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12.3 Fluid Power Systems: Hydraulics & Pneumatics

Key Takeaways

  • Pascal's law dictates that static fluid pressure in a confined liquid transmits undiminished in all directions, enabling force multiplication proportional to actuator piston area (F=P⋅AF = P \cdot A).

  • Fluid compressibility is governed by bulk modulus β=−V(ΔP/ΔV)\beta = -V (\Delta P / \Delta V); entrained air drastically degrades effective bulk modulus, causing spongy actuator response and pressure spikes.

  • Total pump efficiency is the product of volumetric and mechanical efficiencies (ηo=ηv⋅ηm\eta_o = \eta_v \cdot \eta_m), where volumetric efficiency quantifies internal slippage and mechanical efficiency accounts for fluid shear and bearing friction.

  • Differential area in double-acting cylinders causes asymmetric extension and retraction: extension produces higher force (F=PApF = P A_p) at lower speed, whereas retraction delivers lower pull force (F=P[Ap−Arod]F = P [A_p - A_{rod}]) at higher speed for a given pump flow rate.

  • In hydraulic power sizing, hydraulic horsepower is calculated via hp=(Ppsi⋅Qgpm)/1714hp = (P_{\text{psi}} \cdot Q_{\text{gpm}}) / 1714 in USCS units and P=(Pbar⋅QL/min)/600P = (P_{\text{bar}} \cdot Q_{\text{L/min}}) / 600 in kilowatts for metric systems.

Last updated: October 2026

12.3 Fluid Power Systems: Hydraulics & Pneumatics

Fluid power transmits and controls mechanical energy using pressurized liquids (hydraulics) or compressed gases (pneumatics). Hydraulic systems deliver exceptional power density and rigid position holding at pressures exceeding 350 bar350\,\text{bar} (5, ⁣000 psi5,\!000\,\text{psi}), while pneumatic systems provide clean, high-speed, compliant actuation at lower pressures (6−10 bar6 - 10\,\text{bar} or 90−150 psi90 - 150\,\text{psi}). Mastering fluid power principles, actuator kinematics, valve selection, and power sizing calculations is fundamental to machine design.


Principles of Fluid Power

Pascal's Law & Force Multiplication

Pascal's law states that pressure applied to an enclosed, static fluid is transmitted undiminished in all directions and acts with equal force on equal areas perpendicular to the container walls.

P=F1A1=F2A2  ⟹  F2=F1(A2A1)P = \frac{F_1}{A_1} = \frac{F_2}{A_2} \implies F_2 = F_1 \left(\frac{A_2}{A_1}\right)
                      Pascal's Hydraulic Leverage
       Input Force F_1                                  Output Force F_2
             |                                                 |
             v                                                 v
       +-----------+                                   +---------------+
       | Piston A_1|                                   |  Piston A_2   |
       +-----+-----+                                   +-------+-------+
             |               Confined Hydraulic Fluid          |
             +=================================================+
                               Pressure P (Uniform)

By conservation of energy (assuming an incompressible, frictionless fluid), the work input equals work output:

W=F1s1=F2s2  ⟹  s2=s1(A1A2)W = F_1 s_1 = F_2 s_2 \implies s_2 = s_1 \left(\frac{A_1}{A_2}\right)

Force multiplication is balanced by a proportional reduction in displacement stroke.

Hydraulic Fluids & Physical Properties

  1. Fluid Types:

    • Mineral Oil-Based (Petroleum): Most widely used (ISO VG 32, 46, 68). Provides excellent lubricity, anti-wear properties, and corrosion protection.
    • Fire-Resistant Fluids: Water-glycol solutions (HFC), synthetic polyol esters (HFDU), and phosphate esters (HFDR), specified for die casting, steel mills, and aviation.
  2. Bulk Modulus (β\beta) & Compressibility: The Bulk Modulus of Elasticity quantifies a fluid's resistance to uniform volume compression under pressure:

β=−V0ΔPΔV=−ΔPΔV/V0\beta = -V_0 \frac{\Delta P}{\Delta V} = -\frac{\Delta P}{\Delta V / V_0}

For pure petroleum hydraulic oil, β≈1.4−1.8 GPa\beta \approx 1.4 - 1.8\,\text{GPa} (200, ⁣000−260, ⁣000 psi200,\!000 - 260,\!000\,\text{psi}). While considered incompressible for static calculations, high-pressure dynamic systems experience noticeable fluid deflection:

ΔV=−V0ΔPβ\Delta V = -V_0 \frac{\Delta P}{\beta}

Warning

Entrained air bubbles drastically reduce the effective bulk modulus. Even 1%1\% entrained air by volume can slash the effective bulk modulus by over 50%50\%, causing severe actuator sponginess, loss of control stiffness, pump cavitation, and destructive pressure spikes (hydraulic water hammer).

  1. Viscosity & Viscosity Index (VI):
    • Kinematic Viscosity (measured in cSt\text{cSt} or mm2/s\text{mm}^2/\text{s}) determines fluid film thickness, lubricity, and laminar/turbulent pipe friction losses.
    • Viscosity Index (VI): An empirical dimensionless scale indicating how viscosity changes with temperature. A high VI rating indicates that fluid viscosity remains relatively stable across temperature swings.

Positive Displacement Pumps & Hydraulic Motors

Hydraulic pumps do not create pressure; they generate fluid flow (QQ). Pressure arises strictly from resistance to fluid flow imposed by the load, piping restrictions, and relief valves.

Pump Classifications

  • External Gear Pumps: Fixed displacement, inexpensive, compact, tolerant of contamination; pressures up to 250 bar250\,\text{bar}.
  • Vane Pumps: Fixed or variable displacement, low noise, balanced radial loading; pressures up to 200 bar200\,\text{bar}.
  • Piston Pumps (Axial & Radial): Swashplate or bent-axis configurations; variable displacement capability with pressure compensation; high pressures up to 420 bar420\,\text{bar} (6, ⁣000 psi6,\!000\,\text{psi}); high volumetric efficiency.

Pump Efficiencies & Sizing

For a pump with volumetric displacement VDV_D (volume displaced per shaft revolution) rotating at speed nn:

  1. Theoretical Flow Rate (QtQ_t):
Qt=VD⋅nQ_t = V_D \cdot n
  1. Volumetric Efficiency (ηv\eta_v): Accounts for internal fluid leakage (slip) from the high-pressure discharge port back to the suction inlet:
ηv=QactQt=QactVD⋅n(typically 0.88−0.98)\eta_v = \frac{Q_{\text{act}}}{Q_t} = \frac{Q_{\text{act}}}{V_D \cdot n} \qquad (\text{typically } 0.88 - 0.98)
  1. Mechanical / Hydromechanical Efficiency (ηm\eta_m): Accounts for torque losses from bearing friction, seal drag, and fluid viscous shear:
ηm=TtTact=VD⋅ΔP/(2π)Tact(typically 0.85−0.95)\eta_m = \frac{T_t}{T_{\text{act}}} = \frac{V_D \cdot \Delta P / (2\pi)}{T_{\text{act}}} \qquad (\text{typically } 0.85 - 0.95)
  1. Overall Efficiency (ηo\eta_o): The product of volumetric and mechanical efficiencies:
ηo=ηv⋅ηm=Hydraulic Power OutputMechanical Shaft Power Input=Qact⋅ΔPTact⋅ω\eta_o = \eta_v \cdot \eta_m = \frac{\text{Hydraulic Power Output}}{\text{Mechanical Shaft Power Input}} = \frac{Q_{\text{act}} \cdot \Delta P}{T_{\text{act}} \cdot \omega}

Hydraulic Motors

Hydraulic motors convert pressurized fluid flow back into rotary mechanical torque and rotation. Motor relationships invert pump equations:

Tact=Tt⋅ηm=(VD⋅ΔP2π)ηmT_{\text{act}} = T_t \cdot \eta_m = \left(\frac{V_D \cdot \Delta P}{2\pi}\right) \eta_m Qact=Qtηv=VD⋅nηvQ_{\text{act}} = \frac{Q_t}{\eta_v} = \frac{V_D \cdot n}{\eta_v}

Hydraulic Cylinders (Linear Actuators)

Hydraulic cylinders convert fluid power into linear thrust and motion. Most industrial applications use double-acting cylinders with a single rod end.

                  Double-Acting Hydraulic Cylinder Geometry
            +--------------------------------------------+
            |           Piston Area (A_p)                |
       Cap  |      +=========+                           | Rod End
       Port |----->|         |======[ Rod: d_r ]========>| Port
       (P_1)|      | Piston  |   Annular Area (A_r)      | (P_2)
            |      +=========+                           |
            +--------------------------------------------+
                   <--------- Stroke S --------->

Geometry & Effective Areas

  • Bore Diameter (DpD_p) and Piston Area (ApA_p):
Ap=π4Dp2A_p = \frac{\pi}{4} D_p^2
  • Rod Diameter (drd_r) and Rod Area (ArodA_{\text{rod}}):
Arod=π4dr2A_{\text{rod}} = \frac{\pi}{4} d_r^2
  • Annular Area (Retraction Area ArA_r):
Ar=Ap−Arod=π4(Dp2−dr2)A_r = A_p - A_{\text{rod}} = \frac{\pi}{4} \left(D_p^2 - d_r^2\right)

Extension vs. Retraction Force & Speed

Assuming supply pressure PP and pump delivery flow rate QQ:

Operational ParameterExtension Stroke (Cap End Pressurized)Retraction Stroke (Rod End Pressurized)
Effective Working AreaApA_pAr=Ap−ArodA_r = A_p - A_{\text{rod}}
Theoretical Thrust ForceFext=P⋅ApF_{\text{ext}} = P \cdot A_pFret=P⋅Ar=P(Ap−Arod)F_{\text{ret}} = P \cdot A_r = P \left(A_p - A_{\text{rod}}\right)
Velocity (vv)vext=QApv_{\text{ext}} = \frac{Q}{A_p}vret=QAr=QAp−Arodv_{\text{ret}} = \frac{Q}{A_r} = \frac{Q}{A_p - A_{\text{rod}}}
Kinematic RelationshipLower velocity (vext<vretv_{\text{ext}} < v_{\text{ret}})Higher velocity (vret>vextv_{\text{ret}} > v_{\text{ext}})
Dynamic Force OutputHigher force (Fext>FretF_{\text{ext}} > F_{\text{ret}})Lower force (Fret<FextF_{\text{ret}} < F_{\text{ext}})

Regenerative Circuit Operation

In rapid-advance tooling cycles, a directional valve connects the rod end discharge directly back into the cap end inlet. The net extending area equals the rod area ArodA_{\text{rod}}:

vregen=QArod,Fregen=P⋅Arodv_{\text{regen}} = \frac{Q}{A_{\text{rod}}}, \qquad F_{\text{regen}} = P \cdot A_{\text{rod}}

This delivers high extension speed at reduced thrust.

Cylinder End-Position Cushioning

High-speed cylinders contain tapered cushioning spears at stroke ends. As the piston approaches the end cap, the spear restricts fluid exit into a small cavity, forcing discharge fluid through an adjustable needle orifice. A parallel check valve allows unrestricted flow during reverse stroke start-up.


Hydraulic Circuit Control Valves

                             Hydraulic Valve Functions
         +-------------------------------------------------------------+
         | Pressure Control    | Directional Control  | Flow Control   |
         |---------------------+----------------------+----------------|
         | Relief Valves       | 4/3-Way Spool Valves | Meter-In       |
         | Reducing Valves     | Check / Pilot Check  | Meter-Out      |
         | Sequence / CB Valves| Poppet Cartridges    | Bleed-Off      |
         +-------------------------------------------------------------+

1. Pressure Control Valves

  • Pressure Relief Valve (PRV): Sets the maximum system pressure and protects hardware against overload.
    • Direct-Acting PRV: Simple spring-loaded poppet; fast response (<10 ms< 10\,\text{ms}); subject to pressure override (pressure rises noticeably above cracking pressure as flow increases).
    • Pilot-Operated PRV: Two-stage design (pilot poppet and balanced main spool); nearly flat P−QP-Q curve across full flow; ideal for high-flow industrial systems.
  • Pressure Reducing Valve: Normally open valve that regulates down to a constant, lower secondary pressure in a sub-circuit.
  • Counterbalance Valve: Maintains back-pressure on a vertical or overrunning load to prevent uncontrolled gravitational descent.

2. Directional Control Valves (DCV)

Designated by Ports / Positions (e.g., 4/3-way valve = 4 ports, 3 spool positions).

Common 3-position neutral center spool configurations:

  • Closed Center: All ports (P,T,A,BP, T, A, B) blocked. Used with variable-displacement pressure-compensated pumps; holds cylinder in position while maintaining system pressure.
  • Open Center: All ports (P,T,A,BP, T, A, B) connected to tank (TT). Unloads the pump to tank at low pressure, but actuator floats freely.
  • Tandem Center: Pump (PP) connects to Tank (TT) while actuator ports (A,BA, B) are blocked. Unloads fixed-displacement pumps while hydraulically locking the cylinder in position.
  • Float Center: Pump (PP) blocked; actuator ports (A,BA, B) connect to tank (TT). Allows actuator to float or freewheel under external mechanical forces.

3. Flow Control Circuit Strategies

   Meter-In (Restrict Inlet)       Meter-Out (Restrict Return)       Bleed-Off (Bypass to Tank)
          [Pump]                            [Pump]                           [Pump]--[FCV]-->[Tank]
            |                                 |                                 |
          [FCV] (Controls Flow)               +---------> [Cylinder]            +------> [Cylinder]
            |                                 |               |
            v                                 v             [FCV] (Controls Return)
       [Cylinder]                         [Cylinder]          |
            |                                 |               v
         [Tank]                            [Tank]          [Tank]
  1. Meter-In Circuit: Flow control valve installed in the supply line to the actuator. Controls speed against positive (opposing) loads. Risk: Overrunning loads can pull the cylinder forward, inducing cavitation.
  2. Meter-Out Circuit: Flow control valve installed in the discharge line from the actuator. Creates back-pressure on the return fluid. Advantage: Prevents actuator lunging and runaway under overrunning or negative gravitational loads.
  3. Bleed-Off Circuit: Flow control valve installed in a branch tee line, diverting excess pump delivery directly to tank. Operates only at the actual load pressure rather than maximum relief pressure, significantly reducing heat generation. However, cylinder speed varies if the mechanical load fluctuates.

Hydraulic Power Calculations

Hydraulic power is the product of pressure drop and volumetric flow rate:

Phyd=ΔP⋅QP_{\text{hyd}} = \Delta P \cdot Q

Practical Unit Formulations

SI Metric Units

In SI base units:

Power (W)=P (Pa)×Q (m3/s)\text{Power}\,(\text{W}) = P\,(\text{Pa}) \times Q\,(\text{m}^3/\text{s})

In standard industrial plant units (pressure PP in bar\text{bar}, flow rate QQ in L/min\text{L/min}):

Phyd (kW)=P (bar)×Q (L/min)600P_{\text{hyd}}\,(\text{kW}) = \frac{P\,(\text{bar}) \times Q\,(\text{L/min})}{600}

(Derivation: 1 bar=105 N/m21\,\text{bar} = 10^5\,\text{N/m}^2, 1 L/min=10−360 m3/s1\,\text{L/min} = \frac{10^{-3}}{60}\,\text{m}^3/\text{s}; product=10060 W=1600 kW\text{product} = \frac{100}{60}\,\text{W} = \frac{1}{600}\,\text{kW}.)

USCS Engineering Units

With pressure PP in pounds per square inch (psi\text{psi}) and flow rate QQ in gallons per minute (gpm\text{gpm}):

Horsepower (hp)=P (psi)×Q (gpm)1714\text{Horsepower}\,(\text{hp}) = \frac{P\,(\text{psi}) \times Q\,(\text{gpm})}{1714}

(Derivation: 1 gpm=231 in3/min1\,\text{gpm} = 231\,\text{in}^3/\text{min}, 1 hp=33, ⁣000 ft⋅lbf/min=396, ⁣000 in⋅lbf/min1\,\text{hp} = 33,\!000\,\text{ft}\cdot\text{lbf/min} = 396,\!000\,\text{in}\cdot\text{lbf/min}. Constant =396, ⁣000/231=1714.28≈1714= 396,\!000 / 231 = 1714.28 \approx 1714.)

Electric Drive Motor Sizing

Pelec=PhydηoP_{\text{elec}} = \frac{P_{\text{hyd}}}{\eta_o}

where ηo\eta_o is the overall pump efficiency.


Pneumatics & Compressed Air Systems

Pneumatic systems use atmospheric air compressed typically to 6−10 bar6 - 10\,\text{bar} (90−145 psig90 - 145\,\text{psig}).

Compressibility & Gas Laws

Air obeys the Ideal Gas Law over normal industrial operating ranges:

PV=mRTP V = m R T

where Rair=287 J/(kg⋅K)=53.35 ft⋅lbf/(lbm⋅∘R)R_{\text{air}} = 287\,\text{J}/(\text{kg}\cdot\text{K}) = 53.35\,\text{ft}\cdot\text{lbf}/(\text{lbm}\cdot^\circ\text{R}). Absolute pressures and temperatures must be used (Pabs=Pgage+PatmP_{\text{abs}} = P_{\text{gage}} + P_{\text{atm}}; T (K)=∘C+273.15T\,(\text{K}) = ^\circ\text{C} + 273.15; T (∘R)=∘F+459.67T\,(^\circ\text{R}) = ^\circ\text{F} + 459.67).

For compression processes:

  • Isothermal (P1V1=P2V2P_1 V_1 = P_2 V_2): Slow compression with full heat dissipation.
  • Polytropic / Adiabatic (P1V1k=P2V2kP_1 V_1^k = P_2 V_2^k, with k=1.4k = 1.4 for air): Fast compression where temperature rises significantly.

Standard Flow (SCFM) and Free Air Delivery

Compressed-air flow is usually converted to Standard Cubic Feet per Minute (SCFM) at a stated reference condition. Reference conditions differ between organizations (ASME uses 14.7 psia14.7\,\text{psia}, 68∘F68^\circ\text{F} and 36%36\% relative humidity; CAGI uses 14.5 psia14.5\,\text{psia}, 68∘F68^\circ\text{F} and dry air), so always check which one a rating uses. Free air delivery (FAD) is the compressor's delivered flow referred back to its actual inlet conditions. With a 14.7 psia14.7\,\text{psia}, 68∘F68^\circ\text{F} (528∘R528^\circ\text{R}) reference:

SCFM=ACFM(Pact14.7 psia)(528∘RTact+460)\text{SCFM} = \text{ACFM} \left(\frac{P_{\text{act}}}{14.7\,\text{psia}}\right) \left(\frac{528^\circ\text{R}}{T_{\text{act}} + 460}\right)

where ACFM\text{ACFM} is the actual volumetric flow at the measured absolute pressure PactP_{\text{act}} (psia) and temperature TactT_{\text{act}} (∘F^\circ\text{F}).

Air Preparation: The FRL Unit

Before entering pneumatic valves and cylinders, raw plant air must pass through an FRL (Filter-Regulator-Lubricator) conditioning unit:

              FRL (Filter - Regulator - Lubricator) Train
    Main Header                                                   Pneumatic Circuit
    -----------> [ Filter ] ------> [ Regulator ] ------> [ Lubricator ] -------->
                 (Water/Dirt)       (Set Working P)       (Oil Mist Aerosol)
  1. Filter: Removes liquid moisture, condensate, and solid particulates down to 5−40 μm5 - 40\,\mu\text{m} using centrifugal swirl vanes and sintered porous bronze elements.
  2. Regulator: Diaphragm-actuated pressure reducing valve with relieving vent. Maintains uniform working pressure despite line fluctuations.
  3. Lubricator: Utilizes a venturi nozzle to inject a micro-fog aerosol of lubricating oil into the air stream for pneumatic cylinders and vane motors (many modern pneumatic valves specify non-lubricated dry air).

Step-by-Step Worked Hydraulic Sizing Calculation

Engineering Problem Statement

A heavy-duty hydraulic stamping press actuator must meet the following operational specifications:

  • Required Pressing Force (FpressF_{\text{press}}): 180 kN180\,\text{kN} (180, ⁣000 N180,\!000\,\text{N}) during extension stroke.
  • Cylinder Stroke (SS): 600 mm600\,\text{mm} (0.60 m0.60\,\text{m}).
  • Maximum System Working Pressure (PsysP_{\text{sys}}): 210 bar210\,\text{bar} (21.0 MPa=21.0×106 N/m221.0\,\text{MPa} = 21.0 \times 10^6\,\text{N/m}^2).
  • Target Extension Time (textt_{\text{ext}}): 6.0 seconds6.0\,\text{seconds}.
  • Target Retraction Time (trett_{\text{ret}}): 3.5 seconds3.5\,\text{seconds}.
  • Hydraulic Pump Characteristics: Driven by an AC induction motor at n=1, ⁣450 rpmn = 1,\!450\,\text{rpm}; volumetric efficiency ηv=0.92\eta_v = 0.92; overall efficiency ηo=0.85\eta_o = 0.85.

Calculate:

  1. Minimum required piston bore diameter DpD_p and the next larger preferred bore size, in a cylinder series rated for at least 210 bar210\,\text{bar}.
  2. Required pump flow rate QextQ_{\text{ext}} in L/min\text{L/min}.
  3. Required cylinder rod diameter drd_r to achieve the 3.5 s3.5\,\text{s} retraction stroke with this pump flow rate, and the preferred rod size.
  4. Required pump volumetric displacement VDV_D in cc/rev\text{cc/rev} (cm3/rev\text{cm}^3/\text{rev}).
  5. Hydraulic output power PhydP_{\text{hyd}} in kW\text{kW} and required electric drive motor shaft power in kW\text{kW} (and equivalent hphp).

Step-by-Step Solution

Step 1: Piston Bore Diameter (DpD_p)

The full-bore cap-end piston area ApA_p must produce 180 kN180\,\text{kN} at 21.0 MPa21.0\,\text{MPa}:

Ap=FpressPsys=180,000 N21.0×106 N/m2=8.5714×10−3 m2=85.71 cm2A_p = \frac{F_{\text{press}}}{P_{\text{sys}}} = \frac{180{,}000\,\text{N}}{21.0 \times 10^6\,\text{N/m}^2} = 8.5714 \times 10^{-3}\,\text{m}^2 = 85.71\,\text{cm}^2

The theoretical minimum bore diameter is:

Dp=4Apπ=4×8.5714×10−3π=0.10447 m=104.5 mmD_p = \sqrt{\frac{4 A_p}{\pi}} = \sqrt{\frac{4 \times 8.5714 \times 10^{-3}}{\pi}} = 0.10447\,\text{m} = 104.5\,\text{mm}

The preferred bore sizes of ISO 3320 step from 100100 to 125 mm125\,\text{mm}, so select Dp=125 mmD_p = 125\,\text{mm} in a cylinder series rated for at least 210 bar210\,\text{bar} (for example, the 250 bar250\,\text{bar} ISO 6022 series; the common ISO 6020 series is rated 160 bar160\,\text{bar}). Actual piston area:

Ap=π4(0.125)2=1.2272×10−2 m2=122.7 cm2A_p = \frac{\pi}{4} (0.125)^2 = 1.2272 \times 10^{-2}\,\text{m}^2 = 122.7\,\text{cm}^2

Actual maximum thrust at 210 bar210\,\text{bar}:

Factual=Psys⋅Ap=(21.0×106)(1.2272×10−2)=257,700 N=257.7 kN(>180 kN)F_{\text{actual}} = P_{\text{sys}} \cdot A_p = (21.0 \times 10^6)(1.2272 \times 10^{-2}) = 257{,}700\,\text{N} = 257.7\,\text{kN} \quad (> 180\,\text{kN})

(In practice the relief valve could then be set lower, near 147 bar147\,\text{bar}, to deliver just the required force.)

Step 2: Required Pump Flow Rate (QextQ_{\text{ext}})

The required extension velocity is:

vext=Stext=0.60 m6.0 s=0.10 m/sv_{\text{ext}} = \frac{S}{t_{\text{ext}}} = \frac{0.60\,\text{m}}{6.0\,\text{s}} = 0.10\,\text{m/s}

The required flow to the cap end is:

Q=Ap⋅vext=(1.2272×10−2)(0.10)=1.2272×10−3 m3/s=73.63 L/minQ = A_p \cdot v_{\text{ext}} = (1.2272 \times 10^{-2})(0.10) = 1.2272 \times 10^{-3}\,\text{m}^3/\text{s} = 73.63\,\text{L/min}

Step 3: Cylinder Rod Diameter (drd_r)

The retraction velocity required to complete the 0.60 m0.60\,\text{m} stroke in 3.5 s3.5\,\text{s} is:

vret=0.603.5=0.17143 m/sv_{\text{ret}} = \frac{0.60}{3.5} = 0.17143\,\text{m/s}

With the same pump flow, the annular area must be:

Ar=Qvret=1.2272×10−30.17143=7.1586×10−3 m2A_r = \frac{Q}{v_{\text{ret}}} = \frac{1.2272 \times 10^{-3}}{0.17143} = 7.1586 \times 10^{-3}\,\text{m}^2

So the rod area and theoretical rod diameter are:

Arod=Ap−Ar=(12.272−7.159)×10−3=5.113×10−3 m2,dr=4Arodπ=0.0807 m=80.7 mmA_{\text{rod}} = A_p - A_r = (12.272 - 7.159) \times 10^{-3} = 5.113 \times 10^{-3}\,\text{m}^2, \qquad d_r = \sqrt{\frac{4 A_{\text{rod}}}{\pi}} = 0.0807\,\text{m} = 80.7\,\text{mm}

Select the nearest preferred rod size from ISO 3320, dr=80 mmd_r = 80\,\text{mm}, and verify:

Arod=π4(0.080)2=5.0265×10−3 m2,Ar=(12.272−5.027)×10−3=7.2453×10−3 m2A_{\text{rod}} = \frac{\pi}{4} (0.080)^2 = 5.0265 \times 10^{-3}\,\text{m}^2, \qquad A_r = (12.272 - 5.027) \times 10^{-3} = 7.2453 \times 10^{-3}\,\text{m}^2 vret=1.2272×10−37.2453×10−3=0.16938 m/s  ⟹  tret=0.600.16938=3.54 s(≈3.5 s)v_{\text{ret}} = \frac{1.2272 \times 10^{-3}}{7.2453 \times 10^{-3}} = 0.16938\,\text{m/s} \implies t_{\text{ret}} = \frac{0.60}{0.16938} = 3.54\,\text{s} \quad (\approx 3.5\,\text{s}) Fret=Psys⋅Ar=(21.0×106)(7.2453×10−3)=152,200 N=152.2 kNF_{\text{ret}} = P_{\text{sys}} \cdot A_r = (21.0 \times 10^6)(7.2453 \times 10^{-3}) = 152{,}200\,\text{N} = 152.2\,\text{kN}

Step 4: Pump Volumetric Displacement (VDV_D)

The required actual delivery is Qact=73.63 L/minQ_{\text{act}} = 73.63\,\text{L/min}. With volumetric efficiency ηv=0.92\eta_v = 0.92, the theoretical flow is:

Qt=Qactηv=73.630.92=80.03 L/min=80,030 cm3/minQ_t = \frac{Q_{\text{act}}}{\eta_v} = \frac{73.63}{0.92} = 80.03\,\text{L/min} = 80{,}030\,\text{cm}^3/\text{min}

At shaft speed n=1,450 rpmn = 1{,}450\,\text{rpm}:

VD=Qtn=80,0301,450=55.2 cm3/revV_D = \frac{Q_t}{n} = \frac{80{,}030}{1{,}450} = 55.2\,\text{cm}^3/\text{rev}

Selection: a commercial 60 cc/rev60\,\text{cc/rev} variable-displacement axial piston pump set to about 55 cc/rev55\,\text{cc/rev}.

Step 5: Hydraulic and Drive Motor Power

Hydraulic output power at full pressure and flow:

Phyd=P (bar)×Q (L/min)600=210×73.63600=25.77 kWP_{\text{hyd}} = \frac{P\,(\text{bar}) \times Q\,(\text{L/min})}{600} = \frac{210 \times 73.63}{600} = 25.77\,\text{kW}

Shaft power required from the electric motor, with overall pump efficiency ηo=0.85\eta_o = 0.85:

Pshaft=Phydηo=25.770.85=30.32 kW=30.320.7457=40.7 hpP_{\text{shaft}} = \frac{P_{\text{hyd}}}{\eta_o} = \frac{25.77}{0.85} = 30.32\,\text{kW} = \frac{30.32}{0.7457} = 40.7\,\text{hp}

(Check in USCS units: 210 bar=3,046 psi210\,\text{bar} = 3{,}046\,\text{psi} and 73.63 L/min=19.45 gpm73.63\,\text{L/min} = 19.45\,\text{gpm}, so Phyd=(3,046×19.45)/1,714=34.6 hpP_{\text{hyd}} = (3{,}046 \times 19.45)/1{,}714 = 34.6\,\text{hp} and Pshaft=34.6/0.85=40.7 hpP_{\text{shaft}} = 34.6/0.85 = 40.7\,\text{hp}.)

Motor Sizing Decision: 30.3 kW30.3\,\text{kW} slightly exceeds the 30 kW30\,\text{kW} IEC rating, so select the next standard size, 37 kW37\,\text{kW} (50 hp50\,\text{hp}), unless the duty cycle shows that full pressure and full flow never occur together (an RMS-power check could then justify 30 kW30\,\text{kW}).

Test Your Knowledge

A hydraulic power unit operates at a continuous pressure of 2,400 psi delivering a fluid flow rate of 25 gpm. If the pump overall efficiency is 82%, what electric motor brake horsepower is required to drive the pump?

A

28.6 hp

B

35.0 hp

C

52.1 hp

D

42.7 hp

Test Your Knowledge

A vertical hydraulic press cylinder holding a heavy die must lower the tooling slowly and smoothly without lunging forward or cavitating under the pull of gravity. Which valve and circuit configuration should be specified?

A

A meter-in flow control circuit on the cap end supply line.

B

A meter-out flow control circuit with a counterbalance valve on the rod return line.

C

A bleed-off bypass circuit connected directly to the pump discharge line.

D

A direct-acting pressure relief valve placed on the pump suction port.

Test Your Knowledge

An industrial air compressor delivers 150 ACFM of compressed air at an actual operating pressure of 102.9 psig and temperature of 100 degrees F. What is the approximate flow in SCFM, referenced to standard conditions of 14.7 psia and 68 degrees F?

A

150 SCFM

B

850 SCFM

C

1,130 SCFM

D

1,470 SCFM

Sections you finish are checked off in the contents.