CHAPTER I. PRINCIPLE OF STATICS CHAPTER OBJECTIVES 1.Explain the fundamental principle related to Statics of Rigid Bodies. 2.Understand the concepts of force systems. 3.Discuss the introduction of free-body diagram 4. Identify the difference between the vector and scalar quantities. 5.Discuss the parallelogram and triangular law 6.Review the unit of measurement. STATICS OF RIGID BODIES The study of bodies is in equilibrium. This means there are no unbalanced forces on the body, thus the body is at rest or moving at a uniform velocity. DYNAMICS OF RIGID BODIES is the branch of mechanics which deals with the study of bodies in motion. 1.1 FUNDAMENTAL CONCEPTS & DEFINITION f 1.2. FORCE SYSTEM ENGINEERING MECHANICS IS the branch of science which describes and predicts the condition of rest or motion of bodies under the action of forces. FORCE may be defined as the action of one body on another body that affects the state of motion or rest of body. In late 17th century , sir Isaac Newton summarized the effect effects of force in three basic laws. MECHANICS CAN BE DIVIDED INTO THREE BRANCHES: 1. RIGID-BODIES MECHANICS 2. DEFORMABLE-RIGID BODIES 3. FLUID MECHANICS Mechanics of Rigid Bodies: This course deals solely with the mechanics of rigid bodies. A rigid body is a body which does not deform under the influence of forces. .RIGID- BODIES MECHANICS DEALS WITH 1. STATICS 2. DYNAMICS ES11 – STATICS OF RIGID BODIES | FIRST LAW: Any body at rest will remain at rest and any body in motion will move uniformly in a straight line, unless acted upon by the force.( EQUILIBRIUM) PREPARED BY: ENGR. RUTH ANN D. MANINGDING 2 Force A on B F2 Force of B on A F1 A B V b. Action-reaction F3 a. Equilibrium SECOND LAW: The time rate of change of momentum is equal to the force producing it, and the change takes place in the direction in which the force is acting. F=mxa Ground resistance on a building a F b. Accelerated Motion THIRD LAW: For every force of action, there is a reaction that is equal in magnitude, opposite in direction and has the same line of action. ES11 – STATICS OF RIGID BODIES | For example, if a building with a weight W is placed on the ground, we can say that the building is exerting a downward force of W on the ground. However, for the building to remain stable on the resisting ground surface without sinking completely, the ground must resist with an upward force of equal magnitude. If the ground resisted with a force less than W, where R < W, the building would settle. On the other hand, if the ground exerted an upward force greater than W (R > W), the building would rise (levitate). PREPARED BY: ENGR. RUTH ANN D. MANINGDING 3 CHARACTERISTICS OF A FORCE A force is characterized by its (a) magnitude, (b) direction, (c) point of application/position of its line of action a) Point of Application: Defines the point where the force is applied. b) Magnitude: Refers to the quantity of force, a numerical measure of the intensity. c) Direction can be defined by: 1. Line of action refresents an infinite straight line along which the force is acting. Rope pulling on an eyebolt Notes: The sense and direction can be either written as (down and to the right, up and to the left) It can be also expressed in terms of 360 deg.( i,e. 112 degrees, 273 degrees,87.5 degrees). In the later case, one begins with zero and increases clockwise with the direction of the arrow head until 360 is reached. TENSION AND COMPRESSION FORCE a. Tension Force: may be described as the pulling force transmitted through a rope, string or wire b. Compression force: is the action or state of being squished down or pressed down. a. Force in Tension b. Force in Compression 2. SENSE OF A FORCE: specifies direction (positive or negative) in which the force moves along the line of action. Graphically, the sense can be represented by an arrowhead. ES11 – STATICS OF RIGID BODIES | PREPARED BY: ENGR. RUTH ANN D. MANINGDING 4 2. Coplanar- All forces acting in the same plane. RIGID BODIES In Statics, we deal with a body of matter which undergoes no deformation. (a) Original, unloaded box. (b) Rigid body (example: stone) (c) Deformable body (example: foam). Forces in a buttress system Types of forces Force systems are often identified by the type or types of system on which they act. 1. Collinear- All forces acting along the same straight line 3. Coplanar, Parallel- all forces are parallel and act in the same plane. A beam supported by a series of columns ES11 – STATICS OF RIGID BODIES | PREPARED BY: ENGR. RUTH ANN D. MANINGDING 5 4. Coplanar ,Concurrent- all forces intersects at a common point and lie in the same plane 6. Non-coplanar, concurrent-all forces intersects at a common point but do not all lie in the same plane. Loads applied to a roof truss. 5. Non-coplanar, parallel- all forces are parallel to each other, but not all lie in the same plane. One component of a three-dimensional space frame 7. Non-coplanar,non-concurrent skewed - all forces are Column loads in a concrete building. Array of forces acting simultaneously on a house. ES11 – STATICS OF RIGID BODIES | PREPARED BY: ENGR. RUTH ANN D. MANINGDING 6 INTERNAL AND EXTERNAL FORCE EXTERNAL FORCE-the external effect of a force tends to change the state of motion of a body. - are the forces that emanate from the outside the system - are those which are applied to the element such as beam or column. INTERNAL FORCE- the internal effect of a force is to produce stress and deformation in the body on which the forces acts. If we remove the nail and examine the forces acting on it, we discover frictional forces that develop on the embedded surface of the nail to resist the withdrawal force F Withdrawal force on a nail. ES11 – STATICS OF RIGID BODIES | Treating the nail as the body under consideration, we can then say that forces F and S are external forces. They are being applied outside the boundaries of the nail. External forces represent the action of other bodies on the rigid body. Let’s consider just a portion of the nail and examine the forces acting on it. In the frictional force S plus the force R (the resistance generated by the nail internally) resist the applied force F. This internal force R is responsible for keeping the nail from pulling apart. 1.3.Introduction to Free-Body Diagrams One of the most important concepts in mechanics is that of the free-body diagram. A sketch of the isolated body which shows only forces acting upon the body is defined as a free-body diagram. The forces acting on the free body diagram are the action forces, also called the applied forces. The reaction forces are those exerted by the free body upon other bodies. The free body may consist of an entire assembled structure or an isolated part of it. PREPARED BY: ENGR. RUTH ANN D. MANINGDING 7 Vector Quantity has both magnitude and direction. Example: Displacement, velocity, acceleration i1.5.Parallelogram Law and Triangle Law Parallelogram Law The resultant of two forces is the diagonal of the parallelogram formed on the vectors of these forces. Two vectors can be added to give a resultant; this resultant in turn can be added to a third vector i1.4.Scalar and Vector Quantities Introduction Scalar Quantity has only magnitude, but no direction. Example: Length, mass, volume, pressure ES11 – STATICS OF RIGID BODIES | PREPARED BY: ENGR. RUTH ANN D. MANINGDING 8 Triangle Law If two forces are represented by their free vectors placed tip to tail, their resultant vector is the third side of the triangle, the direction of the resultant being from the tail of the first vector to the tip of the last vector. standard unit of length is defined, one can then use it to define distances and geometric properties of a body as multiples of this unit. 2. Mass is a measure of a quantity of matter that is used to compare the action of one body with that of another. This properly manifests itself as a gravitational attraction between two bodies and provides a measure of the resistance of matter to a change in velocity. 3. Time is conceived as a succession of events. Although the principles of statics are time independent, this quantity plays and important role in the study of dynamics. 4. Force . In general time is considered as a "push" or "pull " exerted by one body on another. This interaction can occur when there is direct contact between the bodies, such as a person We will work with two units in Statics: 1.6. UnitS Of Measurement Units are arbitrary names we give to the physical quantities. Four fundamental Physical quantities 1. Length is used to locate the position of a point in space and thereby describe the size of the physical system. Once a ES11 – STATICS OF RIGID BODIES | 1. International System (S.I) The International System of Units, abbreaviated SI after the French “Systѐme International d’ Unitѐs” is a modern version of the metric system which has received worldwide recognition. As shown in Table 1-1, the SI system defines length in meters(m), time in seconds(s), and mass in kilograms (kg). The unit of force, called (N), is derived from F=ma. Thus, 1 newton is equal to a PREPARED BY: ENGR. RUTH ANN D. MANINGDING 9 force required to give 1 kilogram of mass an acceleration of 1m/s2(N=kg. m/s2). 𝑚= 𝑊 𝑔 (𝑔 = 32.2𝑓𝑡 ) 𝑠2 If the weight of a body located at the “standard location” is to be determined in Newton’s, then W=mg must be applied. Here measurements give g=9.80665 m/s2, however, for calculations, the value of g=9.81 m/s2 will be used. Thus, W=mg 1 slug 32.2 lb (g=9.81 m/s2) 1 kg Table 1.1. System Of Units NAME 9.81 N 2.U.S. Costumary (USCS)/ English System In the U.S. customary system of units (FPS) length is measured in feet(ft), time in seconds(s), and force in pounds(lb), in table 1-1.The unit of mass , called a slug, is derived from F=ma.Hence, 1 slug is equal to the amount of matter accelerated at 1 ft/s2 when acted upon by a force of 1 lb(slug=lb.s2/ft).Therefore, if the measurements are made at the “standard location”,where g=32.2 ft/s2, thus ES11 – STATICS OF RIGID BODIES | Internationa l System Of units(SI) U.S. Customary FPS MASS FORCE Meter(m) LENGTH Second(s) TIME Kiligram(kg) Newton(N) (kg.m)/S2 Foot(ft) Second(s) Slug (lb.s2)/ft Pound (lb) Table 1.2. Common Conversion Factors Quantity Force Mass Length Unit of Measurement (FPS) Lb Slug ft Unit of measurement(SI) 4.448 N 14.59Kg 0.3048m PREPARED BY: ENGR. RUTH ANN D. MANINGDING 10 Example1.1: Convert the quantities 300 lb and 52 slug/ft 3 to appropriate SI Units. EXERCISE 1: PROBLEM 1. Determine the weight in N of a cylinder whose mass is 1400 kg. Convert the mass of the cylinder to slugs and then determine its weight in pounds. Solution Using table 1.1. , 1 lb=4.448 N 4.448 𝑁 300 lb.s = 300lb ( 1 𝑙𝑏 ) = 1334.5 N= 1.33 KN ans. Since Slug = 14.59 kg and 1 ft =0.3048 m, then 52𝑠𝑙𝑢𝑔 52 slug/ ft3 =( 𝑓𝑡3 14.59𝑘𝑔 1 𝑓𝑡 )(( 1 𝑠𝑙𝑢𝑔 ) (0.3048) = 26.8(103) Kg/m3 3 ans. PROBLEM#2.Convert each of the following to three significant figures: (a)20 lb.ft to N.m, (b) 450 lb/ft3 to KN/m3, and (c)15 ft/h to mm/s. Problem#3. The density (mass/volume)of aluminum is 5.26 slug/ft3. Determine its density in SI units. Use an appropriate prefix. Proble#4. Water has a density of 1.84 slug/ft3. What is the density expressed in SI units?Express the answer to three significant figures. ES11 – STATICS OF RIGID BODIES | PREPARED BY: ENGR. RUTH ANN D. MANINGDING 11 References: Portrait of Newton at 46 by Godfrey Kneller,1689, https://en.wikipedia.org/wiki/File:GodfreyKnellerIsaacNewton-1689.jpg Barry Onouye, Kevin Kane, C 2012, Statics and Strength of Materials for Architecture and Building Construction 4th edition, Pearson Education, Inc., Prentice Hall, One Lake Street ,Upper Saddle River, New Jersey 07458 R. C. HIBBELER,C 2013, Engineering Mechanics Statics 13th edition, Pearson Education, Inc. Pearson Prentice Hall Upper Saddle River, New Jersey 07458 Singer,Ferdinand L,C 1954,Engineering Mechanics, 2nd edition,Harper & Row, New York, Evanston & London ES11 – STATICS OF RIGID BODIES | PREPARED BY: ENGR. RUTH ANN D. MANINGDING 12