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    Monroe L. Weber-ShirkSchool of Civil and

    Environmental Engineering

    Hydraulic Machinery

    Pumps, Turbines...

    http://ceeserver.cee.cornell.edu/mw24/Default.htmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/index.cfmhttp://www.cee.cornell.edu/faculty/info.cfm?abbrev=faculty&shorttitle=bio&netid=mw24http://ceeserver.cee.cornell.edu/mw24/Default.htmhttp://ceeserver.cee.cornell.edu/mw24/Default.htmhttp://ceeserver.cee.cornell.edu/mw24/Default.htmhttp://www.cornell.edu/
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    Hydraulic Machinery Overview

    Types of Pumps

    Dimensionless Parameters for Turbomachines

    Power requirements Head-discharge curves

    Pump Issues

    Cavitation

    NPSH

    Priming

    Pump selection

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    Types of Pumps

    Positive displacement

    piston pump

    peristaltic pump

    gear pump two-lobe rotary pump

    screw pump

    Jet pumps

    Turbomachines axial-flow (propeller pump)

    radial-flow (centrifugal pump)

    mixed-flow (both axial and radial flow)

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    Positive Displacement Pumps

    Piston pump

    Diaphragm pump

    Peristaltic pump

    Rotary pumps

    gear pump

    two-lobe rotary pump

    screw pump

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    Rotary Pumps

    Gear Pump

    fluid is trapped between gear teeth and the

    housingTwo-lobe Rotary Pump

    (gear pump with two teeth on each gear

    same principle as gear pump fewer chambers - more extreme pulsation

    trapped fluid

    http://www.koboldusa.com/onlinecatalog/flow/zdm/zdm1.html
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    Rotary Pumps

    Disadvantages

    precise machining

    abrasives wear surfaces rapidlypulsating output

    Uses

    vacuum pumps

    air compressors

    hydraulic fluid pumps

    food handling

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    Screw Pump

    Can handle debris

    Used to raise thelevel of wastewater

    Abrasive materialwill damage theseal between screwand the housing

    Grain augers usethe same principle

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    Positive Displacement Pumps

    What happens if you close a valve on the

    effluent side of a positive displacement pump?

    What does flow rate vs. time look like for apiston pump?

    0

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    0 2 4 6 8 10

    rads

    totalflow

    1st piston

    2nd piston

    3rd piston

    3 pistons

    Thirsty Refugees

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    (inefficient process)

    Turbomachines

    impeller

    casing housing

    ( ) ( )2 12 1z t tT Q r V rV r = -

    Demours centrifugal pump - 1730

    Theory conservation of angular momentum

    conversion of kinetic energy to potential energy in flow

    expansion ___________ ________

    Pump components rotating element - ___________

    encloses the rotating element and seals the pressurized

    liquid inside - ________ or _________

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    Radial Pumps

    ImpellerVanes

    Casing

    Suction Eye Impeller

    Discharge

    centrifugal

    Flow Expansion

    diameter rotational speed

    also called _________ pumps

    broad range of applicable flows and heads

    higher heads can be achieved by increasing the_______ or the ________ ______ of the impeller

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    Dimensionless Parameters for

    Turbomachines

    We would like to be able to compare pumps withsimilar geometry. Dimensional analysis to therescue...

    To use the laws of similitude to compareperformance of two pumps we need

    exact geometric similitude

    all linear dimensions must be scaled identically

    roughness must scale homologous - streamlines are similar

    constant ratio of dynamic pressures at correspondingpoints

    also known as kinematic similitude

    3D

    Q

    same

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    Kinematic Similitude:

    Constant Force Ratio

    VD

    gl

    V2

    gl

    V

    lV2

    V

    c

    viscous

    gravity

    surface-tension

    elastic

    Reynolds

    ratio of inertial to _______ forces

    Froude ratio of inertial to ________ force

    Weber

    ratio of inertial to _______ ______ forces

    Mach

    ratio of inertial to _______ forces

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    Turbomachinery Parameters

    2

    2C

    V

    pp

    2

    C

    V

    HgH

    2

    flowD

    Q

    A

    QV

    2

    4

    C

    Q

    HgDflowH

    4

    2 3, , ,

    flow flow

    H

    impeller flow flow

    HgD D QC f Re

    Q D D D

    e

    w

    D= =

    impeller (Impeller is better defined)

    3, , , , , ,

    flow

    p

    impeller flow flow

    D QC f Re F W M

    D D D

    e

    w

    =

    Where is the fluid?

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    Shape Factor

    Related to the ratio of flow passage

    diameter to impeller diameter

    Defined for the point of best efficiency

    What determines the ideal shape for a

    pump?

    )(fS ,,, pQ

    Exercise

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    Impeller Geometry:

    Shape Factor

    0.18

    0.37

    1.25

    2.33

    3.67axial: high _______, low _______

    mixed

    radial

    mixed

    S Q

    gHp 3 4

    pressure flow

    pressureflow

    S

    500

    1000

    3400

    6400

    10000

    N

    43psp

    H

    QNN

    *N in rpm, Q in gpm, H in ft

    *

    Impeller

    diameter

    Nsp= 2732S

    Radial: high _______, low ____

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    Use of Shape Factor:

    Specific Speed

    The maximum efficiencies for all pumps occurswhen the Shape Factor is close to 1!

    Flow passage dimension is close to impeller diameter!

    Low expansion losses!

    There must be an optimal shape factor given adischarge and a head.

    Double suction (like two pumps in parallel) Multistage (pumps in series)

    Use Q and H for each stage

    S Q

    gHp 3 4

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    Additional Dimensionless

    Parameters

    CH Hg

    2D2

    53

    D

    PCP

    CQ Q

    D3

    S

    CQ1 2

    CH3 4

    impeller

    power

    Alternate equivalent way

    to calculate S.

    D is the _______ diameter

    P is the _____

    (defined at max efficiency)

    HQPw

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    Head-Discharge Curve

    Theoreticalhead-dischargecurve

    Actual head-

    discharge curve

    Q

    H circulatory flow -inability of finite

    number of blades to

    guide flow

    friction - ____

    shock - incorrect angle

    of blade inlet ___

    other losses

    bearing friction

    packing friction

    disk friction

    internal leakage

    V2

    V2

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    Pump Power Requirements

    HQPw

    s

    wP

    P

    Pe

    m

    sm

    P

    Pe

    mP

    m

    ee

    HQP

    water

    pump

    shaftmotor

    Water power

    Subscripts

    w = _______

    p = _______

    s = _______m = _______

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    Impeller Shape vs. Power Curves

    S

    1 - O.33

    2 - 0.81

    3 - 1.5

    4 - 2.1

    5 - 3.4

    Discharge (% of design)Powe

    r(%ofde

    sign)

    axial

    radial

    Implicationshttp://www.mcnallyinstitute.com/

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    Affinity Laws

    With speed, , held constant:

    3

    2

    1

    2

    1

    P

    P2

    2

    1

    2

    1

    H

    H

    2

    1

    2

    1

    Q

    Q

    With diameter, D, held constant:

    5

    1 1

    2 2

    P D

    P D

    =

    2

    2

    1

    2

    1

    D

    D

    H

    H3

    1 1

    2 2

    Q D

    Q D

    =

    CH Hg

    2

    D2

    CQQ

    D3

    HQP

    53

    D

    PCP

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    Pump Example

    Given a pump with shape factor of 4.57, a

    diameter of 366 mm, a 2-m head, a speed of

    600 rpm, and dimensionless performancecurves (previous slide).

    What will the discharge be?

    How large a motor will be needed if motorefficiency is 95%?

    Exercise

    0

    0.01

    0.02

    0.03

    0.04

    0.05

    0.06

    0.07

    0.08

    0 0.02 0.04 0.06 0.08 0.1

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    D=0.366 m

    CH

    Hg

    2D

    2

    3D

    QCQ

    Efficiency

    0

    0.01

    0.02

    0.03

    0.04

    0.05

    0.06

    0.07

    0.08

    0 0.02 0.04 0.06 0.08 0.1

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    D=0.366 m

    CH

    Hg

    2D

    2

    3D

    QCQ

    Efficiency

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    Pumps in Parallel or in Series

    Parallel

    Flow ________

    Head ________

    Series

    Flow ________

    Head ________

    Multistage

    adds

    same

    same

    adds

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    Cavitation in Water Pumps

    water vapor bubbles

    form when the pressure

    is less than the vaporpressure of water

    very high pressures

    (800 MPa or 115,000

    psi) develop when thevapor bubbles collapse 0

    1000

    2000

    3000

    4000

    5000

    6000

    7000

    8000

    0 10 20 30 40

    Temperature (C)

    Vaporpressure(

    Pa)

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    Net Positive Suction Head

    1

    2

    2

    2s s v

    R

    p V pNPSH

    gg g= + -

    s = suction

    Total head -pv!

    NPSHRincreases with Q2!

    Elevation datum

    Absolute pressure

    2

    2

    eye eyevR

    p VpNPSH

    gg g= - + At cavitation!

    z

    How much total head in excess of vapor pressure is available?

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    NPSHR

    2

    2atm v s s v

    L

    p p p V pz h

    gg g g g - D - - = + -

    2

    2atm s s

    reservoir L

    p p Vz hgg g+ = + +

    2

    2atm s s

    L

    p p Vz h

    gg g- D - = +

    atm v

    L A

    p pz h NPSH

    g g- D - - =

    Subtract vapor pressure

    2 2

    1 1 2 21 2

    2 2 L

    p V p Vz z h

    g gg g+ + = + + +

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    NPSH problem

    Determine the minimum

    reservoir level relative to the

    pump centerline that will beacceptable. The NPSHrfor

    the pump is 2.5 m. Assume

    you have applied the energyequation and found a head

    loss of 0.5 m.

    18C

    ?

    Exercise

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    Pumps in Pipe Systems

    0

    20

    40

    60

    80

    100

    120

    0 0.2 0.4 0.6 0.8Discharge (m3/s)

    Head(m)

    system operating point

    Static head

    Head vs. dischargecurve for ________pump

    What happens as the static head changes (a tank fills)?

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    Priming

    CH

    p2D2

    p CH2D2

    CH

    Hg

    2D2

    density

    1.225 kg/m3

    The pressure increase created is

    proportional to the _______ of the fluid

    being pumped. A pump designed for water will be

    unable to produce much pressure

    increase when pumping air

    Density of air at sea level is __________

    Change in pressure produced by pump is

    about 0.1% of design when pumping air

    rather than water!

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    Priming Solutions

    Applications with water at less than atmospheric

    pressure on the suction side of the pump require a

    method to remove the air from the pump and the

    inlet piping

    Solutions

    foot valve

    priming tank vacuum source

    self priming

    foot valve

    to vacuum pumppriming tank

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    Self-Priming Centrifugal Pumps

    Require a small volume of liquid in the

    pump

    Recirculate this liquid and entrain airfromthe suction side of the pump

    The entrained air is separated from the

    liquid and discharged in the pressure side ofthe pump

    http://www.gouldspumps.com/download_files/3796/3796_priming.stm
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    Variable Flows?

    How can you obtain a wide range of flows?

    __________________________

    __________________________

    __________________________

    __________________________

    __________________________

    Why is the flow from two identical pumps

    usually less than the 2x the flow from one

    pump?

    Valve

    Multiple pumps (same size)Multiple pumps (different sizes)

    Variable speed motor

    Storage tank

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    RPM for Pumps

    60 cycle

    variable speed

    belt drive

    number of

    poles sync full load rad/sec

    2 3600 3500 367

    4 1800 1750 183

    6 1200 1167 1228 900 875 92

    10 720 700 73

    12 600 583 61

    14 514 500 52

    16 450 438 46

    18 400 389 4120 360 350 37

    22 327 318 33

    24 300 292 31

    26 277 269 28

    28 257 250 26

    30 240 233 24

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    Estimate of Pump rpm

    The best efficiency is obtained when S=1

    Given a desired flow and head the

    approximate pump rpm can be estimated!

    S Q

    gHp 3 4

    ( )3 4

    pgH

    Qw

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    Pump Selection

    Material Compatibility

    Solids

    Flow Head

    NPSHa

    Pump Selection software A finite number of pumps will come close to

    meeting the specifications!

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    Pump Selection Chart

    Model X

    Model M

    http://www.pricepump.com/

    http://www.pricepump.com/http://www.pricepump.com/http://www.pricepump.com/http://www.pricepump.com/
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    End of Curve Operation

    Right of the BEP

    is sufficient NPSH available for the pump to operateproperly?

    fluid velocities through the suction and dischargenozzles of the pump could be extremely high, resultingin increased pump and system noise

    Left of BEP operation

    high thrust loads on the pump bearings and mechanicalface seals result in premature failure.

    The pump is oversized, resulting in lower efficiencyand higher operating and capital costs.

    Q

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    Goulds Pump Curves

    BEP = 1836 L/s

    S Q

    gHp 3 4

    Splitcase double suction890 rpm = 93.2 rad/s

    S=0.787

    Check the Power!

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    Pump Installation Design

    Why not use one big pump?

    Can the system handle a power failure?

    Can the pump be shut down for

    maintenance?

    How is the pump primed?

    Are there enough valves so the pump can be

    removed for service without disabling the

    system?

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    Pump Summary

    Positive displacement vs. turbomachines

    Dimensional analysis

    Useful for scaling

    Useful for characterizing full range of pumpperformance from relatively few data points

    Turbomachines convert shaft work into increasedpressure (or vice versa for turbines)

    The operating point is determined by where thepump and system curves intersect

    NPSH

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    Water problem?

    Early in my college days I took a break and spent 17 months in Salvadoranrefugee camps in Honduras. The refugee camps were located high in themountains and for several of the camps the only sources of water large enoughto sustain the population of 6-10,000 were located at much lower elevations. So

    it was necessary to lift water to the camps using pumps.

    When I arrived at the camps the pumps were failing frequently and the pipeswere bursting frequently. Piston pumps were used. The refugees werecomplaining because they needed water. The Honduran army battalion wasnervous because they didnt want any refugees leaving the camp. There was

    only one set of spare parts (valve springs and valves) for the pump and the lastset of parts only lasted a few days. The pump repair crew didnt want to startusing the pump until the real cause of the problem was fixed because spareparts have to be flown in from Miami.

    Water problem:

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    Water problem:

    proposed solutions?

    piston pump (80 L/min)

    2 km pipeline (2galvanized and then3 PVC) with rise of100 m

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    Pump Curve Solution

    22D

    HgCH

    CQ

    Q

    D3

    srevs

    rev/8.62

    2

    60

    min1

    min

    600

    037.0366.0/8.62

    /8.9222

    2 ms

    smmCH

    068.0QC

    3DCQ Q smmsQ /21.0366.0/8.62068.033

    ( )( )( )

    ( )( )

    3 39800 / 0.21 / 25.55

    0.78 0.95

    N m m s mP kW= =

    mP

    m

    ee

    HQP

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    Pump Curve Solution

    0

    0.01

    0.02

    0.03

    0.04

    0.05

    0.06

    0.07

    0.08

    0 0.02 0.04 0.06 0.08 0.10

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0.8

    0.9

    1

    D=0.366 m

    CH Hg

    2

    D2

    CQ

    Q

    D3

    Efficiency

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    NPSH solution

    18C

    ?A RNPSH NPSH=

    atm vl R

    p pz h NPSH

    g

    -D = - - Papv 2000

    3

    /9789 mN

    101300atmp Pa=

    mmmN

    PaPaz 5.25.0/9789

    20001013003

    mz 14.7

    atm vA L

    p pNPSH z h

    g

    -= - D -

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    Find Q

    ( ) ( )2 1

    2 1z t tT Q r V rV r = -

    2 2z tT QV r r=

    1

    V1

    2

    2gz1 hp

    p2

    V2

    2

    2gz2 hl

    2 2z tT Q V r w r w=

    2 2tz

    p

    V rTh

    Q g

    ww

    g= =

    2

    22 2

    22

    tV r V

    zg g

    w

    = +

    work

    Dimensional analysis

    Neglect head loss

    Datum is reservoir level

    Let A = 10 cm2

    2 2tz

    V rT

    VA g

    ww

    g=

    H ld lift t

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    How could we lift water more

    efficiently?

    2

    22 2

    2

    tV r Vz

    g g

    w= + D

    2 2 22 2tQ A V r g z AV w= - D =

    Solve for Q=AV

    Decrease V without decreasing Q! (

    vt

    r

    cs

    p zh T

    z Q z

    w

    g=

    D D

    2 22 2t

    p z

    A z V r g zz

    h T

    g w

    w

    D - DD=

    2 2z tT Q V r w r w=

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    Lost energy

    2

    22 2

    2

    tV r Vz

    g g

    w= + D

    2

    22 2

    2

    tV r Vz

    g g

    w= + D

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    0.1

    1

    10

    100

    1000

    0.0001 0.001 0.01 0.1 1 10

    Flow (m3/s)

    Pumpinghead(m)

    Axial

    Mixed

    Radial

    Positive

    displacement

    20

    4060

    10

    200

    400600

    100

    2000

    40006000

    1000

    1 2 4 6

    Selection of Pump Type

    P

    ower(kW)