \rho g Q H = \gamma Q H  [\text{Watts}]|
|   - Brake Power:                           P_{\text{brake}} = \frac{\rho g Q H}{\eta_{\text{pump}}} [\text{Watts}] |
+---------------------------------------------------------------------------------------------------+

Note

Derivation of 3960 Constant: In US Customary units: 1 gpm=1448.83 cfs1\text{ gpm} = \frac{1}{448.83}\text{ cfs}, γwater=62.43 lbf/ft3\gamma_{\text{water}} = 62.43\text{ lbf/ft}^3, and 1 hp=550 ft⋅lbf/s1\text{ hp} = 550\text{ ft}\cdot\text{lbf/s}. Power (hp)=Q(gpm)×1448.83 ft3/s×62.43SG lbf/ft3×H(ft)550 ft⋅lbf/s=Q×H×SG3960\text{Power (hp)} = \frac{Q (\text{gpm}) \times \frac{1}{448.83}\text{ ft}^3/\text{s} \times 62.43 SG \text{ lbf/ft}^3 \times H (\text{ft})}{550\text{ ft}\cdot\text{lbf/s}} = \frac{Q \times H \times SG}{3960}


2. System Head Curves and Operating Point Determination

The total dynamic head (HsysH_{\text{sys}}) required by a piping network is partitioned into static head (HstaticH_{\text{static}}) and dynamic friction head (HdynamicH_{\text{dynamic}}):

Hsys(Q)=Hstatic+Hdynamic=(z2−z1+p2−p1γ)+kQ2H_{\text{sys}}(Q) = H_{\text{static}} + H_{\text{dynamic}} = \left( z_2 - z_1 + \frac{p_2 - p_1}{\gamma} \right) + k Q^2

Where:

  • Hstatic=(z2−z1)+p2−p1γH_{\text{static}} = (z_2 - z_1) + \frac{p_2 - p_1}{\gamma} is independent of flow rate QQ.
  • k=8π2gD4(fLD+∑K)k = \frac{8}{\pi^2 g D^4} \left( f \frac{L}{D} + \sum K \right) is the network hydraulic resistance constant.
   Head (H)
       ^
       |                                                  Pump Characteristic: H_pump(Q)
       |  H_0 +---------------------\ 
       |      |                      \\
       |      |                        \\      OPERATING POINT
       |  H_op|--------------------------(•) [Q_op, H_op]
       |      |                         / \\
       |      |                        /    \\
       |      |                       /       \\
       |  H_st+                      /          \\
       |      |   System Curve:     /             \\ 
       |      |   H_sys = H_st + kQ^2               \\
       +------+--------------------+-------------------> Flow Rate (Q)
              0                   Q_op

Series and Parallel Pump Combinations

  • Pumps in Series (High Head):
    • Flow rate through each pump is identical: Qtotal=Q1=Q2Q_{\text{total}} = Q_1 = Q_2.
    • Combined head is the vertical sum of individual heads: Htotal(Q)=H1(Q)+H2(Q)H_{\text{total}}(Q) = H_1(Q) + H_2(Q).
    • Used when piping system resistance exhibits steep static lift or extreme friction.
  • Pumps in Parallel (High Flow):
    • Head produced across each branch is identical: Htotal=H1=H2H_{\text{total}} = H_1 = H_2.
    • Combined flow is the horizontal sum of individual flows: Qtotal(H)=Q1(H)+Q2(H)Q_{\text{total}}(H) = Q_1(H) + Q_2(H).
    • Used in flat system curves where high volumetric throughput is required.
+---------------------------------------------------------------------------------------------------+
|                             SERIES VS. PARALLEL COMBINATIONS                                      |
|                                                                                                   |
|   SERIES (Add Heads vertically at given Q):        PARALLEL (Add Flows horizontally at given H):  |
|          Head H                                           Head H                                  |
|            ^                                                ^                                     |
|            |    Combined (H_1 + H_2)                        |                                     |
|            |         /\                                     |     Pump 1    Combined (Q_1 + Q_2)  |
|            |        /  \                                    |       \            \              |
|            |    Pump 1   \                                  |--------+------------+----           |
|            |       \      \                                 |        |            |               |
|            +--------+------+----> Flow Q                    +--------+------------+----> Flow Q   |
|                     Q_1                                              Q_1         Q_total          |
+---------------------------------------------------------------------------------------------------+

3. Pump Affinity Laws

The Affinity Laws describe how centrifugal pump performance scales when rotational speed (NN) or impeller diameter (DD) is altered:

+---------------------------------------------------------------------------------------------------+
|                                    PUMP AFFINITY LAWS                                             |
|                                                                                                   |
|   SPEED VARIATION (Constant Impeller Diameter D_1 = D_2):                                         |
|   $$\frac{Q_2}{Q_1} = \frac{N_2}{N_1}$$                                                           |
|   $$\frac{H_2}{H_1} = \left( \frac{N_2}{N_1} \right)^2$$                                          |
|   $$\frac{P_2}{P_1} = \left( \frac{N_2}{N_1} \right)^3$$                                          |
|                                                                                                   |
|   DIAMETER VARIATION (Constant Rotational Speed N_1 = N_2, Small Trims < 15%):                    |
|   $$\frac{Q_2}{Q_1} = \frac{D_2}{D_1}$$                                                           |
|   $$\frac{H_2}{H_1} = \left( \frac{D_2}{D_1} \right)^2$$                                          |
|   $$\frac{P_2}{P_1} = \left( \frac{D_2}{D_1} \right)^3$$                                          |
|                                                                                                   |
|   COMBINED VARIATION:                                                                             |
|   $$\frac{Q_2}{Q_1} = \left(\frac{N_2}{N_1}\right)\left(\frac{D_2}{D_1}\right), \quad             |
|     \frac{H_2}{H_1} = \left(\frac{N_2}{N_1}\right)^2\left(\frac{D_2}{D_1}\right)^2, \quad        |
|     \frac{P_2}{P_1} = \left(\frac{N_2}{N_1}\right)^3\left(\frac{D_2}{D_1}\right)^3$$             |
+---------------------------------------------------------------------------------------------------+

Warning

Affinity Law Exam Trap on Static Head Systems: Affinity laws track the locus of points at constant efficiency along parabolas H∝Q2H \propto Q^2 originating from (0,0)(0,0). When a pump is throttled via VFD in a system with high static head (Hstatic>0H_{\text{static}} > 0), the new operating point does not follow Q2/Q1=N2/N1Q_2/Q_1 = N_2/N_1 directly. You must transform the pump curve points via affinity laws and find the new intersection with Hsys=Hstatic+kQ2H_{\text{sys}} = H_{\text{static}} + k Q^2.


4. Specific Speed and Impeller Classification

Specific Speed (NsN_s) is a dimensionless (or standardized dimensional) index that characterizes the geometric shape of a pump impeller at its Best Efficiency Point (BEP):

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

Where (in US Customary engineering conventions): N=Speed (rpm)N = \text{Speed (rpm)}, Q=Flow at BEP (gpm)Q = \text{Flow at BEP (gpm)}, H=Head per stage at BEP (ft)H = \text{Head per stage at BEP (ft)}.

Impeller TypeSpecific Speed Range (NsN_s, US)Flow GeometryHead vs. Flow Characteristic
Radial Vane (Centrifugal)500−1500500 - 1500Pure Radial dischargeHigh head, low flow rate
Francis Vane1500−40001500 - 4000Radial-to-axial turnModerate-to-high head, medium flow
Mixed Flow4000−90004000 - 9000Diagonal dischargeMedium head, high flow rate
Axial Flow (Propeller)9000−15000+9000 - 15000+Pure Axial flowLow head (<30 ft< 30\text{ ft}), extreme flow
+---------------------------------------------------------------------------------------------------+
|                         SUCTION SPECIFIC SPEED (N_ss) & RECIRCULATION                             |
|                                                                                                   |
|   Formula:   N_{ss} = \frac{N \sqrt{Q}}{(NPSHR)^{3/4}}                                            |
|                                                                                                   |
|   - Industry Standard (Hydraulic Institute): Safe N_ss is typically 8,500 to 11,000.              |
|   - N_ss > 12,000: Extreme risk of suction recirculation, cavitation surges, and shaft fatigue.   |
+---------------------------------------------------------------------------------------------------+

5. Cavitation Mechanics and Net Positive Suction Head (NPSH)

The Physics of Cavitation Damage

Cavitation occurs when the local static pressure inside the pump suction eye drops below the liquid's saturation vapor pressure (p<pvp < p_v at the operating temperature). Vapor cavities (bubbles) nucleate instantly. As these vapor bubbles travel into regions of higher pressure along the impeller vanes, they implode violently within microseconds, generating microscopic liquid micro-jets with localized impact pressures exceeding 1000 MPa1000\text{ MPa} (150,000 psi150,000\text{ psi}). This causes pitting erosion, structural vibration, acoustic rattling ("pumping gravel"), and sudden collapse of pump head and efficiency.

+---------------------------------------------------------------------------------------------------+
|                         NET POSITIVE SUCTION HEAD (NPSH) DEFINITIONS                              |
|                                                                                                   |
|   1. NPSHA (Available): Determined strictly by the suction piping geometry, elevations, and fluid |
|      NPSHA = \frac{p_{s,\text{total}}}{\gamma} - \frac{p_v}{\gamma}                                |
|            = \frac{p_0}{\gamma} \pm z_s - h_{fs} - \frac{p_v}{\gamma}                             |
|                                                                                                   |
|   2. NPSHR (Required): Determined strictly by the pump manufacturer via testing (3% head drop)    |
|                                                                                                   |
|   3. CAVITATION AVOIDANCE CRITERION:                                                              |
|      NPSHA >= NPSHR + NPSH_{\text{margin}}   (Typical margin: 3 to 5 ft or 1.10 to 1.25 * NPSHR) |
+---------------------------------------------------------------------------------------------------+
   Suction Tank
      |~~~| Liquid surface at pressure p_0 (e.g., p_atm)
      +---+
        | 
        | +z_s (Flooded Suction: Tank above pump)
        | -z_s (Suction Lift: Tank below pump)
        v
     [ PUMP ]  <--- Suction eye where p_min occurs
        |             h_fs = Suction line friction + entrance + valve head losses
        +---------> p_v = Vapor pressure of liquid at operating temperature

Detailed Variable Definitions for NPSHA Calculation:

  • p0=Absolute pressure on the suction supply surface (Pa abs or psia)p_0 = \text{Absolute pressure on the suction supply surface } (\text{Pa abs or psia}). For open tanks, p0=patmp_0 = p_{\text{atm}}. For closed pressurized deaerators/condensers, p0=ptank, absp_0 = p_{\text{tank, abs}}.
  • zs=Static elevation difference between liquid surface and pump impeller centerlinez_s = \text{Static elevation difference between liquid surface and pump impeller centerline}. (Positive for flooded suction; negative for suction lift).
  • hfs=Total head loss in the suction piping system=(fLsDs+∑Ks)Vs22gh_{fs} = \text{Total head loss in the suction piping system} = \left( f \frac{L_s}{D_s} + \sum K_s \right) \frac{V_s^2}{2g}.
  • pv=Absolute saturation vapor pressure of the pumped liquid at operating temperaturep_v = \text{Absolute saturation vapor pressure of the pumped liquid at operating temperature}.
  • γ=ρg=Specific weight of the pumped fluid at operating temperature\gamma = \rho g = \text{Specific weight of the pumped fluid at operating temperature}.

Thoma's Cavitation Parameter (σ\sigma)

σ=NPSHRH\sigma = \frac{NPSHR}{H}

Cavitation begins when the plant suction condition reaches the critical cavitation parameter: σplant=NPSHAH≤σc\sigma_{\text{plant}} = \frac{NPSHA}{H} \le \sigma_c.

Corrective Strategies to Increase NPSHA When NPSHA<NPSHRNPSHA < NPSHR:

  1. Raise the suction supply vessel elevation (increase +zs+z_s).
  2. Lower the pump elevation into a pit or basement.
  3. Increase the suction pipe diameter DsD_s (reduces velocity VsV_s and dramatically lowers friction hfs∝1/D5h_{fs} \propto 1/D^5).
  4. Remove restrictive suction valves, eliminate elbows, or replace standard elbows with long-radius sweeps.
  5. Subcool the fluid to lower saturation vapor pressure pvp_v.
  6. Select a larger pump operating at a lower rotational speed NN.

6. Step-by-Step Worked Engineering Problem

Problem Statement

A centrifugal pump transfers hot industrial water at 80∘C80^\circ\text{C} (176∘F176^\circ\text{F}) from an open atmospheric storage reservoir (patm=101.3 kPap_{\text{atm}} = 101.3\text{ kPa}) to an elevated pressurized process reactor at a rate of Q=120 m3/hQ = 120\text{ m}^3/\text{h} (0.03333 m3/s=33.33 L/s0.03333\text{ m}^3/\text{s} = 33.33\text{ L/s}). The pump is located 2.5 m2.5\text{ m} below the reservoir water surface (flooded suction, zs=+2.5 mz_s = +2.5\text{ m}). The suction line consists of 12 m12\text{ m} of 150 mm150\text{ mm} inner diameter pipe with total friction and minor loss coefficient ∑(fL/D+K)=3.2\sum (f L/D + K) = 3.2.

Water properties at 80∘C80^\circ\text{C}:

  • Density: ρ=971.8 kg/m3\rho = 971.8\text{ kg/m}^3
  • Specific weight: γ=ρg=971.8×9.81=9.533 kN/m3\gamma = \rho g = 971.8 \times 9.81 = 9.533\text{ kN/m}^3
  • Saturation vapor pressure: pv=47.39 kPa absp_v = 47.39\text{ kPa abs}

The pump manufacturer curve specifies NPSHR=4.2 mNPSHR = 4.2\text{ m} at this operating flow. The total dynamic head required by the system is H=45.0 mH = 45.0\text{ m} with pump efficiency ηp=0.76\eta_p = 0.76.

Determine:

  1. The suction line velocity VsV_s and suction line head loss hfsh_{fs}.
  2. The Net Positive Suction Head Available (NPSHANPSHA) and the cavitation safety margin (NPSHA−NPSHRNPSHA - NPSHR).
  3. The pump Brake Horsepower (BHPBHP) in kilowatts.

Step-by-Step Solution

Step 1: Suction Line Velocity & Friction Loss

  • Suction pipe area: As=π(0.150)24=0.01767 m2A_s = \frac{\pi (0.150)^2}{4} = 0.01767\text{ m}^2.
  • Velocity: Vs=0.03333 m3/s0.01767 m2=1.886 m/sV_s = \frac{0.03333\text{ m}^3/\text{s}}{0.01767\text{ m}^2} = 1.886\text{ m/s}.
  • Velocity head: Vs22g=(1.886)22×9.81=3.55719.62=0.1813 m\frac{V_s^2}{2g} = \frac{(1.886)^2}{2 \times 9.81} = \frac{3.557}{19.62} = 0.1813\text{ m}.
  • Suction head loss: hfs=[∑(fLD+K)]Vs22g=3.2×0.1813 m=0.580 mh_{fs} = \left[ \sum \left( f \frac{L}{D} + K \right) \right] \frac{V_s^2}{2g} = 3.2 \times 0.1813\text{ m} = 0.580\text{ m}

Step 2: Net Positive Suction Head Available (NPSHANPSHA)

  • Convert pressures to head of pumped liquid at 80∘C80^\circ\text{C}: p0γ=101.325 kPa9.533 kN/m3=10.629 m\frac{p_0}{\gamma} = \frac{101.325\text{ kPa}}{9.533\text{ kN/m}^3} = 10.629\text{ m} pvγ=47.39 kPa9.533 kN/m3=4.971 m\frac{p_v}{\gamma} = \frac{47.39\text{ kPa}}{9.533\text{ kN/m}^3} = 4.971\text{ m}
  • Calculate NPSHANPSHA: NPSHA=p0γ+zs−hfs−pvγNPSHA = \frac{p_0}{\gamma} + z_s - h_{fs} - \frac{p_v}{\gamma} NPSHA=10.629 m+2.500 m−0.580 m−4.971 m=7.578 m≈7.58 mNPSHA = 10.629\text{ m} + 2.500\text{ m} - 0.580\text{ m} - 4.971\text{ m} = 7.578\text{ m} \approx 7.58\text{ m}
  • Cavitation Margin: Margin=NPSHA−NPSHR=7.58 m−4.20 m=+3.38 m>0(Safe from Cavitation)\text{Margin} = NPSHA - NPSHR = 7.58\text{ m} - 4.20\text{ m} = +3.38\text{ m} > 0 \quad (\text{Safe from Cavitation})

Step 3: Brake Horsepower Calculation

  • Hydraulic Power: Phyd=γQH=(9533 N/m3)×(0.03333 m3/s)×(45.0 m)=14,297 W=14.30 kWP_{\text{hyd}} = \gamma Q H = (9533\text{ N/m}^3) \times (0.03333\text{ m}^3/\text{s}) \times (45.0\text{ m}) = 14,297\text{ W} = 14.30\text{ kW}
  • Brake Power required at pump shaft: Pbrake=Phydηp=14.297 kW0.76=18.81 kWP_{\text{brake}} = \frac{P_{\text{hyd}}}{\eta_p} = \frac{14.297\text{ kW}}{0.76} = 18.81\text{ kW}

7. Common Exam Traps & PE Pro-Tips

Tip

Boiler Feedwater / Deaerator NPSH Rule: In closed deaerators or saturated steam drums, the water surface is in saturated thermodynamic equilibrium with the vapor space above it (p0=pvp_0 = p_v). Thus, p0γ−pvγ=0\frac{p_0}{\gamma} - \frac{p_v}{\gamma} = 0, reducing the NPSHA equation strictly to: NPSHA=zs−hfsNPSHA = z_s - h_{fs} In such systems, the deaerator tank must be elevated high above the feed pump (zs>NPSHR+hfsz_s > NPSHR + h_{fs}); suction lift is physically impossible.

Warning

Common Traps to Avoid:

  • Trap 1 — Gauge Pressure in NPSHA: Never plug gauge pressure into p0p_0 or pvp_v. If patm=14.7 psiap_{\text{atm}} = 14.7\text{ psia} and you plug in 0 psig0\text{ psig}, the computed NPSHA will be negative and completely wrong.
  • Trap 2 — Specific Gravity in Power vs. Head: A centrifugal pump with a given impeller at a fixed speed produces the exact same head in feet (or meters) regardless of liquid density. However, the Brake Horsepower (BHPBHP) scales directly with specific gravity (SGSG). Pumping brine (SG=1.2SG=1.2) requires 20% more motor power than pumping pure water.
Test Your Knowledge

A centrifugal pump running at 1750 rpm delivers 500 gpm against a total head of 120 ft, drawing 20 BHP. If a variable frequency drive (VFD) increases the rotational speed to 2100 rpm with no change in impeller diameter, what is the new flow rate, head, and required brake horsepower?

A

600 gpm, 144 ft, and 24.0 BHP

B

550 gpm, 160 ft, and 30.2 BHP

C

600 gpm, 172.8 ft, and 34.56 BHP

D

700 gpm, 200 ft, and 40.0 BHP

Test Your Knowledge

A boiler feedwater pump draws saturated liquid water from a deaerator tank operating at 100 kPa abs (p_0 = p_sat = 100 kPa, p_v = 100 kPa, gamma = 9.4 kN/m^3). The pump requires an NPSHR of 3.0 m. The suction piping head loss is h_fs = 0.8 m. What is the minimum required elevation (z_s) of the deaerator water surface above the pump centerline to maintain a safety margin of 1.2 m above NPSHR?

A

3.8 m

B

4.2 m

C

2.6 m

D

5.0 m

Test Your Knowledge

A single-stage centrifugal pump operating at 3500 rpm produces a head of 225 ft at its best efficiency point (BEP) with a flow rate of 900 gpm. What is the specific speed (N_s) in US Customary units and the corresponding impeller classification?

A

N_s = 1800 (Francis / Radial Vane)

B

N_s = 5200 (Mixed Flow)

C

N_s = 9800 (Axial Flow / Propeller)

D

N_s = 650 (Radial Impeller)

Test Your Knowledge

Two identical pumps are connected in parallel to discharge into a common manifold. Which of the following statements correctly describes the resulting system operating characteristics?

A

The shutoff head (head at zero flow) is doubled, while maximum flow remains constant

B

At any given head, the combined flow rate is the sum of the individual pump flow rates

C

The power required by each motor is halved while total discharge head is doubled

D

The operating point flow rate will exactly double for any arbitrary system head curve

Sections you finish are checked off in the contents.