rotordynamics_5

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1 Bernhard Bettig Mechanical Design Research Lab Mechanical Engineering - Engineering Mechanics Dept. Michigan Technological University Web site : http://www.me.mtu.edu/~mdrl Rotordynamics – Unit 5: Modeling Journal Bearings 2 Journal Bearing – review The journal bearing appears in the dynamic finite element equations as a linear spring and damper. = + y x yy yx xy xx yy yx xy xx F F v u k k k k v u c c c c & &

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rotordynamics chapter 5

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  • 11

    Bernhard BettigMechanical Design Research Lab

    Mechanical Engineering - Engineering Mechanics Dept.Michigan Technological UniversityWeb site: http://www.me.mtu.edu/~mdrl

    Rotordynamics Unit 5:Modeling Journal Bearings

    2

    Journal Bearing review The journal bearing appears in the

    dynamic finite element equations as a linear spring and damper.

    =

    +

    y

    x

    yyyx

    xyxx

    yyyx

    xyxx

    FF

    v

    u

    kkkk

    v

    u

    cc

    cc

  • 23

    Journal Bearing review In order to determine the c and k coefficient

    values, we must consider the fluid pressures in the bearing.

    4

    Journal Bearing reviewThe fluid pressures can be calculated using Reynolds equation:

  • 35

    Perturbation Solution To determine the dynamic coefficients,

    we can assume that the pressure is the sum of the static pressure and variations due to small motions of the shaft about the static equilibrium position.

    where:

    6

    Perturbation Solution

    and:

  • 47

    Fluid Pressure Calculations The boundary conditions for a

    journal bearing are:

    boundary pressure static at the 0condition)boundary s(Reynold

    edge trailingfilm at the 0

    grooves,supply at pressure feeding theequals , and 0at 0

    =

    =

    =

    =

    ===

    p

    Zppp

    pLzzp B

    8

    Fluid Pressure Calculations The fluid pressure distribution looks like:

    Static (p0)

    Perturbation (px)Perturbation (py)

  • 59

    Fluid Pressure Calculations The pressure distribution varies as a

    function of e0/c, , and .

    10

    Fluid Pressure Calculations

  • 611

    Fluid Pressure Calculations

    The bearing force is assumed to be comprised of the static force and dynamic forces due to small shaft motions.

    12

    Fluid Pressure Calculations The static force and dynamic coefficients

    are found through integration:

  • 713

    Fluid Pressure Calculations

    14

    Numerical Calculations The pressures are solved numerically

    using the finite difference method.

    Control Volume

    Neighboring Control Volumes

  • 815

    Numerical Calculations

    16

    Numerical Calculations

  • 917

    Numerical Calculations

    18

    Numerical Calculations

  • 10

    19

    Numerical Calculations

    20

    Numerical Calculations The integrations are performed by

    summation of each control volume.

  • 11

    21

    Numerical Calculations

    22

    Sample Questions1. The bearing from last week is discretized into a 20 x

    20 grid of control volumes. The shaft is displaced 3 mm in the +X direction.

    Consider a control volume centered at = 0 and Z = LB/2. What is the new pressure, after the next iteration, if the static pressure in this cell is 1.5 MPaand the neighboring pressures are 1.2 MPa (east), 1.3 MPa (south), 0.7 MPa (west), and 0.8 MPa (north)?

    2. What contribution (in Newtons) does the pressure of this control volume make to the total force (a) in the X direction, (b) in the Y direction.