UNIT 4: PUMPS, COMPRESSORS & POWER TRANSMISSION DEVICES
IV. PUMPS
Centrifugal Pumps
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Main Components:
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Impeller: Rotating disc with curved vanes.
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Casing: Volute (spiral) or diffuser type, converts kinetic energy to pressure.
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Suction & Delivery Pipes: With non-return valves.
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Working Principle: Centrifugal force throws fluid outward from impeller eye, creating low pressure at suction. Fluid gains kinetic energy in impeller, which is converted to pressure energy in the casing.
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Velocity Triangles:
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Inlet (Suction): Ideally radial flow ($$\displaystyle \alpha_1 = 90^\circ $$), $$\displaystyle u_1 = \frac{\pi D_1 N}{60} $$.
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Outlet (Discharge: $$\displaystyle u_2 = \frac{\pi D_2 N}{60} $$, $$\displaystyle V_{r2} $$ makes angle $$\displaystyle \beta_2 $$ with tangent.
[!TIP] Exam Focus: Often asked to draw velocity triangles for centrifugal pump. Key: $$\displaystyle V_w $$ (whirl velocity) at outlet is crucial for Euler's equation.
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Performance Characteristics:
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Head-Flow Curve: Head decreases with increase in flow rate.
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Efficiency-Flow Curve: Efficiency peaks at design flow rate (BEP - Best Efficiency Point).
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Power-Flow Curve: Power increases with flow rate.
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Advantages over Reciprocating Pumps:
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Smooth, continuous discharge (no pulsations).
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Higher capacity for same size.
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Lower maintenance, simpler construction.
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Can handle dirty/suspended fluids.
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Direct coupling to motor possible.
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Positive Displacement Pumps
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Types & Principle:
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Reciprocating: Piston/plunger moves in cylinder, creating suction/discharge via valves. Delivers pulsating flow at high pressure.
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Rotary (Gear, Vane, Lobe): Rotating element traps fluid and forces it from suction to discharge. Smoother than reciprocating.
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Characteristics:
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Flow rate nearly independent of head (positive displacement).
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High pressure generation capability.
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Self-priming generally.
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Pulsations require air chambers/smoothers.
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Pump Specific Speed ($$\displaystyle N_s $$)
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Definition: The speed of a geometrically similar pump that would deliver unit flow rate (1 m³/s) against unit head (1 m) when operating at its maximum efficiency.
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Derivation (from similarity laws):
$$N_s = \frac{N \sqrt{Q}}{H^{3/4}}$$
Where, $N$ = RPM, $Q$ = Discharge (m³/s), $H$ = Head (m).
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Significance:
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Low $$\displaystyle N_s $$ (< 500): Radial flow pumps (Centrifugal).
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Medium $$\displaystyle N_s $$ (500-5000): Mixed flow pumps.
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High $$\displaystyle N_s $$ (> 5000): Axial flow pumps.
\boxed{N_s = \frac{N \sqrt{Q}}{H^{3/4}} \quad \text{(SI Units)}}
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V. COMPRESSORS
Centrifugal Compressors
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Construction: High-speed rotating impeller, diffuser vanes (or volute), multi-stage possible.
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Velocity Diagram:
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Inlet: Usually axial ($$\displaystyle \alpha_1 \approx 0^\circ $$).
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Outlet: High radial component, $$\displaystyle u_2 $$ is high.
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Key Parameter: Slip Factor ($\sigma$) accounts for deviation of $$\displaystyle V_{w2} $$ from ideal due to boundary layer and curvature. $$\displaystyle \sigma = \frac{V_{w2 \text{ actual}}}{V_{w2 \text{ ideal}}} $$.
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Work Done (per kg, for one stage):
$$\Delta h_0 = \sigma u_2 V_{w2} \quad \text{(or } u_2 V_{w2} \text{ ideal)}$$
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Pressure Rise: $$\displaystyle \Delta P = \rho \Delta h_0 $$ (isentropic assumption).
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Performance: High flow rate, moderate pressure rise per stage. Efficiency drops at off-design.
Axial Flow Compressors
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Construction: Alternating rows of rotating (rotor) and stationary (stator) blades. Many stages for high pressure ratio.
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Velocity Diagram: Similar triangles for each stage. Degree of Reaction ($R$) is key.
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Degree of Reaction:
$$R = \frac{\text{Static enthalpy rise in rotor}}{\text{Total static enthalpy rise in stage}}$$
For 50% reaction (Parsons turbine/compressor), $$\displaystyle \alpha_1 = \beta_2 $$, $$\displaystyle \beta_1 = \alpha_2 $$, and blade angles symmetrical.
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Multi-stage: Overall pressure ratio = product of individual stage pressure ratios. Reheat factor improves efficiency.
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Comparison with Centrifugal:
| Feature | Centrifugal Compressor | Axial Flow Compressor | | :--- | :--- | :--- | | Flow Path | Radial | Axial | | Pressure Ratio/Stage | High (3:1 to 5:1) | Low (1.1:1 to 1.4:1) | | Flow Capacity | Lower | Higher | | Efficiency | Moderate | High (at design) | | Size/Weight | Compact for low flow | Larger, slender for high flow | | Application | Gas turbines, small plants | Large gas turbines, aircraft engines |
Compressor Efficiencies
- Isentropic Efficiency ($$\displaystyle \eta_s $$):
$$\eta_s = \frac{\text{Ideal isentropic work input}}{\text{Actual work input}} = \frac{h_{02s} - h_{01}}{h_{02} - h_{01}}$$
Most common, but depends on pressure ratio.
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Polytropic Efficiency ($$\displaystyle \eta_p $$):
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Definition: Efficiency of an infinitesimal stage. Constant for a given compressor over its operating range.
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Advantage: True measure of aerodynamic quality, independent of pressure ratio.
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Calculation:
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$$\eta_p = \frac{n-1}{n} \cdot \frac{\gamma-1}{\gamma} \quad \text{for ideal gas}$$
Where $n$ = polytropic index, $\gamma$ = specific heat ratio.
> \boxed{\eta_p = \frac{\text{Incremental isentropic work}}{\text{Incremental actual work}}}
Operating Limits and Instabilities
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Surging:
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Definition: Complete breakdown of steady flow through the compressor, causing large-amplitude flow reversal and vibration. Occurs at low flow rates.
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Cause: Flow separation on stator/rotor blades at high incidence angles, leading to stall and flow reversal.
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Characteristics: Sharp drop in pressure, flow reversal, violent oscillations. Surge line on compressor map (left boundary).
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Control: Avoid operation left of surge line, use variable stators, bleed valves.
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Choking:
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Definition: Sonic velocity reached at the smallest flow area (throat). Mass flow rate becomes maximum and constant for given speed, regardless of downstream pressure.
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Effect: Limits maximum mass flow at high speeds. Right boundary on compressor map.
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Stall vs Surge:
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Stall: Localized flow separation on a blade row (rotating stall). Can lead to surge.
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Surge: System instability involving the entire compressor and ducting.
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VI. POWER TRANSMISSION DEVICES
Fluid Coupling
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Construction: Impeller (pump) and Runner (turbine) in a casing, filled with oil. No mechanical link.
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Working Principle: Impeller driven by motor imparts kinetic energy to oil. Oil strikes runner blades, transferring momentum and torque. Slip exists ($$\displaystyle \omega_t < \omega_p $$).
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Slip & Efficiency:
$$\text{Slip} = \frac{\omega_p - \omega_t}{\omega_p}$$
$$\eta = \frac{\omega_t}{\omega_p} \quad \text{(for equal diameters)}$$
> \boxed{\eta = \frac{2}{1 + \frac{u_t}{u_p}} \quad \text{(if } u_t/u_p \text{ is slip ratio)}}
- Applications: Soft start, overload protection, vibration damping in conveyors, crushers, pumps.
Torque Converter
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Construction: Impeller (pump), Turbine, Stator (redirects flow). Three elements.
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Working Principle: Oil circulates in a loop. Stator redirects oil to turbine, providing torque multiplication at low turbine speed (high slip).
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Performance:
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Torque Ratio ($$\displaystyle T_{t}/T_{p} $$): >1 at low speed ratio.
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Efficiency: Low at high multiplication, peaks at speed ratio ~0.6-0.7.
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Applications: Automatic transmissions, marine propulsion, heavy machinery.
Hydraulic Intensifier
- Principle: Pressure Multiplication using two pistons of different diameters in a single cylinder.
$$P_1 A_1 = P_2 A_2 \quad \Rightarrow \quad P_2 = P_1 \frac{A_2}{A_1}$$
Small piston area $$\displaystyle A_1 $$ receives low pressure $$\displaystyle P_1 $$, large piston area $$\displaystyle A_2 $$ delivers high pressure $$\displaystyle P_2 $$.
- Applications: Hydraulic presses, test rigs, systems requiring high pressure from a low-pressure source.
Centrifugal Blowers
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Working: Similar to centrifugal compressor but for low pressure rise (typically < 0.5 bar). Often with forward-curved blades.
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Applications: Ventilation, dust collection, drying, combustion air supply.
Hydraulic Press
- Principle: Pascal's Law - Pressure transmitted undiminished in confined fluid.
$$F_1/A_1 = F_2/A_2 \quad \Rightarrow \quad F_2 = F_1 \frac{A_2}{A_1}$$
- Force Multiplication: Small force $$\displaystyle F_1 $$ on small plunger area $$\displaystyle A_1 $$ generates large force $$\displaystyle F_2 $$ on large ram area $$\displaystyle A_2 $$.
Draft Tube (Reaction Turbines - Francis, Kaplan)
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Function: Converts kinetic energy at turbine runner exit to pressure energy, increasing net head. Allows setting turbine above tailrace (regains static head).
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Types:
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Conical: Simple, efficient.
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Elbow: For horizontal shaft turbines, space-saving.
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Simple Tapered: Straight divergent tube.
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Design: Gradually expanding area to decelerate flow with minimal losses. Pressure recovery coefficient is key.
VIII. ADDITIONAL TOPICS (Relevant to UNIT 4)
Polytropic Efficiency of Compressors (Detailed)
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Why Polytropic? Isentropic efficiency varies with pressure ratio. Polytropic efficiency is constant for a given compressor design, representing true aerodynamic blade efficiency.
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Relation to Isentropic:
$$\eta_s = \frac{(r_p)^{(\gamma-1)/\gamma} - 1}{(r_p)^{(n-1)/n} - 1}$$
Where $$\displaystyle r_p $$ = pressure ratio, $n$ = polytropic index.
- For Multi-stage: Overall $$\displaystyle \eta_s $$ can be calculated from stage $$\displaystyle \eta_p $$:
$$\eta_s = \frac{r_p^{(\gamma-1)/\gamma} - 1}{r_p^{(n-1)/n} - 1} \quad \text{with } \frac{n-1}{n} = \frac{\gamma-1}{\gamma} \ln \eta_p$$
Vector Diagram of Centrifugal Compressor
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Inlet: $$\displaystyle V_1 \approx u_1 $$ (radial), $$\displaystyle \alpha_1 \approx 90^\circ $$.
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Outlet: $$\displaystyle u_2 $$ (tangential), $$\displaystyle V_{r2} $$ at angle $$\displaystyle \beta_2 $$ (vane angle), $$\displaystyle V_2 = u_2 - V_{w2} $$ (vector subtraction).
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Slip: $$\displaystyle V_{w2 \text{ actual}} = \sigma u_2 - V_{r2} \cos \beta_2 $$.
DiagramSEARCH: centrifugal compressor velocity diagram
Vector Diagram of Axial Flow Compressor
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Constant Mean Diameter: $$\displaystyle u_1 = u_2 = u $$.
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Symmetrical 50% Reaction Stage: $$\displaystyle \alpha_1 = \beta_2 $$, $$\displaystyle \beta_1 = \alpha_2 $$.
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Rotor: Changes $$\displaystyle \alpha_1 $$ to $$\displaystyle \beta_1 $$ (adds energy).
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Stator: Changes $$\displaystyle \beta_2 $$ to $$\displaystyle \alpha_2 $$ (redirects flow, no work).
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Work Input: $$\displaystyle \Delta h_0 = u (V_{w2} - V_{w1}) $$.
DiagramSEARCH: axial flow compressor velocity diagram stage
Surging and Efficiency of Axial Flow Compressor
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Surge occurs at low mass flow, high incidence → separation → efficiency drops sharply.
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Choking occurs at high mass flow, sonic at throat → flow max, efficiency may still be moderate.
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Efficiency Map: Peak efficiency near design point. Efficiency falls rapidly as surge line is approached from right.
Short Notes
Centrifugal Blower:
A low-pressure, high-volume flow device. Uses centrifugal impeller (often forward-curved blades) to move air against moderate resistance. Simple, compact, used in HVAC, drying, combustion air.
Hydraulic Intensifier:
Pressure multiplication device. Two pistons of different diameters in common cylinder. $$\displaystyle P_2 = P_1 (A_2/A_1) $$. Converts large volume/low pressure to small volume/high pressure. Used in hydraulic presses where system pressure is low.
Draft Tube:
Diffuser at exit of reaction turbine runner. Converts kinetic energy to pressure, recovers static head. Allows turbine placement above tailrace. Types: Conical (most efficient), Elbow (for horizontal shafts), Simple Tapered. Design goal: minimize kinetic energy loss at exit.
Applications of Power Transmitting Devices:
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Fluid Coupling: Soft starters for conveyors, mills, pumps; vibration isolation.
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Torque Converter: Automatic transmissions (cars, earthmovers), marine propulsion.
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Hydraulic Intensifier: High-pressure testing, hydraulic presses with low-pressure source.
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Centrifugal Blowers: Industrial ventilation, dust collection, drying ovens, boiler forced draft.
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Hydraulic Press: Metal forming, molding, assembly (press fits), scrap processing.
KEY FORMULAS FOR UNIT 4
| Concept | Formula |
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| Pump Specific Speed | $$\displaystyle N_s = \frac{N \sqrt{Q}}{H^{3/4}} $$ |
| Polytropic Efficiency | $$\displaystyle \eta_p = \frac{n-1}{n} \cdot \frac{\gamma-1}{\gamma} $$ |
| Hydraulic Press Force | $$\displaystyle F_2 = F_1 \frac{A_2}{A_1} $$ |
| Hydraulic Intensifier Pressure | $$\displaystyle P_2 = P_1 \frac{A_2}{A_1} $$ |
| Fluid Coupling Efficiency | $$\displaystyle \eta = \frac{\omega_t}{\omega_p} $$ |
| Euler's Equation (Pump/Compressor) | $$\displaystyle \Delta h_0 = u_2 V_{w2} - u_1 V_{w1} $$ |
| Degree of Reaction | $$\displaystyle R = \frac{\text{Enthalpy drop in rotor}}{\text{Total enthalpy drop in stage}} $$ |
[!TIP] Exam Strategy: For numerical problems (Pelton, centrifugal pump, compressor stages), always start with a clear velocity diagram. Label $u$, $V$, $$\displaystyle V_w $$, $$\displaystyle V_r $$, $\alpha$, $\beta$. Apply Euler's equation $$\displaystyle \Delta h_0 = u V_w $$ (often $$\displaystyle u_1 V_{w1} \approx 0 $$). Calculate forces ($$\displaystyle F = \dot{m} \Delta V_w $$), power ($$\displaystyle P = \dot{m} \Delta h_0 $$), and efficiency ($$\displaystyle \eta = \frac{\text{Useful output}}{\text{Input}} $$). For specific speed, ensure units are consistent (SI: $N$ in RPM, $Q$ in m³/s, $H$ in m).