Slideshare uses cookies to improve functionality and performance, and to provide you with relevant advertising. If you continue browsing the site, you agree to the use of cookies on this website. See our User Agreement and Privacy Policy.

Slideshare uses cookies to improve functionality and performance, and to provide you with relevant advertising. If you continue browsing the site, you agree to the use of cookies on this website. See our Privacy Policy and User Agreement for details.

Successfully reported this slideshow.

Like this document? Why not share!

- Hookes law by Mahmud Muhammad 627 views
- Review by Mahmud Muhammad 1786 views
- Simple Stress and Strain by Msheer Bargaray 4792 views
- Simpale stress and simple strain by Keval Patel 25787 views
- Stress and strain- mechanics of solid by Kaushal Patel 3593 views
- types of stress and strain by Home 28370 views

No Downloads

Total views

1,433

On SlideShare

0

From Embeds

0

Number of Embeds

22

Shares

0

Downloads

37

Comments

0

Likes

3

No embeds

No notes for slide

- 1. Chapter Objectives •Develop the equations of equilibrium for a rigid body •Concept of the free-body diagram for a rigid body •Solve rigid-body equilibrium problems using the equations of equilibrium When all the forces that act upon an object are balanced, then the object is said to be in a state of equilibrium. If an object is at equilibrium, then the forces are balanced. Balanced is the key word that is used to describe equilibrium situations. Thus, the net force is zero and the acceleration is 0 m/s/s. Objects at equilibrium must have an acceleration of 0 m/s/s. This extends from Newton's first law of motion. But having an acceleration of 0 m/s/s does not mean the object is at rest. An object at equilibrium is either ... at rest and staying at rest, or in motion and continuing in motion with the same speed and direction. If an object is at rest and is in a state of equilibrium, then we would say that the object is at "static equilibrium." "Static" means stationary or at rest. The state of the object is analyzed in terms of the forces acting upon the object. The object is a point on a string upon which three forces were acting. See diagram at right. If the object is at equilibrium, then the net force acting upon the object should be 0 Newton. Thus, if all the forces are added together as vectors, then the resultant force (the vector sum) should be 0 Newton. (Recall that the net force is "the vector sum of all the forces" or the resultant of adding all the individual forces head-to-tail.) Thus, an accurately drawn vector addition diagram can be constructed to determine the resultant. Sample data for such a lab are shown below.
- 2. Force A Force B Force C Magnitude 3.4 N 9.2 N 9.8 N Direction 161 deg. 70 deg. 270 deg Another way of determining the net force (vector sum of all the forces) involves using the trigonometric functions to resolve each force into its horizontal and vertical components. Once the components are known, they can be compared to see if the vertical forces are balanced and if the horizontal forces are balanced. The diagram below shows vectors A, B, and C and their respective components. For vectors A and B, the vertical components can be determined using the sine of the angle and the horizontal components can be analyzed using the cosine of the angle. The magnitude and direction of each component for the sample data are shown in the table below the diagram.
- 3. The data in the table above show that the forces nearly balance. An analysis of the horizontal components shows that the leftward component of A nearly balances the rightward component of B. An analysis of the vertical components show that the sum of the upward components of A + B nearly balance the downward component of C. The vector sum of all the forces is (nearly) equal to 0 Newton. But what about the 0.1 N difference between rightward and leftward forces and the 0.2 N difference between the upward and downward forces? Why do the components of force only nearly balance? The sample data used in this analysis are the result of measured data from an actual experimental setup. The difference between the actual results and the expected results is due to the error incurred when measuring force A and force B. We would have to conclude that this low margin of experimental error reflects an experiment with excellent results. We could say it's "close enough for government work." The equilibrium of a body is expressed as FR=∑F=0 , (∑MR)o=∑Mo=0 Consider summing moments about some other point, such as point A, we require
- 4. ∑MA= r X FR +(MR)O=0 For equilibrium of a rigid body in 2D, ΣFx= 0; ΣFy= 0; ΣMO= 0 •ΣFxand ΣFyrepresent sums of x and y components of all the forces •ΣMOrepresents the sum of the couple moments and moments of the force components Free Body Diagrams- Support Reactions : • If a support prevents the translation of a body in a given direction, then a force is developed on the body in that direction. • If rotation is prevented, a couple moment is exerted on the body.
- 5. Free Body Diagrams-Internal Forces: •External and internal forces can act on a rigid body •For FBD, internal forces act between particles which are contained within the boundary of the FBD, are not represented •Particles outside this boundary exert external forces on the system Weight and Center of Gravity •Each particle has a specified weight
- 6. •System can be represented by a single resultant force, known as weight Wof the body •Location of the force application is known as the center of gravity Procedure for Drawing a FBD: 1. Draw Outlined Shape •Imagine body to be isolated or cut free from its constraints 2. Show All Forces and Couple Moments •Identify all external forces and couple moments that act on the body Procedure for Analysis Equations of Equilibrium •Apply ΣMO= 0 about a point O •Unknowns moments of are zero about O and a direct solution the third unknown can be obtained
- 7. •Orient the x and y axes along the lines that will provide the simplest resolution of the forces into their x and y components •Negative result scalar is opposite to that was assumed on the FBD

No public clipboards found for this slide

×
### Save the most important slides with Clipping

Clipping is a handy way to collect and organize the most important slides from a presentation. You can keep your great finds in clipboards organized around topics.

Be the first to comment