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BRIEF INTRODUCTION ON
BALANCING
PREPARED BY :- GONDALIYA KAUSHIK
WHAT IS BALANCING ??
• Often an unbalance of forces is produced in rotary or reciprocating machinery due
to the inertia forces associated with the moving masses.
• Balancing is the process of designing or modifying machinery so that the
unbalance is reduced to an acceptable level and if possible is eliminated entirely.
• Often an unbalance of forces is produced in rotary or reciprocating machinery due
to the inertia forces associated with the moving masses.
• Balancing is the process of designing or modifying machinery so that the
unbalance is reduced to an acceptable level and if possible is eliminated entirely.
CONT…
• This is a disturbing force on the axis of rotation, the magnitude of which is
constant but the direction changes with the rotation of the mass.
• In a revolving rotor, the centrifugal force remains balanced as long as the center of
the mass of the rotor lies on the axis of the shaft.
• When the center of mass does not lie on the axis or there is an eccentricity, an
unbalanced force is produced.
WHY BALANCING IS NECESSARY ??
• The high speed of engines and other machines is a common phenomenon now-a-
days.
• It is, therefore, very essential that all the rotating and reciprocating parts should be
completely balanced as far as possible.
• If these parts are not properly balanced, the dynamic forces are set up.
• These forces not only increase the loads on bearings and stresses in the various
members, but also produce unpleasant and even dangerous vibrations.
BALANCING OF ROTATING MASSES
• Static and dynamic balancing
• Balancing of single rotating mass by balancing masses in same plane and in different
planes.
• Balancing of several rotating masses by balancing masses in same plane and in
different planes.
• Whenever a certain mass is attached to a rotating shaft, it exerts some centrifugal
force, whose effect is to bend the shaft and to produce vibrations in it.
• In order to prevent the effect of centrifugal force, another mass is attached to the
opposite side of the shaft, at such a position so as to balance the effect of the
centrifugal force of the first mass.
CONT….
• This is done in such a way that the centrifugal force of both the masses are made to
be equal and opposite.
• The process of providing the second mass in order to counteract the effect of the
centrifugal force of the first mass, is called balancing of rotating masses.
Balancing of Rotating Masses
 The following cases are important from the subject point of view:
1. Balancing of a single rotating mass by a single mass rotating in the
same plane.
2. Balancing of a single rotating mass by two masses rotating in
different planes.
3. Balancing of different masses rotating in the same plane.
4. Balancing of different masses rotating in different planes.
Balancing of a Single Rotating Mass By a Single
Mass Rotating in the Same Plane
Consider a disturbing mass m1 attached to a shaft rotating at ω rad/s.
• Let r1 be the radius of rotation of the mass m1 (i.e. distance between the axis of
rotation of the shaft and the centre of gravity of the mass m1).
• We know that the centrifugal force exerted by the mass m1 on the shaft,
• This centrifugal force acts radially outwards and thus produces bending moment on
the shaft.
• In order to counteract the effect of this force, a balancing mass (m2) may be
attached in the same plane of rotation as that of disturbing mass (m1) such that the
centrifugal forces due to the two masses are equal and opposite.
CONT…
• In order to counteract the effect of this force, a balancing mass (m2) may be attached in the same plane of
rotation as that of disturbing mass (m1) such that the centrifugal forces due to the two masses are equal and
opposite.
CONT..
Balancing of a Single Rotating Mass By Two
Masses Rotating in Different Planes
• In the previous arrangement for balancing gives rise to a couple which tends to rock the shaft
in its bearings.
• Therefore in order to put the system in complete balance, two balancing masses are placed in
two different planes, parallel to the plane of rotation of the disturbing mass, in such a way that
they satisfy the following two conditions of equilibrium.
• The following two possibilities may arise while attaching the two balancing masses :
1. The plane of the disturbing mass may be in between the planes of the two balancing masses.
2. The plane of the disturbing mass may lie on the left or right of the two planes containing the
balancing masses.
CONT…
1. When the plane of the disturbing mass lies in between the
planes of the two balancing masses
• Consider a disturbing mass m lying in a plane A to be balanced by
two rotating masses m1 and m2 lying in two different planes L and M
as shown in Fig.
• Let r, r1 and r2 be the radii of rotation of the masses in planes A, L
and M respectively.
CONT…
Subject presiontation of dynamics of motion
CONT…
2. When the plane of the disturbing mass lies on one end of the
planes of the balancing masses
• In this case, the mass m lies in the plane A and the balancing masses
lie in the planes L and M, as shown in Fig. 2.
Subject presiontation of dynamics of motion
Subject presiontation of dynamics of motion
Balancing of Several Masses Rotating in Different Planes
• When several masses revolve in different planes, they may be
transferred to a reference plane (briefly written as R.P.), which may be
defined as the plane passing through a point on the axis of rotation and
perpendicular to it.
• The effect of transferring a revolving mass (in one plane) to a
reference plane is to cause a force of magnitude equal to the
centrifugal force of the revolving mass to act in the reference plane,
together with a couple of magnitude equal to the product of the force
and the distance between the plane of rotation and the reference plane.
CONT…
•Let us now consider four masses m1, m2, m3 and m4 revolving in
planes 1, 2, 3 and 4 respectively as shown in Fig. (a).
•The relative angular positions of these masses are shown in the end
view [Fig. (b)].
The magnitude of the balancing masses mL and mM in planes L and
M may be obtained as discussed below :
Subject presiontation of dynamics of motion
Subject presiontation of dynamics of motion

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Subject presiontation of dynamics of motion

  • 2. WHAT IS BALANCING ?? • Often an unbalance of forces is produced in rotary or reciprocating machinery due to the inertia forces associated with the moving masses. • Balancing is the process of designing or modifying machinery so that the unbalance is reduced to an acceptable level and if possible is eliminated entirely. • Often an unbalance of forces is produced in rotary or reciprocating machinery due to the inertia forces associated with the moving masses. • Balancing is the process of designing or modifying machinery so that the unbalance is reduced to an acceptable level and if possible is eliminated entirely.
  • 3. CONT… • This is a disturbing force on the axis of rotation, the magnitude of which is constant but the direction changes with the rotation of the mass. • In a revolving rotor, the centrifugal force remains balanced as long as the center of the mass of the rotor lies on the axis of the shaft. • When the center of mass does not lie on the axis or there is an eccentricity, an unbalanced force is produced.
  • 4. WHY BALANCING IS NECESSARY ?? • The high speed of engines and other machines is a common phenomenon now-a- days. • It is, therefore, very essential that all the rotating and reciprocating parts should be completely balanced as far as possible. • If these parts are not properly balanced, the dynamic forces are set up. • These forces not only increase the loads on bearings and stresses in the various members, but also produce unpleasant and even dangerous vibrations.
  • 5. BALANCING OF ROTATING MASSES • Static and dynamic balancing • Balancing of single rotating mass by balancing masses in same plane and in different planes. • Balancing of several rotating masses by balancing masses in same plane and in different planes. • Whenever a certain mass is attached to a rotating shaft, it exerts some centrifugal force, whose effect is to bend the shaft and to produce vibrations in it. • In order to prevent the effect of centrifugal force, another mass is attached to the opposite side of the shaft, at such a position so as to balance the effect of the centrifugal force of the first mass.
  • 6. CONT…. • This is done in such a way that the centrifugal force of both the masses are made to be equal and opposite. • The process of providing the second mass in order to counteract the effect of the centrifugal force of the first mass, is called balancing of rotating masses.
  • 7. Balancing of Rotating Masses  The following cases are important from the subject point of view: 1. Balancing of a single rotating mass by a single mass rotating in the same plane. 2. Balancing of a single rotating mass by two masses rotating in different planes. 3. Balancing of different masses rotating in the same plane. 4. Balancing of different masses rotating in different planes.
  • 8. Balancing of a Single Rotating Mass By a Single Mass Rotating in the Same Plane Consider a disturbing mass m1 attached to a shaft rotating at ω rad/s. • Let r1 be the radius of rotation of the mass m1 (i.e. distance between the axis of rotation of the shaft and the centre of gravity of the mass m1). • We know that the centrifugal force exerted by the mass m1 on the shaft, • This centrifugal force acts radially outwards and thus produces bending moment on the shaft. • In order to counteract the effect of this force, a balancing mass (m2) may be attached in the same plane of rotation as that of disturbing mass (m1) such that the centrifugal forces due to the two masses are equal and opposite.
  • 9. CONT… • In order to counteract the effect of this force, a balancing mass (m2) may be attached in the same plane of rotation as that of disturbing mass (m1) such that the centrifugal forces due to the two masses are equal and opposite.
  • 11. Balancing of a Single Rotating Mass By Two Masses Rotating in Different Planes • In the previous arrangement for balancing gives rise to a couple which tends to rock the shaft in its bearings. • Therefore in order to put the system in complete balance, two balancing masses are placed in two different planes, parallel to the plane of rotation of the disturbing mass, in such a way that they satisfy the following two conditions of equilibrium. • The following two possibilities may arise while attaching the two balancing masses : 1. The plane of the disturbing mass may be in between the planes of the two balancing masses. 2. The plane of the disturbing mass may lie on the left or right of the two planes containing the balancing masses.
  • 12. CONT… 1. When the plane of the disturbing mass lies in between the planes of the two balancing masses • Consider a disturbing mass m lying in a plane A to be balanced by two rotating masses m1 and m2 lying in two different planes L and M as shown in Fig. • Let r, r1 and r2 be the radii of rotation of the masses in planes A, L and M respectively.
  • 15. CONT… 2. When the plane of the disturbing mass lies on one end of the planes of the balancing masses • In this case, the mass m lies in the plane A and the balancing masses lie in the planes L and M, as shown in Fig. 2.
  • 18. Balancing of Several Masses Rotating in Different Planes • When several masses revolve in different planes, they may be transferred to a reference plane (briefly written as R.P.), which may be defined as the plane passing through a point on the axis of rotation and perpendicular to it. • The effect of transferring a revolving mass (in one plane) to a reference plane is to cause a force of magnitude equal to the centrifugal force of the revolving mass to act in the reference plane, together with a couple of magnitude equal to the product of the force and the distance between the plane of rotation and the reference plane.
  • 20. •Let us now consider four masses m1, m2, m3 and m4 revolving in planes 1, 2, 3 and 4 respectively as shown in Fig. (a). •The relative angular positions of these masses are shown in the end view [Fig. (b)]. The magnitude of the balancing masses mL and mM in planes L and M may be obtained as discussed below :