DYNAMICS OF MACHINES To know the purpose for

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DYNAMICS OF MACHINES • To know the purpose for which the m/c is needed.

DYNAMICS OF MACHINES • To know the purpose for which the m/c is needed. • To develop concept design. • To analyze the motion involved - Kinematics • To calculate & analyze the forces and torques required for producing the motion - Kinetics • To give physical shape to the components. - Machine Design

STATIC FORCE ANALYSIS IN MACHINES • To evaluate the forces acting on the machine

STATIC FORCE ANALYSIS IN MACHINES • To evaluate the forces acting on the machine members at a particular configuration. • Each configuration is considered as system of rigid bodies in static equilibrium under the action of external forces. • Helps in finding load carried by each part of the machine during cycle of its operation

TYPES OF FORCES • Applied forces : Gas, hydraulic & pneumatic forces etc. .

TYPES OF FORCES • Applied forces : Gas, hydraulic & pneumatic forces etc. . Electrical, magnetic & gravity forces • Constraint forces : Reaction forces. • Friction forces. • Inertia forces. Due to mass of accelerating parts

Condition for static equilibrium F 1 F 2 • ∑ Fi =0 F 5

Condition for static equilibrium F 1 F 2 • ∑ Fi =0 F 5 M/c part CG • ∑ Mi = 0 F 4 F 3

EQUATIONS FOR STATIC EQUILIBRIUM Fi = 0 M i= 0

EQUATIONS FOR STATIC EQUILIBRIUM Fi = 0 M i= 0

EQUILIBRIUM OF TWO FORCE AND THREE FORCE MEMBERS Two force member in equilibrium F

EQUILIBRIUM OF TWO FORCE AND THREE FORCE MEMBERS Two force member in equilibrium F 2 F 1

THREE FORCE MEMBER IN EQUILIBRIUM F 1 F 2 F 1 O F 3

THREE FORCE MEMBER IN EQUILIBRIUM F 1 F 2 F 1 O F 3 F 2 O F 3

STATIC FORCE ANALYSIS IN SLIDER-CRANK MACHANISM A 3 2 4 O 2 P 1

STATIC FORCE ANALYSIS IN SLIDER-CRANK MACHANISM A 3 2 4 O 2 P 1 B FBDof Link 2 C 12 2 F 34 P F 12 4 F 34 FBDof Link 3 F 14 P 3 FBDof Link 4 B F 43 F 23 A

STATIC FORCE ANALYSIS IN 4 -BAR MECHANISM F 34 A B 3 C 2

STATIC FORCE ANALYSIS IN 4 -BAR MECHANISM F 34 A B 3 C 2 O P 4 4 P F 14 F 34 O 2 O 4 F 43 3 F 32 C 12 h F 12 F 23 O 2 C 12 = F 32 X h

P O 2 6 5 C B 3 P A 2 6 C 5

P O 2 6 5 C B 3 P A 2 6 C 5 O 2 4 F 16 1 P O 4 F 56 F 16 F 56

F 65 5 F 45 O C F 54 LINE OF OF A F

F 65 5 F 45 O C F 54 LINE OF OF A F 3 4 F 54 CTIO N 4 AC F 14 OF OF F 34 NE LI 3 ON TI F 32 A 2 O 2 F 12 C 12 F 43 3 F 23 F 14

Inertia force - -Inertia torque - ma Iα

Inertia force - -Inertia torque - ma Iα

D’ Alemberts principle In order to find the effect of inertia of the actual

D’ Alemberts principle In order to find the effect of inertia of the actual link on the forces transmitted to the adjacent links of a mechanism, the actual link may be replaced by a rigid mass-less link to which inertia force F i = -ma is applied. The mass-less link is then under equilibrium under systems of forces along with inertia force.