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Free and constrained bodies. A body treats as free if its displacements are not

2. The helicopter is free.

Слайды и текст этой презентации

Слайд 1Free and constrained bodies.
A body treats

as free if its displacements are not restricted by any

other bodies, in opposite case a body is constrained.


Examples of free body:

The airplane in the sky is free body.

Free and constrained bodies.	    A body treats as free if its displacements are not

Слайд 22. The helicopter is free.

2. The helicopter is free.

Слайд 33. Bird treats as free body.

3. Bird treats as free body.

Слайд 4 Examples of constrained body.
1. The motion of the balloon is

restricted by four cords.
Cord 1
Cord 2
Cord 3
Cord 4

Examples of constrained body.1. The motion of the balloon is restricted by four cords.Cord 1Cord 2Cord 3Cord

Слайд 5The motion of the yellow rectangular plate ABCD is restricted

by hinges at A and B and is supported by

pined joint link DE.









The motion of the yellow rectangular plate ABCD is restricted by hinges at A and B and

Слайд 6The bodies that restrict the motion of some body are

called constraints imposed upon the body.
Mechanical effect of a constraint

action is the same as action of a force. Therefore the constraints can be replaced by forces that are called reactions.
Axiom of constraint eliminating: any constrained body can be considered free if constraints applied to the body are mentally eliminated and replaced with the corresponding reaction forces.
The bodies that restrict the motion of some body are called constraints imposed upon the body.Mechanical effect

Слайд 7Forces classification: applied forces and reactions
In mechanics all forces acting

on the body or mechanical system are subdivided into two

classes in two ways.
In the first way forces are subdivided into applied (given) and reactive forces. Active (applied) forces are independent from constraints and usually it is supposed that active forces are given in statement of a problem.

Forces classification: applied forces and reactions 	In mechanics all forces acting on the body or mechanical system

Слайд 8 Some reactions at supports and connections for two-dimensional structure
Smooth

surfaces

Some reactions at supports and connections for two-dimensional structure Smooth surfaces

Слайд 9Weightless flexible, nonstretchable cord or
weightless rigid link
Sliding joint or roller

support

Weightless flexible, nonstretchable cord orweightless rigid linkSliding joint or roller support

Слайд 10Pinned joint

Pinned joint

Слайд 11Collar or sliding support
Double stage sliding support
Fixed support, сlamped joint

Collar or sliding supportDouble stage sliding supportFixed support, сlamped joint

Слайд 13Some reactions at supports and connections for three-dimensional structure
Ball-and-socket joint

and footstep bearing

Some reactions at supports and connections for three-dimensional structureBall-and-socket joint and footstep bearing

Слайд 14Hinge
Bearing supports

HingeBearing supports

Слайд 15Fixed support

Fixed support

Слайд 17In the second way forces are subdivided into external and

internal.
Forces are called external with respect to a given object

(body or mechanical system) if they are produced by particles and other bodies not included into a given object (by external objects). Forces of interaction between particles or parts of the given object are called internal.
In the second way forces are subdivided into external and internal.Forces are called external with respect to

Слайд 19Concurrent force system
If lines of action of all forces of

a system intersect at the same point the force system

is called concurrent.
Concurrent force system resultant
Concurrent force system is equivalent to single force (resultant). Resultant is equal to the vector sum of the forces of system. Resultant is applied at the point of intersection all forces lines of action.
Concurrent force system 	If lines of action of all forces of a system intersect at the same

Слайд 20The composition of forces can be accomplished:

geometrically, constructing a vector

force polygon

analytically, summing projections of all forces

on
selected coordinate axes:

The composition of forces can be accomplished:geometrically, constructing a vector force polygon   analytically, summing projections

Слайд 21Equilibrium conditions for the concurrent force system
To be balanced any

concurrent force system must have zero resultant.
Analytical conditions of concurrent

force system equilibrium

In geometrical form it can be formulated as follows: closure of the polygon of forces is a necessary and sufficient condition for the concurrent force system to be in balance.

Equilibrium conditions for the concurrent force systemTo be balanced any concurrent force system must have zero resultant.Analytical

Слайд 22Problems of statics
There are two general problems of rigid body

statics:
The composition of forces and the reduction of the force

system acting on rigid bodies to the simplest possible form.
The determination of conditions for the equilibrium of the force system acting on rigid bodies.
Problems of staticsThere are two general problems of rigid body statics:The composition of forces and the reduction

Слайд 23Moment of a force about a point

Moment of a force about a point

Слайд 24Moment of a force about an axis
The projection of the

moment about the point onto an axis that passes through

the point is called the moment of force about the axis




Moment of a force about an axisThe projection of the moment about the point onto an axis

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