Week%2002
Course Introduction
Instructor: Dr. Uzair Khaleeq uz Zaman
Course Code: DMTS - College of E&ME
Course Title: ME 113 – ENGINEERING MECHANICS I: STATICS
Week: 02
Chapter 2: Force Vectors
Author: Dr. Uzair Khaleeq uz Zaman
Outline
Scalars & Vectors
Vector Operations
Vector Addition of Forces
Addition of a System of Coplanar Forces
Cartesian Vectors
Addition of Cartesian Vectors
Position Vectors
Force Vector Directed along a Line
Dot Product
Vectors
Types of Vectors
Free Vector:
Action not confined to a line; defined by magnitude and direction.
Example: Movement of a body without rotation.
Sliding Vector:
Unique line of action, but no specific point of application; described by magnitude, direction, and line of action.
Example: External force on a rigid body.
Fixed Vector:
Unique point of application; described by magnitude, direction, and point of application.
Vector Operations
Basic Operations
Multiplication & Division by a Scalar:
Positive scalar: increases magnitude.
Negative scalar: decreases magnitude and reverses direction.
Vector Addition
Parallelogram Law:
Vectors A and B combined to form resultant R = A + B.
Steps:
Join tails of A and B.
Draw lines from heads of A and B parallel to opposite vectors.
Intersection point defines resultant vector R.
Triangle Rule:
Vectors A and B added in head-to-tail configuration.
Resultant R extends from tail of A to head of B.
Commutative property: R = A + B = B + A.
Collinear Case:
If A and B are collinear, thence R = A + B becomes scalar addition.
Vector Subtraction
Defined as R' = A – B = A + (-B); follows addition rules.
Zero Vector
Resultant of a vector subtracted from itself: P - P = 0 (Null Vector).
Vector Addition of Forces
Finding Resultant Forces
Finding Resultant Force:
Two force components F1 and F2 lead to resultant force FR = F1 + F2.
Applying Laws:
Use parallelogram construction or the triangle rule with laws of cosines or sines.
Resolving Forces
Force resolved into two components with respect to specific axes (u and v).
Addition of Several Forces
Use successive applications of the parallelogram law for multiple forces:
FR = (F1 + F2) + F3.
Important Points
Scalars: Positive or negative numbers.
Vectors: Quantities with magnitude, direction, and sense.
Proper analysis uses x-y coordinate systems for resolving forces.
Practice & Example Problems
Example 2-1: Calculate resultant force generated by two forces at a specified angle using the parallelogram law.
Example 2-3: Component forces determination involving vector operations.
Addition of a System of Coplanar Forces
Types of Forces
Coplanar Forces: Lines of action reside in the same plane.
Collinear Forces: Lines of action reside on the same line.
Concurrent Forces: Meet at a point (not necessarily collinear).
Coplanar Concurrent Forces: Meet at one point on the same plane.
Coplanar Non-concurrent Forces: Do not meet at a point, but in the same plane.
Non-coplanar Concurrent Forces: Meet at one point not in the same plane.
Non-coplanar Non-concurrent Forces: Do not meet and are not on the same plane.
Notation Approaches
Scalar Notation:
F = Fx + Fy
Fx = F Cos θ ; Fy = F Sin θ.
Cartesian Vector Notation:
F = Fx i + Fy j, where i and j are unit vectors.
Coplanar Force Resultants
Resolving forces into x and y components and adding them.
Resultant force calculated using law of cosines or using component addition techniques.
Important Synopsis
Forces resolved in an established x, y coordinate system expedite resultant determinations.
Positive directions designated by Cartesian unit vectors.
Magnitude calculated using the Pythagorean theorem and direction from trigonometric relations.
Conclusion
A systematized approach to vectors in statics enhances understanding of force interactions.
Thank You
Instructor: Dr. Uzair Khaleeq uz Zaman
Affiliation: College of E&ME