statics chapter 2

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CHAPTER 2 – PART 3: POSITION & FORCE VECTORS Today’s Objectives : Students will be able to : a) Represent a position vector in Cartesian coordinate form, from given geometry. b) Represent a force vector directed along a line. Class contents : Daily quiz Applications Position vectors Force vectors Examples Group problem solving

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Chapter 2 Part 3

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Page 1: Statics Chapter 2

CHAPTER 2 – PART 3: POSITION & FORCE VECTORS

Today’s Objectives:

Students will be able to :

a) Represent a position vector in Cartesian coordinate form, from given geometry.

b) Represent a force vector directed along a line.

Class contents:

• Daily quiz

• Applications

• Position vectors

• Force vectors

• Examples

• Group problem solving

Page 2: Statics Chapter 2

Wing strut

APPLICATIONS

How can we represent the force along the wing strut in a 3-D Cartesian vector form?

Page 3: Statics Chapter 2

POSITION VECTOR

A position vector is defined as a fixed vector that locates a point in space relative to another point.

Consider two points, A & B, in 3-D space. Let their coordinates be (XA, YA, ZA) and ( XB, YB, ZB ), respectively.

The position vector directed from A to B, r AB , is defined as

r AB = {( XB – XA ) i + ( YB – YA ) j + ( ZB – ZA ) k }m

Please note that B is the ending point and A is the starting point. So ALWAYS subtract the “tail” coordinates from the “tip” coordinates!

Page 4: Statics Chapter 2

FORCE VECTOR DIRECTED ALONG A LINE (Section 2.8)

If a force is directed along a line, then we can represent the force vector in Cartesian Coordinates by using a unit vector and the force magnitude. So we need to:

a) Find the position vector, r AB , along two points on that line.

b) Find the unit vector describing the line’s direction, uAB = (rAB/rAB).

c) Multiply the unit vector by the magnitude of the force, F = F uAB .

Page 5: Statics Chapter 2

Example 2.12

An elastic rubber band is attached to points A and B. Determine its length and its direction measured from A towards B.

Page 6: Statics Chapter 2

SolutionPosition vector

r = [-2m – 1m]i + [2m – 0]j + [3m – (-3m)]k = {-3i + 2j + 6k}m

Magnitude = length of the rubber band

Unit vector in the director of ru = r /r = -3/7i + 2/7j + 6/7k

mr 7623 222

Example 2.12

Page 7: Statics Chapter 2

Solutionα = cos-1(-3/7) = 115°

β = cos-1(2/7) = 73.4°

γ = cos-1(6/7) = 31.0°

Example 2.12

Page 8: Statics Chapter 2

The man pulls on the cord with a force of 350N. Represent this force acting on the support A, as a Cartesian vector and determine its direction.

Example 2.13

Page 9: Statics Chapter 2

SolutionEnd points of the cord are A (0m, 0m, 7.5m) and B (3m, -2m, 1.5m)r = (3m – 0m)i + (-2m – 0m)j + (1.5m – 7.5m)k

= {3i – 2j – 6k}mMagnitude = length of cord AB

Unit vector, u = r /r = 3/7i - 2/7j - 6/7k

mmmmr 7623 222

Example 2.13

Page 10: Statics Chapter 2

SolutionForce F has a magnitude of 350N, direction specified by u

F = Fu = 350N(3/7i - 2/7j - 6/7k) = {150i - 100j - 300k} N

α = cos-1(3/7) = 64.6° β = cos-1(-2/7) = 107° γ = cos-1(-6/7) = 149°

Page 11: Statics Chapter 2

The roof is supported by cables. If the cables exert FAB = 100N and FAC = 120N

on the wall hook at A, determine the magnitude of the resultant force acting at A.

GROUP PROBLEM SOLVING

Page 12: Statics Chapter 2

GROUP PROBLEM SOLVING (continued)

Page 13: Statics Chapter 2

GROUP PROBLEM SOLVING (continued)

Page 14: Statics Chapter 2

GROUP PROBLEM SOLVING (continued)

Page 15: Statics Chapter 2