Download presentation

Presentation is loading. Please wait.

Published byStuart Bevel Modified about 1 year ago

1
Basic Biomechanics BIOMECHANICS: BIO = living, MECHANICS = forces & effects The application of mechanics to the living organism involves the principles of anatomy and physics in the descriptions and analysis of movement Chaitali Prabhudesai

2
Basic Biomechanics Mechanics-study of forces and motions produced by their action. Biomechanics-apply that to the structure and function of the human body.

3
Basic Biomechanics Anatomical Reference position : Erect standing position with all body parts, including the palms of the hands, facing forward; considered the starting position for body segment movements Chaitali prabhudesai

4
Basic Biomechanics Anatomical Reference Planes: Cardinal planes – 3 imaginary perpendicular reference planes that divide the body in half by mass Sagittal plane(rotates about frontal axis) Frontal plane(rotates about sagital axis) Transverse plane(rotates about longitudinal axis) Anatomical Reference Axis: Longitudinal axis, Frontal Axis,Sagittal Axis Chaitali Prabhudesai

5

6
Force Force : Force is a mechanical disturbance which when applied to a body may produce a chance in the existing state of a body Thus a force when acting on a object,can deform the object, change its state of motion or both But a force will not always cause a change in motion E.g. if we sit on a chair then our wt is the force acting on the chair, but the chair remains stationary- stationary force Chaitali Prabhudesai

7
Properties Force is a vector quantity Thus in order to describe a force we need to know 1)pt of application 2)line of action of force 3)sense along which the force is acting 4)Magnitude Forces can be added graphically and trigonometrically Dimensions and units: F=ma,unit-newton/kg-m/s^2 Chaitali Prabhudesai

8
Types Of forces There are some forces constantly present in nature 1) Gravitational Force: Every object on the surface of the earth or near it, is attracted towards the center of center of the earth F=mg Example: Gravitational force on a planet X is 40% of that found on the earth. If the person weighs N on the earth, what is the persons weight on planet X? What is the persons mass on the earth and planet X? Chaitali Prabhudesai

9
Types Of forces Gravitational force on earth = 9.81 Gravitational force on planet X=0.4*9.81=3.92 Mass of the person on earth, planet X= 667.5/9.81=68 Weight of the person on planet X=68*3.92= Chaitali prabhudesai

10
Types Of forces 2)Reaction : A force generated when an object applies a force on another object in contact with it 3)Friction : When two bodies are in surface contact with each other a force is generated as one of them starts moving over the other. The force of friction is the one which opposes the force causing movement of the body on the surface of the other Chaitali Prabhudesai

11
4)Inertia : Inertia force is present in every object which tends to resist any attempt to change its existing state of rest or motion by application of force from outside

12
Law of Acceleration-the amount of acceleration depends on the strength of the force applied to an object.

13
Types Of forces Forces can also be classified according to their effect on the bodies upon which they are applied 1)External & Internal: External forces are commonly known forces like while kicking a football, hammer a nail, a external force is applied on the football, nail 2)Normal and Tangential forces: If a force is applied in a direction perpendicular to the surface then it is called a normal force A tangential force is that applied on the surface in the direction of the surface.eg:Frictional force. 3)Tensile and compressive forces: Tensile force is the one which stretches or elongates a body.eg:rubber band,muscles contract to produce tensile force that pulls together the bones to which they are attached. Compressive forces:These are the forces which shrink the body upon which they are acting. Eg: Poking a needle into an inflated balloon. Chaitali Prabhudesai

14
Resolution Resolution of a force implies breaking a force in the components,such that the components combined together will have the same effect as the original force The force f acting at an angle theta can be resolved into two forces F1 and F2. The components Fx and Fy are known as the perpendicular components of force since they are perpendicular to each other F ѳ FF ѳ ѳ F1 F2 Fx Fy Chaitali Prabhudesai

15
Force Systems System of forces tells us the arrangement of forces and is classified as follows: system of forces coplanarnoncoplanar concurrentparallelgeneral Chaitali Prabhudesai

16
Coplanar force system In this arrangement all forces lie in one plane y x f1 f2 f3 f4 Chaitali Prabhudesai

17
Coplanar force system A)Concurrent: In this system all the forces meet at a point. E.g. A lamb hanging from two strings T1T2 W A Chaitali Prabhudesai

18
Coplanar force system two or more forces act from the same common point but pull in different directions Chaitali prabhudesai

19
p1 p2 p3 w R1 Chaitali Prabhudesai B)Parallel force system: In these forces line of action of forces are parallel E.g. 3 people sitting on a bed

20
coplanar force system General system: Also known as a non concurrent & non parallel system, has forces which do not meet at a single point, nor are parallel to each other F1 F3 F4 F2

21
Non coplanar force system When the forces acting on a system do not lie in a single plane, they are termed as non coplanar forces or space forces y x z f1 f3 f2 Chaitali Prabhudesai

22
Combination of forces Combination means to combine the forces acting in a system into a single force which has same effect as the no of forces acting together Such a force is known as the resultant of the system Finding the resultant helps us to understand the effect of forces on the system and may form an important step to solution of engineering problems Chaitali Prabhudesai

23
Resultant of concurrent force system Parallelogram law of forces : If two forces acting simultaneously on a body at a point are represented in magnitude and direction by 2 adjacent sides of a parallelogram then their resultant is represented in magnitude and direction by the diagonal of the parallelogram which passes through the point of intersection of the two sides representing the forces. Mathematically R^2=(p^2+q^2+2pqcos ά) & tan θ= q sin ά p+q cos ά p q ά p A B D c q R άθ Chaitali Prabhudesai

24
Resultant of concurrent force system Example: Find the magnitude of the forces p & q such that if they act at right angles their resultant is √34.If they act at an angle of 60 their resultant is 7 N p2+ q2+2pqcos 90 =34 p2+ q2=34………………………..(1) p2+ q2+2pqcos 60=49 p2+ q2+pq=49,so pq=15,Thus p=15/q…………….(2) Put (2) in (1) P=,q= Chaitali Prabhudesai

25
Resultant of concurrent force system Method of resolution: 1)Resolve the inclined forces if any in horizontal x direction and vertical y direction 2)Add up the horizontal forces to get ∑Fx 3)Add up the vertical forces to get ∑Fy The resultant force R=√(∑Fx^2+∑Fy^2) Tan θ= ∑Fy/ ∑Fx Example: Find the resultant of 4 concurrent forces acting on a particle P N 300 N 500 N 250 N P Chaitali Prabhudesai

26
Resultant of parallel force system Since in a parallel system the forces are in one direction they can be added up using a sign convention for the sense of force R=∑F Chaitali Prabhudesai

27
Equilibrium Of forces A body is said to be in equilibrium if it is in the state of rest or uniform motion. For the body to be in equilibrium the resultant of the system should be zero. This implies: 1)The sum of all forces should be zero ∑F=0 2)The sum of all moments should be zero ∑M=0 Chaitali Prabhudesai

28
Equilibrium Of forces Eg: skier moving at constant speed down a slope: Contact force from Earth on skier Gravitational force from Earth on skier Frictional force from Earth on skier Chaitali prabhudesai

29

30
Equilibrium of a two force body If only two forces act on a member and the member is in equilibrium then the 2 forces would be of equal magnitude, opposite in direction and collinear Such members are referred to as 2 force members and their identification is useful in solution of equilibrium problems Chaitali Prabhudesai

31
Equilibrium of a two force body A frame consist of three members Af,BC and DE Member BC is isolated Let Rb and Rc be the pin reactions at points B and c respectively Since only 2 forces are acting on a member BC it is a 2 force member Therefore Rb=Rc in magnitude, opposite in direction and collinear Rb Rc C F B E D A W C C B B Chaitali Prabhudesai

32
Equilibrium of a three force body IF three coplanar forces act on a member and the member is in equilibrium then the forces would be either concurrent or parallel Concurrent: Parallel: p C BA Chaitali Prabhudesai Ra Rb

33
Equilibrium of concurrent forces Conditions of equilibrium for concurrent system of forces in a plane: ∑Fx=0 ∑Fy=0 Or ∑Fx=0 ∑Ma=0 or ∑Ma=0 ∑Mb=0 Chaitali Prabhudesai

34
Equilibrium of concurrent forces Triangle law of forces: When a set of 3 concurrent forces are in equilibrium, they can be represented in magnitude and direction with 3 sides of a triangle Conversely when 3 concurrent forces can be represented by the 3 sides of a triangle, they are in equilibrium. Q P R P R Q Chaitali Prabhudesai

35
Equilibrium of multiple coplanar forces Polygon Law of Forces: If a set of multiple coplanar forces acting concurrently on a body are in equilibrium then they can be represented in magnitude and direction by the sides of a polygon having number of sides equal to number of forces. Thus 5 forces can be represented by a pentagon and so on. Chaitali Prabhudesai p q r s t q r s tp

36
Equilibrium of parallel forces A force has a tendency to rotate a body about a point. This tendency is known as its moment. Moment is a vector quantity. Magnitude of moment is given by following expression: M A= F.d where F=mg, d=perpendicular distance of the force from the moment centre, M A= magnitude of moment about pt A Chaitali Prabhudesai

37
Conditions for Equilibrium: ∑F=0 ∑Ma=0 where a is any pt on the plane but not on y-axis Or or ∑Ma=0 Where a and b are any 2pts on the plane but line AB is not parallel to the forces ∑Mb=0 Chaitali prabhudesai

38
Equilibrium of general force system Conditions for Equilibrium of a general force system: ∑Fx=0 ∑Fy=0 ∑Ma=0 Where a is any pt on the plane but not on y-axis Or ∑F=0 ∑Ma=0 ∑Mb=0 Chaitali Prabhudesai

39
Lami’s Theorem If three concurrent forces are in equilibrium then the magnitude of each force is proportional to the sine of the angle between the other two forces in the system. F1 F3 F2 ѳ3 ѳ1 ѳ2 Chaitali Prabhudesai

40
Lami’s Theorem F1 = F2 = F3 Sin(180-ѳ1) Sin(180-ѳ2) Sin(180-ѳ3) F1 = F2 = F3 Sin ѳ1 Sinѳ2 Sin ѳ3 F3 F2 F1 ѳ1 ѳ2 ѳ3 Chaitali Prabhudesai

41
Equilibrium Stable Equilibrium: If a rigid body in the state of rest is slightly disturbed from its initial position, return to its initial position of equilibrium then it is said to be in stable state of equilibrium Chaitali prabhudesai

42
Equilibrium Unstable Equilibrium: If a rigid body in the state of rest is slightly disturbed from its initial position, does not return to its initial position of equilibrium then it is said to be in unstable state of equilibrium Chaitali prabhudesai

43
Equilibrium Neutral Equilibrium: If a rigid body in the state of rest is slightly disturbed from its initial position, remains in the state of rest at the new position then it is said to be in neutral equilibrium Chaitali prabhudesai

Similar presentations

© 2016 SlidePlayer.com Inc.

All rights reserved.

Ads by Google