Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 181 Pumps • Source of hydraulic power • Converts mechanical energy to hydraulic energy • prime movers - engines, electrical motors, manual power • Two main types: • positive displacement pumps • non-positive displacement pumps M..E., University of Minnesota (updated 12.2010) 1 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 182 Pump - Introduction M..E., University of Minnesota (updated 12.2010) 2 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 183 Positive displacement pumps • Displacement is the volume of fluid displaced cycle of pump motion • unit = cc or in3 • Positive displacement pumps displace (nearly) a fixed amount of fluid per cycle of pump motion, (more of less) independent of pressure • leak can decrease the actual volume displaced as pressure increases • Therefore, flow rate Q gpm = D (gallons) * frequency (rpm) • E.g. pump displacement = 0.1 litre • Q = 10 lpm if pump speed is 100 rpm • Q = 20 lpm if pump speed is 200 rpm M..E., University of Minnesota (updated 12.2010) 3 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 184 Non positive displacement pumps Centrifugal Pump Impeller Pump M..E., University of Minnesota (updated 12.2010) 4 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 185 Non-positive displacement pump • Flow does not depend on kinematics only - pressure important • Also called hydro-dynamic pump (pressure dependent) • Smooth flow • Examples: centrifugal (impeller) pump, axial (propeller) pump • Does not have positive internal seal against leakage • If outlet blocks, Q = 0 while shaft can still turn • Volumetric efficiency = actual flow / flow estimated from shaft speed = 0% M..E., University of Minnesota (updated 12.2010) 5 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 186 Positive vs. non-positive displacement pumps • Positive displacement pumps • • • • • • most hydraulic pumps are positive displacement high pressure (10,000psi+) high volumetric efficiency (leakage is small) large ranges of pressure and speed available can be stalled ! Non-positive displacement pumps • • • • many pneumatic pumps are non-positive displacement used for transporting fluid rather than transmitting power low pressure (<300psi), high volume flow blood pump (less mechanical damage to cells) M..E., University of Minnesota (updated 12.2010) 6 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 187 Types of positive displacement pumps • Gear pump (fixed displacement) • internal gear (gerotor) • external gear • Vane pump • fixed or variable displacement • pressure compensated • Piston pump • axial design • radial design M..E., University of Minnesota (updated 12.2010) 7 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 188 External gear pump • • • • Driving gear and driven gear Inlet fluid flow is trapped between the rotating gear teeth and the housing The fluid is carried around the outside of the gears to the outlet side of the pump As the fluid can not seep back along the path it came nor between the engaged gear teeth (they create a seal,) it must exit the outlet port. M..E., University of Minnesota (updated 12.2010) 8 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 189 Gerotor pump Inlet port Outlet port • Inner gerotor is slightly offset from external gear • Gerotor has 1 fewer teeth than outer gear • Gerotor rotates slightly faster than outer gear • Displacement = (roughly) volume of missing tooth • Pockets increase and decrease in volume corresponding to filling and pumping • Lower pressure application: < 2000psi • Displacements (determined by length): 0.1 in3 to 11.5 in3 M..E., University of Minnesota (updated 12.2010) 9 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 190 Vane Pump • • • • • • Vanes are in slots As rotor rotates, vanes are pushed out, touching cam ring Vane pushes fluid from one end to another Eccentricity of rotor from center of cam ring determines displacement Quiet Less than 4000psi M..E., University of Minnesota (updated 12.2010) 10 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 191 Pressure Compensated Vane Pump M..E., University of Minnesota (updated 12.2010) 11 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 192 PC Vane Pump (Cont’d) • Eccentricity (hence displacement) is varied by shifting the cam ring • Cam ring is spring loaded against pump outlet pressure • As pressure increases, eccentricity decreases, reducing flow rate • Spring constants determines how the P-Q curve drops: • small stiffness (sharp decrease in Q as P increases) • large stiffness (gentle decreases in Q as P increases) • Preload on spring determines • pressure at which flow starts cutting off M..E., University of Minnesota (updated 12.2010) 12 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 193 Axial Piston Pump • • • Each piston has a pumping cycle Interlacing pumping cycles produce nearly uniform flow (with some ripples) Displacement is determined by the swash plate angle • Generally can be altered manually or via (electro-) hydraulic actuator. Displacement can be varied by varying swashplate angle M..E., University of Minnesota (updated 12.2010) 13 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 194 Bent-Axis Piston Pump • • • Thrust-plate rotates with shaft Piston-rods connected to swash plate Piston barrel rotates and is connected to thrust plate via a U-joint • More efficient than axial piston pump (less friction) M..E., University of Minnesota (updated 12.2010) 14 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 195 Radial Piston Pump • • • • • Similar to axial piston pump, pistons move in and out as pump rotates. Displacement is determined by cam profile (i.e. eccentricity) Displacement variation can be achieved by moving the cam (possible, but not common though) High pressure capable, and efficient Pancake profile M..E., University of Minnesota (updated 12.2010) 15 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 197 Piston Pump - flow ripples 1 piston • Pumping • Filling • • 2 piston Total flow Even # cylinders n*rpm Odd # cylinders (2n)*rpm • • • Each cylinder has a pumping cycle Total flow = flow of each cylinder More cylinders, less ripple Frequency: Can be problematic for manual operator (ergonomic issue) Noise Displacement = # Cylinders x Stroke x Bore Area M..E., University of Minnesota (updated 12.2010) 16 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 198 # of Pistons Effect on Flow Ripples 1 n=2 n=3 n=4 n=5 0.9 0.8 0.7 Flow - 0.6 0.5 0.4 0.3 0.2 0.1 0 0 1 2 3 Angle - rad 4 5 6 M..E., University of Minnesota (updated 12.2010) 17 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 199 Pumping theory • Create a partial vacuum (i.e. reduced pressure) • Atmospheric / tank pressure forces fluid into pump • usually tank check valve opens • outlet check valve closes • Power stroke expels fluid to outlet • outlet check valve opens • tank check valve closes • Power demand for prime mover (ideal calculation) • (piston pump) Power = Force*velocity = Pressure*area*piston speed = Pressure * Flow rate • If power required > power available => Pumps stall or decrease speed M..E., University of Minnesota (updated 12.2010) 18 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 200 Aeration and Cavitation • Disastrous events - cause rapid erosion • Aeration • • • • • air bubbles enter pump at low pressure side bubbles expand in partial vacuum when fluid+air travel to high pressure side, bubbles collapse micro-jets are formed which cause rapid erosion Cavitation • dissolved air in fluid evaporates in partial vacuum to form bubbles • bubbles expands then collapse • as bubbles collapse, micro-jets formed, causing rapid erosion M..E., University of Minnesota (updated 12.2010) 19 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 201 Causes of cavitation and aeration • For positive displacement pumps, the filling rate is determined by pump speed; (Q-demand) = D * freq) • Filling pressure = tank pressure - inlet pressure • Q-actual = f(filling pressure, viscosity, orifice size, dirt) • If Q-actual < Q-demand, inlet pressure decreases significantly • This causes air to enter (via leakage) or to evaporation (cavitates) • To prevent cavitation/aeration • increase tank pressure • low viscosity, large orifice • lower speed (hence lower Q-demand) M..E., University of Minnesota (updated 12.2010) 20 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 202 Aeration and Cavitation M..E., University of Minnesota (updated 12.2010) 21 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 203 Hydraulic Motor / Actuator • Hydraulic motors / actuators are basically pumps run in reverse • Input = hydraulic power • Output = mechanical power • For motor: • Frequency (rpm) = Q (gallons per min) / D (gallons) * efficiency • Torque (lb-in) = Pressure (psi) * D (inch^3) * efficiency • efficiency about 90% • Note: units M..E., University of Minnesota (updated 12.2010) 22 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 204 Models for Pumps and Motors • M..E., University of Minnesota (updated 12.2010) 23 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 205 Non-ideal Pump/Motor Efficiencies • • • • • Ideal torque = torque required/generated for the ideal pump/motor Ideal flow = flow generated/required for the ideal pump/motor Torque loss (friction) Flow loss (leakage) Signs different for pumping and motoring mode Qact u al Pump volumetric eff: Friction Qi deal Pump mechanical eff: Ql oss Tin/out Tideal (Reverse if motor case !! ) leakage Total efficiency: vol Ideal pump Functions of speed, pressure and displacements M..E., University of Minnesota (updated 12.2010) 24 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 206 Hydro-static Transmission • A combination of a pump and a motor • Either pump or motor can have variable displacement • Replaces mechanical transmission • By varying displacements of pump/motor, transmission ratio is changed • Various topologies: • • • • • single pump / multi-motors multi (pump-motor) Open / closed circuit Open / closed loop control Integrated package / split implementation M..E., University of Minnesota (updated 12.2010) 25 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 207 Hydrostatic Transmission M..E., University of Minnesota (updated 12.2010) 26 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 208 General Consideration - Hydrostats • Advantages: • • • • • • • Wide range of operating speeds/torque Infinite gear ratios - continuous variable transmission (CVT) High power, low inertia (relative to mechanical transmission) Dynamic braking via relief valve Engine does not stall No interruption to power when shifting gear Disadvantage: • Lower energy efficiency (85% versus 92%+ for mechanical transmission) • Leaks ! M..E., University of Minnesota (updated 12.2010) 27 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 209 Closed Circuit Hydrostat Circuit Notes: • Charge pump circuit (pump + shuttle valve) • Bi-directional relief • Circuit above closed circuit because fluid re-circulates. • Open circuit systems draw and return flow to a reservoir M..E., University of Minnesota (updated 12.2010) 28 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 210 Hydrostatic Transmission • • • Let pump and motor displacements be D1 and D2, with one or both being variable. Let the torque (Nm) and speeds (rad/s) of the pump and motor be (T1, S1) and (T2,S2) Assuming ideal pumps and motors: Transmission ratio Variable by varying D1 or D2 Infinite and negative ratios possible if pump can go over-center M..E., University of Minnesota (updated 12.2010) 29 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) 211 Hydraulic Transformer • • • Used to change pressure in a power conservative way Pressure boost or buck is accompanied by proportionate flow decrease and increase Note: Hydrostatic transmission can be thought of as a mechanical transformer (torque boost/buck) Q1 Q2 D1 D2 Research opportunity! M..E., University of Minnesota (updated 12.2010) 30 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Hydraulic Hybrid Vehicles M..E., University of Minnesota (updated 12.2010) 31 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) How Hybrid Vehicles Save Energy? With a secondary power source/storage, it is possible to: • • • • Manage engine operation Store/reuse braking energy Turn off engine Downsize engine for continuous power Energy storage Engine Drive-train wheel 38% Required for maximum performance Example vehicle on EPA-UDDS cycle: • Baseline (10% engine efficiency): 24 mpg • Engine management (38% efficiency): 95 mpg • Above with regeneration: 140 mpg 10-15% Normal driving operating range M..E., University of Minnesota (updated 12.2010) 32 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Why Hydraulic Hybrids? Why not stick with electric hybrids? • Electric batteries / ultracaps (cost, reliability, recycling, power density) • Electric motors & inverters (cost, power density) • Affect overall cost, weight, and power Metrics • Fuel economy • Cost • Performance Toyota Prius M..E., University of Minnesota (updated 12.2010) 33 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Hybrid Hydraulic versus Hybrid Electric Vehicle • • • • Hydraulic pump/motor have significantly higher power density than electric motor/generator (16:1 by weight , 8:1 by volume) Hydraulic drives have much lower torque density than electric drives limits acc/braking and Accumulators are 10x more power dense than batteries hence regenerative Efficient power electronics are expensive braking • • Batteries have 2 order magnitude higher energy density than accumulators Current hydraulic systems tend to be noisy and leaky • Overall tradeoff: Hydraulic hybrids can be significantly lighter and cheaper than electric hybrids if energy density limitation can be solved. Accumulator Battery & ultracapacitor Hydraulic pump/motor Engine Engine Accumulator Parallel Hybrid Hydraulic Electric motor/ generator M..E., University of Minnesota (updated 12.2010) Parallel Hybrid Electric 34 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Hydraulic Hybrids Versus Electric Hybrids Electric Fluid Power • acceleration -- ++ • regenerative braking -- ++ Component efficiency + - Regenerative efficiency -- ++ Weight -- ++ Cost -- ++ Reliability -- ++ Environmental impact - + Energy storage ++ -- NVH ++ -- Performance Realize opportunities for • Both performance & efficiency • Cost and reliability Overcome threats in • Inefficient components • Low density energy storage • Noise, vibration, harshness + + M..E., University of Minnesota (updated 12.2010) 35 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Parallel Architecture Example: HLA system for F150 & garbage trucks • Regenerates braking energy • Utilizes efficient mechanical transmission • Does not allow full engine management Achievable engine op. points M..E., University of Minnesota (updated 12.2010) 36 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Series Architecture • Example: Eaton/UPS (truck), Ford/EPA (Escape), Artemis (BMW-5), … – Regenerates braking energy – Allows for full engine management – Independent wheel torque control possible – All power must be transmitted through fluid power components 38% 38% Required for maximum performance 10-15% 10-15% Normal driving Normal operating driving range operating range M..E., University of Minnesota (updated 12.2010) 37 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Power-Split: Hydromechanical Transmission (HMT) • Power split between mechanical and hydraulic paths • Hybridized HMT – i.e. w/ regeneration Efficient Mechanical Transmission Regenerative Braking Full engine management M..E., University of Minnesota (updated 12.2010) 38 Fluid Power Controls Laboratory (Copyright – Perry Li, 2004-2010) Hypothesized hydraulic & overall efficiencies Highway Urban 0.45 0.7 0.4 0.6 0.35 0.3 Overall efficiency Overall efficiency 0.5 0.4 0.3 0.25 0.2 0.15 0.2 series parallel hmt 0.1 0 0.05 0 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 Mean hydraulic efficiency 0.8 0.9 series parallel hmt 0.1 1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 Mean hydraulic efficiency 0.8 0.9 1 • Series / HMT at peak engine efficiency (38.5%) • Parallel at lower engine efficiency (33%) M..E., University of Minnesota (updated 12.2010) 39