equilibrium & equation of equilibrium in 3d

28
AHSANULLAH UNIVERSITY OF SCIENCE & TECHNOLOGY • Name : MD. Moinul Islam. • Student ID : 10.01.03.076. • Course No : CE-416. • Course Title: Prestress Concrete Design Sessional.

Upload: imoinul007

Post on 19-Jan-2015

1.819 views

Category:

Technology


4 download

DESCRIPTION

 

TRANSCRIPT

Page 1: Equilibrium & equation of equilibrium in 3D

AHSANULLAH UNIVERSITY OF SCIENCE & TECHNOLOGY

• Name : MD. Moinul Islam.• Student ID : 10.01.03.076.• Course No : CE-416.• Course Title: Prestress Concrete Design

Sessional.

Page 2: Equilibrium & equation of equilibrium in 3D

Equilibrium & Equation of Equilibrium :3D

Page 3: Equilibrium & equation of equilibrium in 3D

The Word Equilibrium Derived From

• The word equilibrium is derived from the Latin word æquilībrium, from æquus (“equal”) + lībra (“balance”). which means equal balance.

• In physics it means a state of even balance in which opposing forces or tendencies neutralize each other.

Page 4: Equilibrium & equation of equilibrium in 3D

Equilibrium

• Is the condition of force where it is acted but simply cancelled out. These forces may be even large enough to cause permanent deformation.

Page 5: Equilibrium & equation of equilibrium in 3D

Basic Idea of Equilibrium

Page 6: Equilibrium & equation of equilibrium in 3D

Terms Related To Equilibrium

Page 7: Equilibrium & equation of equilibrium in 3D

CENTER OF GRAVITY

• The center of gravity of a body is the point where its entire weight maybe assumed concentrated.

Practical example of equilibrium and center of gravity: A tight rope walker in a circus carries a weighted pole or an umbrella.

Page 8: Equilibrium & equation of equilibrium in 3D

Concurrent & Non-Concurrent

Force System

Concurrent system occur when the lines of actions of the forces acting on a body intersect at a common point.

Non-concurrent system occurs when the forces are acting at different points.

Page 9: Equilibrium & equation of equilibrium in 3D

TypesThere are two basic conditions of equilibrium.

Translational equilibrium.Rotational equilibrium.

• The term "translational equilibrium" describes an object that experiences no linear acceleration. (First condition of equilibrium )

• An object experiencing no rotational acceleration (a component of torque) is said to be in rotational equilibrium. (Second condition of equilibrium )

• Typically, an object at rest in a stable situation experiences both linear and rotational equilibrium.

Page 10: Equilibrium & equation of equilibrium in 3D

Types

There are two kinds of mechanical equilibrium:

static equilibrium anddynamic equilibrium.

• Any object which is in static equilibrium has zero net force acting on it and is at rest.

• Any object which is in dynamic equilibrium has zero net force acting on it and is moving at a constant velocity.

Page 11: Equilibrium & equation of equilibrium in 3D

Newton’s First Law of Physics:

• A body at rest will stay at rest and a body in motion will stay in motion unless acted upon by an unbalanced force.

• Therefore, sum of all forces must be zero. F = 0

Resultant of all forces acting on a particle is zero.

Equilibrium

Page 12: Equilibrium & equation of equilibrium in 3D

Equilibrium Equation from Newton’sLaw

• If an object is in equilibrium, then the resultant force acting on an object equals zero. This is expressed as follows:

equation)(vector 0R FF

Some problems can be analyzed using only 2D, while others require 3D.

Page 13: Equilibrium & equation of equilibrium in 3D

Necessary Condition for Equilibrium

• The necessary conditions for equilibrium are:

(i) the vector sum of all external forces is zero. (ii) the sum of the moments of all external

forces about any line is zero.

Page 14: Equilibrium & equation of equilibrium in 3D

EQUATIONS OF EQUILIBRIUM

• As stated earlier, when a body is in equilibrium, the net force and the net moment equal zero, i.e.

F = 0 and M = 0These two vector equations can be written as six scalar equations of equilibrium. These are

FX = 0 FY = 0 FZ = 0

åMX = 0 MY = 0 MZ = 0

6 equations for 3D equilibrium

Note: The moment equations can be determined about any point. Usually, choosing the point where the maximum number of unknown forces are present simplifies the solution.

Page 15: Equilibrium & equation of equilibrium in 3D

Categories of equilibrium according to Force system

Page 16: Equilibrium & equation of equilibrium in 3D

Three-Dimensional Reaction at Supports & Connections

Page 17: Equilibrium & equation of equilibrium in 3D
Page 18: Equilibrium & equation of equilibrium in 3D
Page 19: Equilibrium & equation of equilibrium in 3D
Page 20: Equilibrium & equation of equilibrium in 3D

Free Body Diagram(FBD)

Page 21: Equilibrium & equation of equilibrium in 3D

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 is key to being able to write the equations of equilibrium— which are used to solve for the unknowns (usually forces or angles).

Page 22: Equilibrium & equation of equilibrium in 3D

Steps of Drawing a FBD

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.

Page 23: Equilibrium & equation of equilibrium in 3D

Steps of Drawing a FBD

FBDIdealized modelReal world example

Page 24: Equilibrium & equation of equilibrium in 3D

THE PROCESS OF SOLVING RIGID BODY EQUILIBRIUM PROBLEMS

1) Draw a free-body diagram (FBD) showing all the external forces.

2) Apply the equations of equilibrium to solve for any unknowns.

Note: If there are more unknowns than the number of independent equations, then we have a statically indeterminate situation. We cannot solve these problems using just statics.

Page 25: Equilibrium & equation of equilibrium in 3D

APPLICATION

Ball-and-socket jointCrane

Straps

Page 26: Equilibrium & equation of equilibrium in 3D

Application

Journal bearing Pinned connection

Page 27: Equilibrium & equation of equilibrium in 3D

The tie rod from point A is used to support the overhang at the entrance of a building. It is pin connected to the wall at A and to

the center of the overhang B.

If A is moved to a lower position D, will the force in the rod change or remain the same? By making such a change without understanding if there is a change in forces, failure might occur.

Page 28: Equilibrium & equation of equilibrium in 3D

Thank You