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Presented by:
RONAK D. SONI
Assistant Professor
CHAPTER 1: GYROSCOPE
GYROSCOPIC EFFECT ON ROTOR
2By: Ronak Soni (RDS) Gyroscopic effect on Rotor
3
 Consider a disc fixed rigidly to a rotating shaft such
that the polar axis of the disc makes an angle with the
shaft axis, as shown in Figure.
By: Ronak Soni (RDS) Gyroscopic effect on Rotor
4
 Let the shaft rotates with an angular velocity ω rad/s in the
clockwise direction when viewed from the front. A little
consideration will show that the disc will also rotate about OX
with the same angular velocity ω rad/s.
 Let OP be the polar axis and OD the diametral axis of the
disc.
 Angular velocity of the disc about the polar axis OP or the
angular velocity of spin
= ωcosθ ... (Component of in the direction of OP)
 Since the shaft rotates, therefore the point P will move in a
plane perpendicular to the plane of paper. In other words,
precession is produced about OD.
Angular velocity of the disc about the diametral axis OD or
the angular velocity of precession
= ωsinθ
By: Ronak Soni (RDS) Gyroscopic effect on Rotor
 If IP is the mass moment of inertia of the disc about the polar
axis OP, then gyroscopic couple acting on the disc,
CP = IP. ωcosθ.ωsinθ = ½×IP.ω2sin2θ; (∵ 2 sinθ cosθ=sinθ2)
 The effect of this gyroscopic couple is to turn the disc in the
anticlockwise when viewed from the top, about an axis through
O in the plane of paper.
 Now consider the movement of point D about the polar axis
OP. In this case, OD is axis of spin and OP is the axis of
precession.
 Angular velocity of disc about OD or angular velocity of spin,
= ωsinθ
 and angular velocity of D about OP or angular velocity of
precession
= ωcosθ
5By: Ronak Soni (RDS) Gyroscopic effect on Rotor
6
 If ID is the mass moment of inertia of the disc about the
diametral axis OD, then gyroscopic couple acting on the disc,
CD = ID. ωcosθ.ωsinθ = ½×ID.ω2sin2θ
 The effect of this couple will be opposite to that of CP.
 Resultant gyroscopic couple acting on the disc,
C = CP – CD =1/2×ω2sin2θ (IP – ID)
 This resultant gyroscopic couple will act in the anticlockwise
direction as seen from the top.
 In other words, the shaft tends to turn in the plane of paper
in anticlockwise direction as seen from the top, as a result the
horizontal force is exerted on the shaft bearings.
By: Ronak Soni (RDS) Gyroscopic effect on Rotor
7By: Ronak Soni (RDS) Gyroscopic effect on Rotor
ANY QUERY PLEASE?
8By: Ronak Soni (RDS) Gyroscopic effect on Rotor

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Gyroscopic effect on rotor

  • 1. Presented by: RONAK D. SONI Assistant Professor CHAPTER 1: GYROSCOPE GYROSCOPIC EFFECT ON ROTOR
  • 2. 2By: Ronak Soni (RDS) Gyroscopic effect on Rotor
  • 3. 3  Consider a disc fixed rigidly to a rotating shaft such that the polar axis of the disc makes an angle with the shaft axis, as shown in Figure. By: Ronak Soni (RDS) Gyroscopic effect on Rotor
  • 4. 4  Let the shaft rotates with an angular velocity ω rad/s in the clockwise direction when viewed from the front. A little consideration will show that the disc will also rotate about OX with the same angular velocity ω rad/s.  Let OP be the polar axis and OD the diametral axis of the disc.  Angular velocity of the disc about the polar axis OP or the angular velocity of spin = ωcosθ ... (Component of in the direction of OP)  Since the shaft rotates, therefore the point P will move in a plane perpendicular to the plane of paper. In other words, precession is produced about OD. Angular velocity of the disc about the diametral axis OD or the angular velocity of precession = ωsinθ By: Ronak Soni (RDS) Gyroscopic effect on Rotor
  • 5.  If IP is the mass moment of inertia of the disc about the polar axis OP, then gyroscopic couple acting on the disc, CP = IP. ωcosθ.ωsinθ = ½×IP.ω2sin2θ; (∵ 2 sinθ cosθ=sinθ2)  The effect of this gyroscopic couple is to turn the disc in the anticlockwise when viewed from the top, about an axis through O in the plane of paper.  Now consider the movement of point D about the polar axis OP. In this case, OD is axis of spin and OP is the axis of precession.  Angular velocity of disc about OD or angular velocity of spin, = ωsinθ  and angular velocity of D about OP or angular velocity of precession = ωcosθ 5By: Ronak Soni (RDS) Gyroscopic effect on Rotor
  • 6. 6  If ID is the mass moment of inertia of the disc about the diametral axis OD, then gyroscopic couple acting on the disc, CD = ID. ωcosθ.ωsinθ = ½×ID.ω2sin2θ  The effect of this couple will be opposite to that of CP.  Resultant gyroscopic couple acting on the disc, C = CP – CD =1/2×ω2sin2θ (IP – ID)  This resultant gyroscopic couple will act in the anticlockwise direction as seen from the top.  In other words, the shaft tends to turn in the plane of paper in anticlockwise direction as seen from the top, as a result the horizontal force is exerted on the shaft bearings. By: Ronak Soni (RDS) Gyroscopic effect on Rotor
  • 7. 7By: Ronak Soni (RDS) Gyroscopic effect on Rotor
  • 8. ANY QUERY PLEASE? 8By: Ronak Soni (RDS) Gyroscopic effect on Rotor