Equilibrium of Rigid Body
Table of Contents
Equilibrium of Rigid Body – what is rigid body , definition of Rigid Body , Rigid Body dynamics , mention the general conditions for equilibrium of a rigid body ,
Rigid Meaning in Hindi – कठोर
Rigid Meaning – not able to be changed or adapted ( fixed , set, firm, inflexible, unalterable , unchangeable , immutable )
EQUILIBRIUM OF RIGID BODY
Free body Diagram
A diagram of a body (or a part of it) which shows all the forces and couples applied on it, and which has all the forces and couples labeled for use in the solution of the problem is called a free-body diagram. Follow these steps to draw a free-body diagram.
1. Select the body (or part of a body) that you want to analyze, and draw it.
2. Identify all the forces and couples that are applied onto the body and draw them on the body. Place each force and couple at the point that it is applied.
3. Label all the forces and couples with unique labels for use during the solution process.
4. Add any relevant dimensions onto your picture.
1. Forces and couples on a free-body diagram
Each force or couple you put on a free-body diagram represents a model of how the body in the free-body diagram is effected by its surroundings. In selecting the forces and couples that are to be applied on the free-body diagram follow these steps:
1. Identify all the forces which come from the interaction of one body with another. Many of the common supports and their effects are shown in Table 5-1 on page 184. Remember that for each way in which a support restricts the free motion of the body, a force or a moment must be applied to the body to impose the restriction on the motion.
2. Apply the weight of the body to its center of gravity (if it is uniform, then apply it to the centroid).
3. Remember that strings and cables can only pull on an object.
4. Remember that internal loads cancel out and should not be put on the free-body diagram.
5 Remember that if you have selected the direction of forces or couples of interaction on one body, then Newton’s 3rd law states that you must apply the forces or couples in the opposite direction on
the other body.
Types of supports and their reactions
Types of reaction and its direction will depend upon the type of support provided.
1.Friction less or smooth surface support
3.Knife edge support
4.Hinged or pinned support
5.Fixed or built in support
1 Roller Supports
Roller supports are free to rotate and translate along the surface upon which the roller rests. The surface may be horizontal, vertical or slopped at any angle. Roller supports are commonly located at one end of long bridges in the form of bearing pads. This support allows bridge structure to expand and contract with temperature changes and without this expansion the forces can fracture the supports at the banks. This support cannot provide resistance to lateral forces. Roller support is also used in frame cranes in heavy industries as shown in figure, the support can move towards left, right and rotate by resisting vertical loads thus a heavy load can be shifted from one place to another horizontally
2 Hinge Supports
The hinge support is capable of resisting forces acting in any direction of the plane. This support does not provide any resistance to rotation. The horizontal and vertical component of reaction can be determined using equation of equilibrium. Hinge support may also be used in three hinged arched bridges at the banks supports while at the center internal hinge is introduced. It is also used in doors to produce only rotation in a door. Hinge support reduces sensitivity to earthquake.
3 Fixed Support
Fixed support can resist vertical and horizontal forces as well as moment since they restrain both rotation and translation. They are also known as rigid support For the stability of a structure there should be one fixed support. A flagpole at concrete base is common example of fixed support In RCC structures the steel reinforcement of a beam is embedded in a column to produce a fixed support as shown in above image. Similarly all the riveted and welded joints in steel structure are the examples of fixed supports Riveted connection are not very much common now a days due to the introduction of bolted joints.
4 Pinned Supports
A pinned support is same as hinged support. It can resist both vertical and horizontal forces but not a moment. It allows the structural member to rotate, but not to translate in any direction. Many connections are assumed to be pinned connections even though they might resist a small amount of moment in reality. It is also true that a pinned connection could allow rotation in only one direction; providing resistance to rotation in any other direction. In human body knee is the best example of hinged support as it allows rotation in only one direction and resists lateral movements. Ideal pinned and fixed supports are rarely found in practice, but beams supported on walls or simply connected to other steel beams are regarded as pinned. The distribution of moments and shear forces is influenced by the support condition.
5 Internal Hinge
Interior hinges are often used to join flexural members at points other than supports. For example in above fig two halves of an arch is joined with the help of internal hinge. In some cases it is intentionally introduced so that excess load breaks this weak zone rather than damaging other structural elements as shown in above image.
The tendency of a force to move the body in the direction of its application a force can tend to rotate a body about an axis. This axis may be any line which is neither intersects nor parallel to the line of the action of the force. This rational tendency of force is know as the moment of force. As a familiar example of the concept of moment, consider the pipe wrench as shown in figure (a).
One effect of the force applied perpendicular to the handle of the wrench is the tendency to rotate the pipe about its vertical axis. The magnitude of this tendency depends on both the magnitude of the force and the effective length d of the wrench handle. Common experience shown that a pull which is not perpendicular to the wrench handle is less effective than the right angle pull. Mathematically this tendency of force (moment) is calculated by multiplying force to the moment
1 Moment about a point
Consider following body (two dimensional) acted by a force F in its plane. The magnitude of moment or tendency of the force to rotate the body about the axis O_O perpendicular to the plane of the body is proportional both to the magnitude of the force and to the moment arm d, therefore magnitude of the moment is defined as the product of force and moment arm.
Moment = Force x moment arm
M = Fd
Where d = moment arm and F = magnitude of force
Moment arm is defined as the perpendicular distance between axis of rotation and the line of action of force.
2 Direction of moment of a force
The direction Mo is specified using the “right-hand rule”. To do this the fingers of the right hand are curled such that they follow the sense of rotation, which would occur if the force could rotate about point O. The thumb then point along the moment axis so that it gives the direction and sense of the moment vector, which is upward and perpendicular to the shaded plane containing F and d.
3 Clock Wise And Anti Clock Wise Moments
The moment are classified as clockwise and anticlockwise moment according to the direction in which the force tends to rotate the body about a fixed point
When the force tends to rotate the body in the same direction in which the hands of clock move is called clockwise moment the clockwise moment is taken as positive or other wise mentioned.
When the force tends to rotate the body in the opposite direction in which the hands of clock move is called anti clockwise moment which is taken as negative or otherwise mentioned.
4 Unit of moment
S.I unit is N.m. (Newton. meter)
F.P.S unit is lb. ft (Pound. foot)
G.G.S unit is dyne.cm (dyne. Centimeter) etc
Example 1: Determine the moment of the force about point “O” for following diagram.
Given Force=100 N
Working formula: – MO=Force x Moment arm.
Sol putt the values in first w, f
Mo= F x r = 100 x 2
Result: – Moment = 200N.m Direction =Clock wise
Example 2: Determine the moment of the force 800 N acting on the frame about points A, B, C and D.
Force = F = 800 N
Required MA=? MB? MC=? MD=?
Moment =force x moment arm. Sol Solve this question step by step Now first consider the Point A. MA = F x r
And MA = 800 x (1.5+1)
MA = 2000 N.m clock wise_______ I Now Moment about B
MB = F x r = 800x 5
MB = 1200 N m clock wise________ (2)
From (1) and (2) it is evidence that when force remain constant then moment varies with moment arm that is moment depends upon moment arm. Similarly it can be proved that moment about any point varies with force when moment arm remain same.
Now consider point C Moment = Force x distance Mc = 800 x 0
Mc = 0. _______ (3)
As the line of action of force passes through point C
that is point of application it shows that the line of action should be perpendicular to the point i.e. “C”
Now consider the point D. MD = F x r.
MD = 800 x 0.5 MD= 400 N.m
MA =2000 N.m clock wise Or
MA = + 200 N.m
MB = 1200 N.m clock wise Or
MB = + 1200 N.m
MC = O.
Mc = O
MD =. 400 N.m anti clock wise
MD = – 400N.m
4 Principle of Moments ( Varignon’s Theorem )
It is stated that the moment of a force about a point is equal to the sum of the moments of the force components about the point. Or the moment produce by the resultant force is equal to the moment produce by the force components.
Mathematically MFo = Σ Mo
Example 3: A 200 N force acts on the bracket as shown determine the moment of force about “A”
Given F=200N θ = 45º
Required MA =?
Solution Resolve the force into components F1 am F2
F1= F cos θ F1=200 cosine 45º
F2= F sin θ F2 = 200 sin 45º
We know that MA = 0
MA = moment produce due to component F1+ moment produce due to component F2.
MA =F1 x r1+ F2 x r2.
Let us consider that clock wise moment is + ve. MA = F1 x r1+ F2 x r2
And MA = – 141.42 x 0.1 + 2.468 x (0.1 +0.1) MA = – 13.648 N
MA = 13 .648 N anti clock wise.
When two parallel forces that have the same magnitude but opposite direction is known as couple. The couple is separated by perpendicular distance. As matter of fact a couple is unable to produce any straight-line motion but it produces rotation in the body on which it acts. So couple can be defined as unlike parallel forces of same magnitude but opposite direction which produce rotation about a specific direction and whose resultant is zero
1 Application of Couple
1. To open or close the valves or bottle head, tap etc
2. To wind up a clock.
3. To Move the paddles of a bicycle
4. Turning a key in lock for open and closing.
2 Couple Arm
The perpendicular distance between the lines of action of the two and opposite parallel forces is known as arm of the couple.
3 Moment of couple or couple moment
The moment of the couple is the product of the force (one of the force of the two equal and opposite parallel forces) and the arm of the couple. Mathematically
Moment of couple = force x arm of couple Moment of couple = F x r
4 Direction of couple
The direction and sense of a couple moment is determined using the right hand rule, here the thumb indicates the direction when the fingers are curled with the sense of rotation caused by the two forces.
5 Classification of Couple
The couplet are classified as clockwise couple and anticlockwise couple
1. Clockwise couple
A couple whose tendency is to rotate the body in a clockwise direction is known as clockwise couple
2. Anticlockwise couple
A couple whose tendency is to rotate the body in anticlockwise direction is known as anticlockwise couple
Example 4: Determine the moment of couple acting on the moment shown.
GivenF1=F2 =90lb F3 = F4 = 120lb.
Required Moment of couple = M=?
Solution The moment of couple can be determined at any point for example at A, B or D.
Let us take the moment about point B
MB = Σ F R.
And MB = -F1 x r1 – F2 x r2 .
And MB = – 90(3) – 120 (1)
MB = – 390 lb ft
Result MB = MA=MD =390 lb .ft counter clock wise.
Moment of couple = 390 lb.ft count clock wise
State varignon’s theorem ? (rigid body)
The algebraic sum of moments due to all forces acting on the object about any point is equal to the moment of their resultant about the same point.
2. Define couple?
Two non collinear parallel forces having same magnitude but opposite direction from a couple.
3. Why the couple moment is said to be a free vector?
Couple moment is said to be a free vector as it can be transferred to any point in the plane without causing any change in its effect on the body.
4. Distinguish between couple and moment?
Moment represents the turning effect of a force where as couple consists of two equal and opposite forces separate by some distance. moment of force various from point to point but moment of a couple is same about any point in the plane.
5. What is meant by force-couple system?
A system of coplanar non concurrent force system acting in a rigid body can be replaced by a single resultant force and couple moment at a point known as force couple system.
6. Can a coplanar non concurrent system with zero resultant force necessarily be in equilibrium?
A coplanar non concurrent system with zero resultant force is not necessarily In equilibrium as it can have a non zero resultant moment.
7.When is moment of force zero about a point?
The moment of force about a point is zero its line of action passes through that point.
8.When is moment of force maximum about a point ?
Moment of force is maximum about a point when,
i)Its applied at maximum result from the point and,
ii)It is applied perpendicular to the line joining the point to the point of application of force.
9.When is moment of force zero about a line?
Moment of force about a line is zero when,
i)Force is parallel to that line or,
ii)Line of action of force intersects that line.
10. Explain free body diagram with one example?
Free body diagram is the isolated diagram of an object\system of objects\any point in the system in which all forces at couple moment acting on it are shown including support reactions example: consider a ladder of weight W having rollers at it’s end’s as shown in figure.
11. State the necessary and sufficient conditions for equilibrium of rigid body in two dimensions?
The necessary and sufficient conditions for equilibrium of rigid body in two dimensions are:
1)algebraic sum of horizontal components of all forces acting on the body is must be zero,
2)Algebraic sum of vertical components all forces acting on the body is must be zero,
3)Algebraic sum of moments due to all forces and couple moments acting the body is in must be zero.
12.Write the equation of equilibrium of a rigid body?
The three equations of a rigid body are:
13.Write the conditions equilibrium of a system of parallel force acting in a plane ?
The two conditions of equilibrium of a system of parallel forces acting in a plane are :
1)Algebraic sum of all forces must be zero,
2)Algebraic sum of moments due to all forces about any point must be zero.
14.What are the reactions at a fixed support of a plane beam that are possible?
The reaction at fixed support of a plane beam consist of ,
1)A reaction force in the plane which can be represented by it’s two components(Generally taken to be horizontal and vertical)&,
2)A reaction moment.
15.How many scalar equations can be obtained for equilibrium of rigid body in three dimensions?
Six scalar equations can be obtained for equilibrium of a rigid body in three dimensions.
1. State Varignon’s theorem
2. What is a couple? what is a moment of a couple?
3. A force vector F has the components Fx = 150N, Fy= -200N and Fx = 300N. Determine the magnitude F and the angle made by the force with coordinate axes.
4. Sketch the different types of supports.
5. Write down the conditions of equilibrium of a particle in space
6. A force vector of magnitude 100N is represented by a line of coordinates A (1, 2, 3) and B (5, 8, 12). Determine components of the force along X, Y and Z axes.
7. Explain will you reduce a force into an equivalent force-couple system with an example.
9. Draw Compute the moment of the 100 N force about point A and B
1. Four forces act on a 700mm X 375mm plate as shown in fig. a) Find the resultant of these forces b) Locate the two points where the line of action of the resultant intersects the edge of the plate.
2. Four coplanar non concurrent non parallel forces act on a square plate of side 2m as shown in fig. Locate the resultant force.
3. In figure below, two forces act on a circular disc as shown. If the resultant moment of all these forces about point D on the disc is zero, determine: a) Magnitude of force P (b) Magnitude of the resultant of two forces (c) The point on the Y-axis through which the line of action of the resultant passes through.
4. Four forces act on a square of side 1 m as shown in fig. Reduce the force system into an equivalent force – couple system at A.
5. Reduce the system of forces shown in fig.5 to a force – couple system at A.
6. Blocks A and B of weight 200N and 100N respectively, rest on a 30 inclined plane and are attached to the post which is held perpendicular to the plane by force P, parallel to the plane, as shown in fig. Assume that all surfaces are smooth and that the cords are parallel to the plane. Determine the value of P. Also find the Normal reaction of Blocks A and B.
8. A Uniform meter rod AB, assumed rigid of mass 0.5 kg is suspended from its ends in an inclined position and a mass of 1 kg is suspended from a point D, as shown in fig. determine the tension in each string. Where should the suspended mass be placed in order to get equal tension in the strings.
9. A rod AB of weight 200 N is supported by a cable BD and the corner of wall and floor surface as shown in fig. Find the reaction at A and tension in the cord.
10. Find reactions at points A & B