KULIAH VI MEKANIKA TEKNIK KESETIMBANGAN PARTIKEL (2D)

Slides:



Advertisements
Similar presentations
Statics of Particles MET 2214 Ok. Lets get started.
Advertisements

Today’s Objectives: Students will be able to :
KULIAH II MEKANIKA TEKNIK TI KESEIMBANGAN PARTIKEL (2D)
Problem y x Collars A and B are connected P
Statics of Particles.
Follow the same procedure as other force problems, but keep in mind: 1) Draw a free body diagram for EACH object or for each junction in a rope.
Equilibrium of a Rigid Body
Translational Equilibrium Physics Montwood High School R. Casao.
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
EQUILIBRIUM OF A PARTICLE IN 3-D (Section 3.4)
Today’s Objectives: Students will be able to :
EQUILIBRIUM OF A PARTICLE IN 2-D Today’s Objectives:
EQUILIBRIUM OF A PARTICLE IN 2-D Today’s Objectives: Students will be able to : a) Draw a free body diagram (FBD), and, b) Apply equations of equilibrium.
Chapter 2 Statics of Particles
Copyright © 2010 Pearson Education South Asia Pte Ltd
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
Forces and equilibrium
Statics of Particles.
Overview of Mechanical Engineering for Non-MEs Part 1: Statics 2 Statics of Particles Concurrent Forces.
Statics of Particles.
Statics of Particles.
3D Rigid Body Equilibrium. (Reference 5.5 and 5.6)
Equilibrium of a particle
Today’s Objectives: Students will be able to :
Force Vector (cont’).
Objectives: The student will be able to: Draw an accurate free body diagram locating each of the forces acting on an object or a system of objects. Use.
EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMBERS
Today’s Objectives: Students will be able to :
College of Engineering CIVE 1150 Fall Rectangular Components of a Force: Unit Vectors Vector components may be expressed as products of the unit.
Engineering Mechanics: Statics
Problem y C D A container of weight W = 1165 N is supported O
Today’s Objective: Students will be able to:
Force Vectors Phy621- Gillis
THREE-DIMENSIONAL FORCE SYSTEMS Today’s Objectives: Students will be able to solve 3-D particle equilibrium problems by a) Drawing a 3-D free body diagram,
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
ME 201 Engineering Mechanics: Statics Chapter 3 – Part A 3.1 Condition for the Equilibrium of a Particle 3.2 The Free-Body Diagram 3.3 Co-Planar Force.
Theoretical Mechanics STATICS KINEMATICS
Midterm Review  Five Problems 2-D/3-D Vectors, 2-D/3-D equilibrium, Dot Product, EoE, Cross Product, Moments  Closed Book & Note  Allowed to bring.
EQUATIONS OF EQUILIBRIUM & TWO- AND THREE-FORCE MEMEBERS In-Class Activities: Check Homework, if any Reading Quiz Applications Equations of Equilibrium.
Chapter 3 Equilibrium of a Particle. 3.1 Condition for the Equilibrium of a Particle o "static equilibrium" is used to describe an object at rest. o To.
THREE-DIMENSIONAL FORCE SYSTEMS In-class Activities: Check Homework Reading Quiz Applications Equations of Equilibrium Concept Questions Group Problem.
ME 201 Engineering Mechanics: Statics Chapter 3 – Part b - continued 3.1 Condition for the Equilibrium of a Particle 3.2 The Free-Body Diagram 3.3 Co-Planar.
Problem 4-c 1.2 m y 1.5 m z x 5 kN A B C E D  1 m 2 m A 3-m pole is supported by a ball-and-socket joint at A and by the cables CD and CE. Knowing that.
Equilibrium of a Particle 3 Engineering Mechanics: Statics in SI Units, 12e Copyright © 2010 Pearson Education South Asia Pte Ltd.
ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo
Statics. Equilibrium Moves at constant velocity V =C Moves at constant velocity V =C At rest V = 0 At rest V = 0 Constant Velocity.
MEC 0011 Statics Lecture 3 Prof. Sanghee Kim Fall_ 2012.
A PHYSICS EXAM Don’t be Static!.
Statics, Fourteenth Edition R.C. Hibbeler Copyright ©2016 by Pearson Education, Inc. All rights reserved. In-class Activities: Check Homework Reading Quiz.
 Particle Assumption  Modeling of Problem  Free Body Diagram: FBD  Newton’s Law of Motion  1 st Law  2 nd Law  3 rd Law Chap.#3: Statics of Particles.
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS Objectives: a) Identify support reactions, and, b) Draw a free-body diagram.
Today’s Objectives: Students will be able to :
Today’s Objectives: Students will be able to :
Today’s Objectives: Students will be able to :
Copyright © 2010 Pearson Education South Asia Pte Ltd
Today’s Objectives: Students will be able to :
THREE-DIMENSIONAL FORCE SYSTEMS
Engineering Mechanics : STATICS
Today’s Objectives: Students will be able to :
Engineering Mechanics : STATICS
THREE-DIMENSIONAL FORCE SYSTEMS
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg.
Engineering Mechanics: Statics
1.
General Principles.
General Principles.
FORCES ON CABLES EQUIBILIRIUM ON PARTICLE
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
Statics Course Code: CIVL211 Equilibriums Dr. Aeid A. Abdulrazeg.
Engineering Mechanics : STATICS
Presentation transcript:

KULIAH VI MEKANIKA TEKNIK KESETIMBANGAN PARTIKEL (2D) RIYANTO PENDIDIKAN TEKNIK MESIN, JPTK FKIP UNS

Berapa besar gaya yg bekerja pada tali AB dan AD ? 2 kN

Equilibrium of a Particle (2-D) Learning’s Objectives: Students will be able to : 1. Draw a free body diagram (FBD), and, 2. Apply equations of equilibrium to solve a 2-D problem. For a given cable strength, what is the maximum weight that can be lifted ?

THE WHAT, WHY AND HOW OF A FREE BODY DIAGRAM (FBD) Free Body Diagrams are one of the most important things for you to know how to draw and use. What ? - It is a drawing that shows all external forces acting on the particle. Why ? - It helps you write the equations of equilibrium used to solve for the unknowns (usually forces or angles).

2. Show all the forces that act on the particle. 1. Imagine the particle to be isolated or cut free from its surroundings. 2. Show all the forces that act on the particle. Active forces: They want to move the particle. Reactive forces: They tend to resist the motion. 3. Identify each force and show all known magnitudes and directions. Show all unknown magnitudes and / or directions as variables . Mainly explain the three steps using the example . A Note : Engine mass = 250 Kg FBD at A

Free Body Diagram (FBD) (2-D)

Equations of Equilibrium (2-D) Since particle A is in equilibrium, the net force at A is zero. So FAB + FAD + FAC = 0 or  F = 0 In general, for a particle in equilibrium,  F = 0 or Fx i + Fy j = 0 = 0 i + 0 j (A vector equation) Or, written in a scalar form, These are two scalar equations of equilibrium (EofE). They can be used to solve for up to two unknowns. Fx = 0 and  Fy = 0

Solving the second equation gives: TB = 4.90 kN EXAMPLE Note : Engine mass = 250 Kg FBD at A Write the scalar EofE: +   Fx = TB cos 30º – TD = 0 +  Fy = TB sin 30º – 2.452 kN = 0 You may tell students that they should know how to solve linear simultaneous equations by hand and also using calculator . If they need help they can see you . Solving the second equation gives: TB = 4.90 kN From the first equation, we get: TD = 4.25 kN

Problem Solving (2-D) F = 600 N θ = 25o Given: The car is towed at constant speed by the 600 N force and the angle  is 25°. Find: The forces in the ropes AB and AC. Plan: 1. Draw a FBD for point A. 2. Apply the EofE to solve for the forces in ropes AB and AC.

Problem Solving (2-D) 600 N FBD at point A A FAC FAB F = 600 N θ = 25o 30° 25° 600 N FAB FAC A FBD at point A Applying the scalar EofE at A, we get; +  Fx = FAC cos 30° – FAB cos 25° = 0 +  Fy = -FAC sin 30° – FAB sin 25° + 600 = 0 Solving the above equations, we get; FAB = 634 N FAC = 664 N

Example SOLUTION: Construct a free-body diagram for the particle at the junction of the rope and cable. Determine the unknown force magnitudes. In a ship-unloading operation, a 15.6 kN automobile is supported by a cable. A rope is tied to the cable and pulled to center the automobile over its intended position. What is the tension in the rope?

Given: Sack A weighs 20 N. and geometry is as shown. EXAMPLE Given: Sack A weighs 20 N. and geometry is as shown. Find: Forces in the cables and weight of sack B. Plan: 1. Draw a FBD for Point E. 2. Apply EofE at Point E to solve for the unknowns (TEG & TEC). 3. Repeat this process at C. You may ask the students to give a plan You may explain why analyze at E, first, and C, later

+   Fx = TEG sin 30º – TEC cos 45º = 0 EXAMPLE (continued) A FBD at E should look like the one to the left. Note the assumed directions for the two cable tensions. The scalar EofE are: +   Fx = TEG sin 30º – TEC cos 45º = 0 +   Fy = TEG cos 30º – TEC sin 45º – 20 N = 0 Solving these two simultaneous equations for the two unknowns yields: TEC = 38.6 N TEG = 54.6 N You may ask students to give equations of equilibrium.students hand-outs should be without the equations.

   Fy = (3/5) TCD + 38.64 sin 45 – WB = 0 EXAMPLE (continued) Now move on to ring C. A FBD for C should look like the one to the left. The scalar EofE are:    Fx = 38.64 cos 45 – (4/5) TCD = 0    Fy = (3/5) TCD + 38.64 sin 45 – WB = 0 You may ask the students to give equations of equilibrium.Students hand-outs should be without the equation. You may also explain about the direction of 38.6 lb force (see fig. 3.7 d, page 88) Solving the first equation and then the second yields TCD = 34.2 N and WB = 47.8 N .

READING QUIZ 1) When a particle is in equilibrium, the sum of forces acting on it equals ___ . (Choose the most appropriate answer) A) a constant B) a positive number C) zero D) a negative number E) an integer. 2) For a frictionless pulley and cable, tensions in the cable (T1 and T2) are related as _____ . A) T1 > T2 B) T1 = T2 C) T1 < T2 D) T1 = T2 sin  Answers: 1. C 2. B

ATTENTION QUIZ 3. Using this FBD of Point C, the sum of forces in the x-direction ( FX) is ___ . Use a sign convention of +  . A) F2 sin 50° – 20 = 0 B) F2 cos 50° – 20 = 0 C) F2 sin 50° – F1 = 0 D) F2 cos 50° + 20 = 0 F2 20 N 50° C F1 Answers: 2. B

tentukan harga P dan jarak a SOAL TANTANGAN Jika b = 4 m, tentukan harga P dan jarak a

Terima Kasih