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Chapter 2: Force Vectors Engineering Mechanics: Statics Objectives To show how to add forces and resolve them into components using the Parallelogram Law. To express force and position in Cartesian vector form and explain how to determine the vector’s magnitude and direction. Chapter Outline Scalars and Vectors Vector Operations Vector Addition of Forces Addition of System of Coplanar Forces Vector operation Cartesian Addition Vectors and Subtraction of Cartesian Vectors Position Force Dot Vectors Vector Directed along a Line Product Review of Scalars and Vectors Number Any positive or negative value. e.g.: 5, -3.07, π... Scalar A quantity characterized by a positive or negative number and has a unit. e.g.: mass (5.1 kg), volume (0.028 m3)... Scalars and Vectors Vector A quantity that has both magnitude and direction measured from a given axis. e.g.: Position (3.4 km North), force (8.73 N towards right side), ... – Represented by a letter with an arrow over it such as A or bold such as A – Magnitude is shown by A or simply A Scalars and Vectors Scalars Characteristics Application VALUE (POSITIVE OR NEGATIVE) & UNIT (both togather called MAGNITUDE) mass, speed, volume, time Vectors VALUE (POSITIVE OR NEGATIVE) UNIT (both togather called MAGNITUDE) & DIRECTION velocity, acceleration force Scalars and Vectors Example Magnitude of Vector = 4 units Direction of Vector = 20° measured counterclockwise from the horizontal axis Sense of Vector = Upward and to the right The point O is called tail of the vector and the point P is called the tip or head Vector Operations Multiplication and Division of a Vector by a Scalar - Product of vector A and scalar a = aA - Magnitude = aA - If a is positive (+), sense of aA is the same as sense of A - If a is negative (-), sense of aA, it is opposite to the sense of A Vector Operations Multiplication and Division of a Vector by a Scalar - Negative of a vector is found by multiplying the vector by ( -1 ) - Law of multiplication applies e.g.: A/a = ( 1/a ) A, if a≠0 Vector Operations Vector Addition Addition of two vectors A and B gives a resultant vector R by the parallelogram law special case of parallelogram law is triangle construction (see the next slide) Commutative rule e.g.: R = A + B = B + A Vector Operations Vector Addition Parallelogram Law Triangular Construction Vector Addition of Forces Parallelogram Law description - To resolve a force into components along two axes directed from the tail of the force - Start at the head, constructing lines parallel to the axes Vector Operations Vector Addition - Special case: Vectors A and B are collinear (both have the same line of action). Triangular shape does not form. Vector Operations Vector Subtraction Special case of addition e.g.: R’ = A – B = A + ( - B ) Rules of Vector Addition Applies Vector Operations Resolution of Vector Any vector can be resolved into two components by the parallelogram law The two components A and B are drawn such that they extend from the tail of R Vector Operations Resolution of a vector is breaking up a vector into its components. It is the reverse application of the parallelogram law. Vector Addition of Forces When two or more forces are added, successive applications of the parallelogram law is carried out to find the resultant e.g.: Forces F1, F2 and F3 acts at a point O - First, find resultant of F1 + F2 - Resultant, FR = ( F1 + F2 ) + F3 Vector Addition of Forces Method 1: (graphical) parallelogram Law OR Establishing triangles Method 2: Trigonometry Procedure for Analysis: Parallelogram Law - Make a sketch showing the vector addition using the parallelogram law - Two “component” forces add according to the parallelogram law yielding a resultant force. - Resultant force is shown by the diagonal of the parallelogram - The components are the sides of the parallelogram - Label all the known and unknown force magnitudes and angles. - Identify the two unknowns. Procedure for Analysis: Trigonometry - Redraw half portion of the parallelogram - Magnitude of the resultant force can be determined by the law of COSINE - Direction of the resultant force can be determined by the law of SINE Procedure for Analysis: Magnitude of the two components can be determined by the law of COSINE. Direction of the two components can be determined by the law of SINE. Vector Addition of Forces Example: The screw eye is subjected to two forces F1 and F2. Determine the magnitude and direction of the resultant force. Vector Addition of Forces Solution Parallelogram Law Unknown: magnitude of FR and angle θ Vector Addition of Forces Half portion of the parallelogram FR= Magnitude of the resultant force (determined by the law of cosine) θ= angle (determined by the law of sine) ϕ = direction of the resultant force = θ +15° Vector Addition of Forces Solution Trigonometry Law of Cosine FR 100 N 2 150 N 2 - 2 100 N 150 N cos 115 10000 22500 30000 0.4226 212.6 N Vector Addition of Forces Solution Trigonometry Law of Sines 150 N 212.6 N sin θ sin115 150 N 0.9063 sin θ 212.6 N θ 39.8 Vector Addition of Forces Solution Trigonometry Direction Φ of FR measured from the horizontal ϕ = 39.7613 +15 = 54.7613 Vector Operations Example: The p and q axes are not perpendicular to each other. If the component of 365 N force along pp axis is 237.5 N, determine the other component along qq axis and the unknown angle β. q p 365 N 38.5° β p q Vector Operations Solution: The p and q axes are not perpendicular to each other. If the component of 365 N force along pp axis is 237.5 N, determine the other component along qq axis and the unknown angle β. Establish a paralelogram or a triangle. Given are: resultant and component along pp axis. q p 38.5° β p q Vector Operations Solution: The p and q axes are not perpendicular to each other. If the component of 365 N force along pp axis is 237.5 N, determine the other component along qq axis and the unknown angle β. Establish a paralelogram or a triangle. Given are: resultant and component along pp axis. q p 38.5° β 38.5° p q Vector Operations Solution: The p and q axes are not perpendicular to each other. If the component of 365 N force along pp axis is 237.5 N, determine the other component along qq axis and the unknown angle β. Establish a paralelogram or a triangle. Given are: resultant and component along pp axis. q p 38.5° β β 38.5° p q Addition of a System of Concurrent Coplanar (2D) Forces Concurrent at a point: FR = ∑F Addition of a System of Concurrent Coplanar (2D) Forces Cartesian Vector Notation - Cartesian unit vectors i and j are used to designate the x and y directions - Unit vectors i and j have dimensionless magnitude of unity ( = 1 ) Addition of a System of Concurrent Coplanar (2D) Forces Cartesian Vector Notation F = F x i + Fy j F’ = F’x i + F’y (-j) F’ = F’x i – F’y j Addition of a System of Concurrent Coplanar (2D) Forces Resolve vectors into components using x and y axes system. Each component of the vector will have a magnitude and a direction. The directions are based on the x and y axes. The “unit vectors” i and j are used to designate x and y axes. x and y axes are always perpendicular to each other. Together, they can be directed at any inclination. F = Fx i + Fy j Cartesian Vector Notation Vector components may be expressed as products of the unit vectors with the scalar magnitudes of the vector components. F = Fx i +Fy j Fx and Fy are referred to as the scalar components of F Addition of a System of Concurrent Coplanar (2D) Forces Coplanar Force Resultants To determine resultant of several coplanar forces: - Resolve force into x and y components - Addition of the respective components using scalar algebra - Resultant force is found using the parallelogram law Addition of a System of Concurrent Coplanar (2D) Forces Coplanar Force Resultants - Positive scalars = sense of direction along the positive coordinate axes - Negative scalars = sense of direction along the negative coordinate axes - Magnitude of FR can be found by Pythagorean Theorem FR = F 2 Rx +F 2 Ry Addition of a System of Concurrent Coplanar (2D) Forces Coplanar Force Resultants - Direction angle θ (orientation of the force) can be found by trigonometry θ = tan 1 FRy FRx Addition of a System of Concurrent Coplanar (2D) Forces Addition of a System of Concurrent Coplanar (2D) Forces Example: Add (sum) the given three coplanar forces Addition of a System of Concurrent Coplanar (2D) Forces Cartesian Vector Method (solution by three steps) Step 1: to resolve each force into its x-y components. Step 2: to add all the x components together and add all the y components together. These two totals become the resultant vector. Step 3: find the magnitude and the angle of the resultant vector. Addition of a System of Concurrent Coplanar (2D) Forces Example: Add (sum) the given three coplanar forces Step 1 Cartesian vector notation F1 = F1x i + F1y j F2 = - F2x i + F2y j F3 = F3x i – F3y j Addition of a System of Concurrent Coplanar (2D) Forces Step 2 Vector resultant is therefore FR = F1 + F2 + F3 = F1x i + F1y j - F2x i + F2y j + F3x i – F3yj = (F1x - F2x + F3x)i + (F1y + F2y – F3y)j = (FRx)i + (FRy)j Addition of a System of Concurrent Coplanar (2D) Forces Coplanar Force Resultants (→ ) FRx = (F1x - F2x + F3x) (+↑) F = (F + F – F ) + Ry 1y 2y 3y In all cases, FRx = ∑Fx FRy = ∑Fy * Take note of the sign conventions Addition of a System of Concurrent Coplanar (2D) Forces Step 3 The magnitude and the angle of the resultant vector Scalar Notation: 2 Rx 2 Ry FR = F + F θ = tan 1 FRy FRx Addition of a System of Concurrent Coplanar (2D) Forces WAYS OF FINDING THE COMPONENTS OF FORCES IN 2D By an ANGLE measured from any axis (Cosine of this angle gives the component of that axis) 1- Addition of a System of Concurrent Coplanar (2D) Forces WAYS OF FINDING THE COMPONENTS OF FORCES IN 2D 2- By right angle TRIANGLE of known sides Addition of a System of Concurrent Coplanar (2D) Forces WAYS OF FINDING THE COMPONENTS OF FORCES IN 2D 3- By COORDINATES or known lengths. (18, 10) 10 cm (0, 0) 18 cm Addition of a System of Concurrent Coplanar (2D) Forces Example: The end of the boom O is subjected to three concurrent and coplanar forces. Determine the magnitude and orientation of the resultant force. 3 35˚ Addition of a System of Concurrent Coplanar (2D) Forces Solution 35˚ FRx Σ Fx : 4 FRx 400 N 250 sin 35 N 200 N 5 416.606 N FRy Σ Fy : 3 FRy 250 cos 35 N 200 N 5 324.788 N 324.788 N 416.606 N Addition of a System of Concurrent Coplanar (2D) Forces Solution Resultant Force 2 2 FR 416.606 N 324.788 N 528.250 N From vector addition, Direction angle θ is 324.788 N θ tan 1 416.606 N 37.9402 180 37.9402 142.0598 324.788 N 142.0598° 416.616 N Addition of a System of Concurrent Coplanar (2D) Forces Example: Addition of a System of Concurrent Coplanar (2D) Forces Example: R R