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PREPARED BY
RAHUL KSHIRSAGAR
OVERVIEW
 Difference between Rigid Rotor and Flexible Rotor.
 Rigid Rotor balancing using cradle balancing machine.
 Graphical method for calculating correction of mass and
its position.
 Flexible Rotor balancing using influence coefficient
method.
DIFFERENCE BETWEEN RIGID
ROTOR AND FLEXIBLE ROTOR
 Rigid Rotor:-As long the rotor does not experience any
deformations while operating at the critical speed, the
rotor is known as rigid rotor
 Flexible rotor:- While running at critical speed, if the rotor
bends and the bend centre line whirls around and set up
additional centrifugal forces then the rotor is called as
flexible rotor.
Rigid Rotor balancing using cradle
balancing machine.
Procedure is followed by based on following four
observations
 without addition of trial mass to the rotor
 with a trial mass at θ = 00
 with a trial mass at θ = 1800
 with same trial mass at θ = ±900
Where θ is measured from reference plane
Graphical method for calculating correction of mass
required to be placed and its position for system
balancing.
 OA vector is the amplitude
measured without trial mass
 OB vector is the amplitude
measured in the trial run by adding
a trial mass at 0˚
 AB vector represents the effect of
the trial mass
 OC vector measured in the trial
run at 180˚
 Thus, AB vector = AC vector with
phase difference of 180˚
BALANCING OF FLEXIBLE ROTOR USING
INFLUENCE COEFFICIENT METHOD
A ROTOR SYSTEM WITH MEASUREMENT
LOCATIONS AND BALANCING PLANES
 Let p number of balancing planes where p>2
 q number of measuring planes and these are q=2 at the
bearing planes
 let unbalance in each plane U = me
 Therefore the response can be related with influence
coefficient and unbalance as
 By knowing the influence coefficient, from
equation (1),we can obtain residual unbalance as
follows
 Influence coefficient is obtained
experimentally as follows by adding a trial
mass at plane 1.
Balancing of rigid rotor and balancing of flexible rotor-A Review
Balancing of rigid rotor and balancing of flexible rotor-A Review

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Balancing of rigid rotor and balancing of flexible rotor-A Review

  • 2. OVERVIEW  Difference between Rigid Rotor and Flexible Rotor.  Rigid Rotor balancing using cradle balancing machine.  Graphical method for calculating correction of mass and its position.  Flexible Rotor balancing using influence coefficient method.
  • 3. DIFFERENCE BETWEEN RIGID ROTOR AND FLEXIBLE ROTOR  Rigid Rotor:-As long the rotor does not experience any deformations while operating at the critical speed, the rotor is known as rigid rotor  Flexible rotor:- While running at critical speed, if the rotor bends and the bend centre line whirls around and set up additional centrifugal forces then the rotor is called as flexible rotor.
  • 4. Rigid Rotor balancing using cradle balancing machine.
  • 5. Procedure is followed by based on following four observations  without addition of trial mass to the rotor  with a trial mass at θ = 00  with a trial mass at θ = 1800  with same trial mass at θ = ±900 Where θ is measured from reference plane
  • 6. Graphical method for calculating correction of mass required to be placed and its position for system balancing.  OA vector is the amplitude measured without trial mass  OB vector is the amplitude measured in the trial run by adding a trial mass at 0˚  AB vector represents the effect of the trial mass  OC vector measured in the trial run at 180˚  Thus, AB vector = AC vector with phase difference of 180˚
  • 7.
  • 8. BALANCING OF FLEXIBLE ROTOR USING INFLUENCE COEFFICIENT METHOD
  • 9. A ROTOR SYSTEM WITH MEASUREMENT LOCATIONS AND BALANCING PLANES
  • 10.  Let p number of balancing planes where p>2  q number of measuring planes and these are q=2 at the bearing planes  let unbalance in each plane U = me
  • 11.  Therefore the response can be related with influence coefficient and unbalance as
  • 12.
  • 13.  By knowing the influence coefficient, from equation (1),we can obtain residual unbalance as follows
  • 14.  Influence coefficient is obtained experimentally as follows by adding a trial mass at plane 1.