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Engr221 Chapter 5 1 Announcements Equilibrium of a Rigid Body Today’s Objectives Identify support reactions Draw a free body diagram Class Activities • Applications Support reactions Free body diagrams • Examples

Announcements Equilibrium of a Rigid Body

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Page 1: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 1

Announcements

Equilibrium of a Rigid Body

Today’s Objectives• Identify support reactions

• Draw a free body diagram

Class Activities• Applications

• Support reactions

• Free body diagrams

• Examples

Page 2: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 2

Applications

A 200 kg platform is suspended off an oil rig. How do we determine the force reactions at the joints and the forces in the cables?

How are the idealized model and the free body diagram used to do this? Which diagram above is the idealized model?

A steel beam is used to support roof joists. How can we determine the support reactions at A & B?

Again, how can we make use of an idealized model and a free body diagram to answer this question?

Applications - continued

Page 3: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 3

Conditions for Rigid-Body Equilibrium

In contrast to the forces on a particle, the forces on a rigid-body are not usually concurrent and may cause rotation of the body (due to the moments created by the forces).

For a rigid body to be in equilibrium, the net force as well as the net moment about any arbitrary point O must be equal to zero.

∑∑∑∑F = 0 and ∑∑∑∑MO = 0

Solving Rigid-Body Equilibrium Problems

For analyzing an actual physical system, it is helpful to create an idealized model.Then we need to draw a free-body diagram showing all the external (active and reactive) forces.Finally, we need to apply theEquations of Equilibrium (E-of-E) to solve for any unknowns.

Page 4: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 4

Drawing a Free-Body-Diagram

1. Draw an outlined shape. Imagine the body to be isolated or cut “free” from its constraints and draw its outlined shape.

2. Show all the external forces and couple moments. These typically include: a) applied loads, b) support reactions, and c) the weight of the body.

Idealized model Free body diagram

3. Label loads and dimensions: All known forces and couple moments should be labeled with their magnitudes and directions. For the unknown forces and couple moments, use letters like Ax, Ay, MA, etc. Indicate any necessary dimensions.

Drawing a Free-Body-Diagram - continued

Idealized model Free body diagram

Page 5: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 5

Support Reactions in 2-D

As a general rule, if a support prevents translation of a body in a given direction, then a force is developed on the body in the opposite direction. Similarly, if rotation is prevented, a couple moment is exerted on the body.

Support Reactions in 2-D - continued

Page 6: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 6

Support Reactions in 2-D - continued

Support Reactions in 2-D - continued

Page 7: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 7

Free Body Diagram Example

Given: An operator applies 20 lb to the foot pedal. A spring with k = 20 lb/in is stretched 1.5 in.

Draw: A free body diagram of the foot pedal.

The idealized model The free body diagram

Examples

Draw a FBD of the bar, which has smooth points of contact at A, B, and C. (smooth = no friction)

Page 8: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 8

Examples - continued

Draw a FBD of the 5000 lb dumpster (D). It is supported by a pin at A and the hydraulic cylinder BC (treat as a short link).

Examples - continued

Page 9: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 9

Examples - continued

Examples - continued

Page 10: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 10

Question

The beam and the cable (with a frictionless pulley at D) support an 80 kg load at C. In a FBD of the beam itself, how many unknowns are there?

A) 2 forces and 1 couple moment

B) 3 forces and 1 couple moment

C) 3 forces

D) 4 forces

If the directions of the force and the couple moments are reversed, what will happen to the beam?

A) The beam will lift from A

B) The beam will lift at B

C) The beam will be restrained

D) The beam will break

Question

Page 11: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 11

Questions

1. If a support prevents translation of a body, then the support exerts a ___________ on the body.

A) couple moment

B) force

C) both A and B

D) none of the above

2. Internal forces are _________ shown on the free body diagram of a whole body.

A) always

B) often

C) rarely

D) never

Questions

1. Internal forces are not shown on a free body diagram because the internal forces are_____

A) equal to zero

B) equal and opposite and they do not affect the calculations

C) negligibly small

D) not important

2. How many unknown support reactions are there in this problem?

A) 2 forces and 2 couple moments

B) 1 force and 2 couple moments

C) 3 forces

D) 3 forces and 1 couple moment

Page 12: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 12

• Identify support reactions

• Draw a free body diagram

Summary

Announcements

Page 13: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 13

Equations of Equilibrium in 2-D

Today’s Objectives• Apply equations of equilibrium to

solve for unknowns

• Recognize two-force members

Class Activities• Applications

• Equations of equilibrium

• Two-force members

• Examples

For a given load on the platform, how can we determine the forces at the joint A and the force in the link cylinder BC?

Applications

Page 14: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 14

A steel beam is used to support roof joists. How can we determine the support reactions at each end of the beam?

Applications - continued

Equations of Equilibrium

A body is subjected to a system of forces that lie in the x-y plane. When in equilibrium, the net force and net moment acting on the body are zero (as discussed earlier in Section 5.1). This 2-D condition can be represented by the three scalar equations:

∑ Fx = 0 ∑ Fy = 0 ∑ MO = 0

where point O is any arbitrary point.

Note that these equations are the ones most commonly usedfor solving 2-D equilibrium problems. There are two other sets of equilibrium equations that are rarely used. For your reference, they are described in the textbook.

x

y

F1

F2

F3

F4

O

Page 15: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 15

Two-Force Members

The solution to some equilibrium problems can be simplifiedif we recognize members that are subjected to forces at only two points (e.g., at points A and B).

If we apply the equations of equilibrium to such members, we can quickly determine that the resultant forces at A and Bmust be equal in magnitude and act in the opposite directions along the line joining points A and B.

Example of Two-Force Members

In the cases above, members AB can be considered as two-force members, provided that their weight is neglected.

This fact simplifies the equilibrium analysis of some rigid bodies since the directions of the resultant forces at A and B are thus known (along the line joining points A and B).

Page 16: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 16

Steps for Solving 2-D Equilibrium Problems

1. If not given, establish a suitable x-y coordinate system.

2. Draw a free body diagram (FBD) of the object under analysis.

3. Apply the three equations of equilibrium to solve for the unknowns.

Important Notes

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

2. The order in which we apply equationsmay affect the simplicity of the solution. For example, if we have two unknown vertical forces and one unknown horizontal force, then solving ∑ FX = 0 first, allows us to find the horizontal unknown quickly.

3. If the answer for an unknown comes out as a negative number, then the sense of the unknown force is opposite to that assumed when starting the problem.

Page 17: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 17

Given: Weight of the boom = 125 lb, the center of mass is at G, and the load = 600 lb.

Find: The support reactions at A and B.

Plan:

1. Put the x and y axes in the horizontal and vertical directions, respectively

2. Determine if there are any two-force members

3. Draw a complete FBD of the boom

4. Apply the E-of-E to solve for the unknowns

Example A

Note: Upon recognizing CB as a two-force member, the number of unknowns at B are reduced from two to one. Now, using the E-of-E,

+ ∑MA = 125 ∗ 4 + 600 ∗ 9 – FB sin 40° ∗ 1 – FB cos 40° ∗ 1 = 0

FB = 4188 lb or 4.19 kip

→ + ∑FX = AX + 4188 cos 40° = 0; AX = – 3.21 kip

↑ + ∑FY = AY + 4188 sin 40° – 125 – 600 = 0; AY = – 1.97 kip

AX

AY

A

1 ft 1 ft 3 ft 5 ft

B GD

600 lb125 lbFB

40°

FBD of the boom:

Example A - continued

Page 18: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 18

Given:The load on the bent rod is supported by a smooth inclined surface at B and a collar at A. The collar is free to slide over the fixed inclined rod.

Find: Support reactions at A and B

Plan:

a) Establish the x–y axes

b) Draw a complete FBD of the bent rod

c) Apply the E-of-E to solve for the unknowns

Example B

→ + ∑FX = (4 / 5) NA – (5 / 13) NB = 0

↑ + ∑FY = (3 / 5) NA + (12 / 13) NB – 100 = 0

Solving these two equations, we get

NB = 82.5 lband NA = 39.7 lb

+ ∑ MA = MA – 100 ∗ 3 – 200 + (12 / 13) NB ∗ 6 – (5 /13) NB ∗ 2 = 0

MA = 106 lb • ft

2 ft

200 lb•ftMA

3 ft 3 ftNA

53

4

13

5

12

100 lb

NB

FBD of the rod

Example B - continued

Page 19: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 19

1. For this beam, how many support reactions are there and is the problem statically determinate?

A) (2, Yes) B) (2, No)

C) (3, Yes) D) (3, No)

2. For the given beam loading: a) how many support reactions are there, b) is this problem statically determinate, and, c) is the structure stable?

A) (4, Yes, No) B) (4, No, Yes)

C) (5, Yes, No) D) (5, No, Yes)

F F F F

FFixed support

Pin joints

Questions

1. The three scalar equations ∑ FX = ∑ FY = ∑ MO = 0, are ____ equations of equilibrium in two dimensions.

A) incorrect

B) the only correct

C) the most commonly used

D) not sufficient

2. A rigid body is subjected to forces as shown. This body can be considered a ______ member.

A) single-force

B) two-force

C) three-force

D) six-force

Questions

Page 20: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 20

1. Which equation of equilibrium allows you to determine FB right away?

A) ∑ FX = 0

B) ∑ FY = 0

C) ∑ MA = 0

D) Any one of the above

AX A B

FBAY

100 lb

Question

• Apply equations of equilibrium to solve for unknowns

• Recognize two-force members

Summary

Page 21: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 21

Announcements

The mobile crane has a weight of 120,000 lb and a center of gravity at G1. The boom has a weight of 30,000 lb and a center of gravity at G2. Determine the smallest angle of tilt θ of the boom, without causing the crane to overturn if the suspended load is W = 40,000 lb. Neglect the thickness of the tracks at A and B.

Textbook Problem 5.44

θ = 26.4º

Page 22: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 22

The mobile crane has a weight of 120,000 lb and a center of gravity at G1. The boom has a weight of 30,000 lb and a center of gravity at G2. If the suspended load has a weight of W = 16,000 lb, determine the normal reactions at the tracks A and B. For the calculation, neglect the thickness of the tracks and take θ = 30º.

Textbook Problem 5.45

RA = 40.9 kip

RB = 125 kip

The uniform rod of length L and weight W is supported on the smooth planes. Determine its position θ for equilibrium. Neglect the thickness of the rod.

Textbook Problem 5.50

θ = tan-1(.5cotψ - .5cotφ)

Page 23: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 23

The rigid beam of negligible weight is supported by two springs and a pin at A. If the springs are uncompressed when the load is removed, determine the force in each spring when the load P is applied. Also, compute the vertical deflection of the end at C.

Textbook Problem 5.52

FB = 0.3P

FC = 0.6P

xC = 0.6P/k

The rigid metal strip of negligible weight is uses as part of an electromagnetic switch. Determine the maximum stiffness kof the springs at A and B so that the contact at C closes when the vertical force developed there is 0.5 N. Originally the strip is horizontal as shown.

Textbook Problem 5.56

k = 250 N/m

Page 24: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 24

Determine the distance d for placement of the load Pfor equilibrium of the smooth bar in the position θ as shown. Neglect the weight of the bar.

Textbook Problem 5.57

d = a/cos3θ

• Apply equations of equilibrium to solve for unknowns

• Recognize two-force members

Summary

Page 25: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 25

Announcements

Rigid Body Equilibrium in 3-D

Today’s Objectives• Identify support reactions in 3-D and

draw a free body diagram

• Apply the equations of equilibrium

Class Activities• Applications

• Support reactions in 3-D

• Equations of equilibrium

• Examples

Page 26: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 26

Ball-and-socket joints and journal bearings are often used in mechanical systems. How can we determine the support reactions at these joints for a given loading?

Applications

The weights of the fuselage and fuel act through A, B, and C. How will we determine the reactions at the wheels D, E, and F ?

A 50 lb sign is kept in equilibrium using two cables and a smooth collar. How can we determine the reactions at these supports?

Applications - continued

Page 27: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 27

Support Reactions in 3D - Table 5-2

As a general rule, if a support preventstranslation of a body in a given direction, then a reaction force acting in the opposite direction is developed on the body. Similarly, if rotation is prevented, a couple momentis exerted on the body by the support.

Support Reactions in 3D - continued

Page 28: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 28

Support Reactions in 3D - continued

Support Reactions in 3D - continued

Page 29: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 29

Important Note

A single bearing or hinge can prevent rotation by providing a resistive couple moment. However, it is usually preferred to use two or more properly aligned bearings or hinges. Thus, in these cases, only force reactions are generated and there are no moment reactions created.

Equilibrium Equations in 3-D

As stated earlier, when a body is in equilibrium, the net force and the net moment equal zero, i.e. ∑∑∑∑F = 0 and ∑∑∑∑MO = 0

These two vector equations can be written as six scalar equations of equilibrium. These are:

∑ FX = ∑ FY = ∑ FZ = 0

∑ MX = ∑ MY = ∑ MZ = 0

The moment equations can be determined about any point. Usually, choosing the point where the maximum number of unknown forces are presentsimplifies the solution. Those forces do not appear in the moment equation since they pass through the point.

Page 30: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 30

Constraints for a Rigid Body

Redundant Constraints: When a body has more supports than necessary to hold it in equilibrium, it becomes statically indeterminate.

A problem that is statically indeterminate has more unknowns than equations of equilibrium.

Are statically indeterminate structures used in practice? Why or why not?

Improper Constraints

Here, we have 6 unknowns but there is nothing restricting rotation about the x axis.In some cases, there may be as many unknown reactions as there are equations of equilibrium. However, if the supports are not properly constrained, the body may become unstable for some loading cases.

Page 31: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 31

Given:The cable of the tower crane is subjected to an 840N force. A fixed base at A supports the crane.

Find: Reactions at the fixed base A.

Plan:

a) Establish the x, y, and z axes

b) Draw a FBD of the crane

c) Write the forces using Cartesian vector notation

d) Apply the E-of-E (vector version) to solve for the unknown forces

Example A

rBC = {12 i + 8 j − 24 k } m

F = F [uBC ] N

= 840 [12i + 8 j − 24 k] / (122 + 82 + (– 242 ))½

= {360 i + 240 j − 720 k} N

FA = {A X i + AY j + AZ k } N

Example A - continued

Page 32: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 32

From the E-of-E we get, F + FA = 0

{(360 + AX) i + (240 + AY) j + (-720 + AZ ) k} = 0

Solving each component equation yields:

AX = −−−− 360 N AY = −−−− 240 N AZ = 720 N

Example A - continued

Sum the moments acting at point A:∑ M = MA + rAC ×××× F = 0

= 0

= MAX i + MAY j + MAZ k - 7200 i + 10800 j = 0

MAX = 7.200 kN-m MAY = -1.08 kN-m MAZ = 0

= MAX i + MAY j + MAZ k +

Example A - continued

720240360

01015

kji

Page 33: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 33

Given: A rod is supported by a ball-and-socket joint at A, a journal bearing at B and a short link at C. Assume the rod is properly aligned.

Find: The reactions at all the supports for the loading shown.

Plan:

a) Draw a FBD of the rod

b) Apply scalar E-of-E to solve for the unknowns

Example B

Applying the scalar E-of-E in appropriate order, we get:

∑ MY = 2 (0.2) – FC (0.2) = 0 ; FC = 2 kN

∑ FY = AY + 1 = 0 ; AY = – 1 kN

∑ MZ = – 2 (1.4) + BX (0.8) = 0 ; BX = – 3.5 kN

AZ

Ay

Z

AXX

BZ

BX2 kN

A FBD of the rod:

Y

FC

1 kN

Example B - continued

Page 34: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 34

∑ FX = AX – 3.5 + 2 = 0 ; AX = 1.5 kN

∑ MX = – 2 (0.4) + BZ (0.8) + 1 (0.2) = 0 ; BZ = 0.75 kN

∑ FZ = AZ + 0.75 – 2 = 0 ; AZ = 1.25 kN

AZ

Ay

Z

AXX

BZ

BX2 kN

A FBD of the rod:

Y

FC

1 kN

Example B - continued

If an additional couple moment in the vertical direction is applied to rod AB at point C, what will happen to the rod?

A) The rod remains in equilibrium as the cables provide the necessary support reactions.

B) The rod remains in equilibrium as the ball-and-socket joint will provide the necessary resistive reactions.

C) The rod becomes unstable as the cables cannot support compressive forces.

D) The rod becomes unstable since a moment about AB cannot be restricted.

Question

Page 35: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 35

The rod AB is supported using two cables at B and a ball-and-socket joint at A. How many unknown support reactions exist in this problem?

A) 5 force and 1 moment reaction

B) 5 force reactions

C) 3 force and 3 moment reactions

D) 4 force and 2 moment reactions

Question

1. If a support prevents rotation of a body about an axis, then the support exerts a ________ on the body about that axis.

A) couple moment

B) force

C) both A and B

D) none of the above

2. When doing a 3-D problem analysis, you have ________ scalar equations of equilibrium.

A) 2 B) 3 C) 4

D) 5 E) 6

Questions

Page 36: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 36

A plate is supported by a ball-and-socket joint at A, a roller joint at B, and a cable at C. How many unknown support reactions are there in this problem?

A) 4 forces and 2 moments

B) 6 forces

C) 5 forces

D) 4 forces and 1 moment

Question

What will be the easiest way to determine the force reaction BZ ?

A) Scalar equation ∑ FZ = 0

B) Vector equation∑ MA = 0

C) Scalar equation∑ MZ = 0

D) Scalar equation∑ MY = 0

Question

Page 37: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 37

• Identify support reactions in 3-D and draw a free body diagram

• Apply the equations of equilibrium

Summary

Announcements

Page 38: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 38

Due to an unequal distribution of fuel in the wing tanks, the centers of gravity for the airplane fuselage A and wings B and C are located as shown. If these components have weights WA = 45000 lb, WB = 8000 lb, and WC = 6000 lb, determine the normal reactions of the wheels D, E, and F on the ground.

Textbook Problem 5.68

FD = 22.6 kip

FE = 22.6 kip

FF = 13.7 kip

Determine the x and z components of reaction at the journal bearing A and the tension in cords BC and BDnecessary for equilibrium of the rod.

Example Problem

Ax = 0 N

FBD = 208 N

FBC = 792 N

AZ = 0 N

MAX = 0 Nm

MAZ = 700 Nm

Page 39: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 39

Determine the x, y, and z components of reaction at the pin A and the tension in the cable BC necessary for equilibrium of the rod.

Textbook Problem 5.84

FBC = 101 lb

AY = -140 lb

AZ = 77.8 lb

MAY = -389 lb-ft

MAZ = 93.3 lb-ft

The boom AC is supported at A by a ball-and-socket joint and by two cablesBDC and EC. Cable BDC is continuous and passes over a frictionless pulley at D. Calculate the tension in the cables and thex, y, and z components of reaction at A if the crate has a weight of 80 lb.

Example Problem

Answer: Unknown

Page 40: Announcements Equilibrium of a Rigid Body

Engr221 Chapter 5 40

The uniform table has a weight of 20 lb and is supported by the framework shown. Determine the smallest vertical force P that can be applied to its surface that will cause it to tip over. Where should this force be applied?

Textbook Problem 5.72

P = 14.1 lb, at the corner of the table

• Identify support reactions in 3-D and draw a free body diagram

• Apply the equations of equilibrium

Summary