Pump CFD Analysis

Category: Fluid Analysis (CFD) | Integrated 2026-04-06
CAE visualization for mixed flow pump cfd theory - technical simulation diagram
Pump CFD Analysis โ€” Fundamental Theory of Head and Efficiency

Pump CFD: Theoretical Foundations

Overview

๐Ÿง‘โ€๐ŸŽ“

What does CFD analysis of a centrifugal pump predict?


๐ŸŽ“

The three basics are Head, Efficiency, and Shaft Power. Creating the H-Q characteristic curve is the main purpose of CFD.


Definition of Head and Efficiency

๐Ÿง‘โ€๐ŸŽ“

Please tell me the head equation.


๐ŸŽ“

The pump head is the difference in total head between the inlet and outlet.


$$ H = \frac{p_2 - p_1}{\rho g} + \frac{V_2^2 - V_1^2}{2g} + (z_2 - z_1) $$

In CFD, it's convenient to calculate directly from the total pressure difference. $H = (p_{t2} - p_{t1})/(\rho g)$.


Efficiency is divided into hydraulic efficiency and overall efficiency.


$$ \eta = \frac{\rho g Q H}{P_{shaft}} = \frac{\rho g Q H}{\tau \omega} $$

$\tau$ is the impeller torque obtained from CFD, and $\omega$ is the angular velocity.


๐Ÿง‘โ€๐ŸŽ“

What's the difference between hydraulic efficiency and overall efficiency?


๐ŸŽ“

Hydraulic efficiency includes only hydrodynamic losses, excluding disc friction and leakage. Overall efficiency includes all: disc friction, leakage flow, and mechanical losses. What CFD directly yields is hydraulic efficiency; disc friction and leakage won't appear unless a gap model with the wear ring is included.


Euler Head (Theoretical Head)

๐Ÿง‘โ€๐ŸŽ“

The theoretical head can be derived from the Euler equation, right?


๐ŸŽ“
$$ H_{Euler} = \frac{U_2 C_{\theta 2} - U_1 C_{\theta 1}}{g} $$

Assuming no swirl at the inlet for a centrifugal pump ($C_{\theta 1}=0$), it becomes $H_{Euler} = U_2 C_{\theta 2}/g$. The head considering the slip factor $\sigma_s$ is $H_{th} = \sigma_s \cdot H_{Euler}$. The CFD head corresponds to this theoretical head plus hydraulic losses.


Steady-State Analysis with MRF Method

๐Ÿง‘โ€๐ŸŽ“

Is the MRF method common for pump CFD?


๐ŸŽ“

For obtaining the H-Q curve, the MRF method (steady-state) is standard. For cases with a volute, Frozen Rotor or Sliding Mesh is used. For a guide vane pump without a volute, Mixing Plane can also be used.

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Specific Speed as a Compass โ€“ The Starting Point of Mixed-Flow Pump Design

The first step in turbo pump design is calculating the Specific Speed (Ns). This dimensionless number, defined by Ns = nโˆšQ / H^(3/4) (n: rotational speed, Q: flow rate, H: head), determines the pump type (centrifugal, mixed-flow, axial). In the design domain for mixed-flow pumps (Ns = 400โ€“1200), the standard two-step approach is theoretically to determine basic dimensions with 1D design (velocity triangles) and then verify 3D flow details with CFD. The theory of specific speed was systematized by American hydraulic engineers in the early 20th century, followed by confusion with different unit systems in Europe and Japan. Today, the IEC standard has internationalized the dimensionless specific speed in mยณ/s and m units.

Computational Methods for Pump CFD

Mesh Generation

๐Ÿง‘โ€๐ŸŽ“

What should I be careful about with centrifugal pump meshing?


๐ŸŽ“

For the impeller, generating a structured grid with TurboGrid yields the highest quality. For the volute, use an unstructured tetra/polyhedral mesh.


RegionMesh TypeApprox. Cell CountTool
ImpellerStructured Grid (H/J/L+O-grid)0.5โ€“1.5 million/pitchTurboGrid
VoluteUnstructured Tetra+Prism1โ€“3 millionFluent Meshing, STAR-CCM+
Suction PipeStructured or Unstructured0.2โ€“0.5 millionAny
Wear Ring GapStructured (Hexahedral)0.1โ€“0.3 millionManual
๐Ÿง‘โ€๐ŸŽ“

Should the wear ring gap also be included in the model?


๐ŸŽ“

It's essential if you want to evaluate the effect of leakage flow. The gap is very narrow, 0.2โ€“0.5mm, so a minimum of 10 cells radially and 50 cells axially is recommended.


Turbulence Model Selection

๐Ÿง‘โ€๐ŸŽ“

Which turbulence model is suitable for pumps?


๐ŸŽ“

SST k-omega is the standard. It excels at predicting adverse pressure gradients and separation on blade surfaces. For pumps, since the number of blades is small (5โ€“7) and blade loading is high, k-epsilon tends to underpredict separation.


๐Ÿง‘โ€๐ŸŽ“

Should I use wall functions or Low-Re?


๐ŸŽ“

Pump Re is on the order of $10^6$, sufficiently high, so wall functions with y+ = 30โ€“100 generally yield reasonable results. However, for higher accuracy, the Low-Re solution with y+ < 2 is recommended. Particularly for predicting blade surface separation at partial load, wall functions have limitations.


Boundary Conditions

๐Ÿง‘โ€๐ŸŽ“

What are typical pump boundary conditions?


๐ŸŽ“
  • Inlet: Mass flow rate specified (varied from 0.2 to 1.4 times design flow rate)
  • Outlet: Static pressure specified (atmospheric or actual system pressure)
  • Blade surface, Hub, Shroud: No-slip wall
  • Impeller-Volute interface: Frozen Rotor or Sliding Mesh

Setting the outlet to fixed static pressure and varying the inlet flow rate is the most stable configuration.

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Between Axial and Centrifugal โ€“ Numerical Difficulties in Mixed-Flow Pump CFD

Mixed-flow pumps lie in the intermediate specific speed (Ns) range between axial and centrifugal pumps (Ns = 400โ€“1200), and because flow mechanisms from both types coexist, numerical analysis is difficult. The axial flow component is dominated by tip vortices and secondary flows, while the centrifugal component is affected by flow curvature due to Coriolis forces. In this mixed region, turbulence model selection directly impacts pump efficiency prediction, and many comparative studies show the k-ฯ‰ SST model is typically several percent more accurate than standard k-ฮต. In mesh design, balancing resolution in the axial, circumferential, and radial directions is important; making one direction finer is not necessarily better.

Pump CFD in Practice

H-Q Characteristic Calculation Procedure

๐Ÿง‘โ€๐ŸŽ“

How do you create the H-Q characteristic curve?


๐ŸŽ“

1. Converge a steady-state MRF (or Frozen Rotor) calculation at design flow rate $Q_d$

2. Set 7โ€“10 points in the flow rate range $0.2Q_d$ to $1.4Q_d$

3. Recalculate at each point by changing the inlet mass flow rate (using the previous point's result as the restart value)

4. Calculate head H, torque ฯ„, efficiency ฮท at each point and plot


๐Ÿง‘โ€๐ŸŽ“

Why does convergence worsen on the low flow rate side?


๐ŸŽ“

At low flow rates, the incidence angle at the impeller inlet becomes large, causing large-scale separation on the blade surface. In steady-state calculations, trying to converge an unsteady separation structure into a single solution causes oscillations. Below about 0.3$Q_d$, unsteady calculations are often necessary.


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