36
ENGR 3340: Fundamentals of Statics and ENGR 3340: Fundamentals of Statics and Dynamics Dynamics Fundamentals of Statics and Fundamentals of Statics and Dynamics - ENGR 3340 Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo Professor: Dr. Omar E. Meza Castillo [email protected] http://facultad.bayamon.inter.edu/omeza Department of Mechanical Engineering Department of Mechanical Engineering

ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

Embed Size (px)

DESCRIPTION

MSP21 Universidad Interamericana - Bayamón ENGR 3340: Fundamentals of Statics and Dynamics Equilibrium Topic 5: Equilibrium of a Particle in 2-D 3 One thing you learn in science is that there is no perfect answer, no perfect measure. A. O. Beckman

Citation preview

Page 1: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

Fundamentals of Statics and Fundamentals of Statics and Dynamics - ENGR 3340Dynamics - ENGR 3340

Professor: Dr. Omar E. Meza CastilloProfessor: Dr. Omar E. Meza [email protected]

http://facultad.bayamon.inter.edu/omezaDepartment of Mechanical EngineeringDepartment of Mechanical Engineering

Page 2: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

2

Tentative Lectures Schedule

TopicTopic LectureLectureEquilibrium of a Particle in 2-DEquilibrium of a Particle in 2-D 55

Page 3: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

EquilibriumEquilibrium

Topic 5: Equilibrium of a Particle in 2-D

3

One thing you learn in science is that there is One thing you learn in science is that there is no perfect answer, no perfect measure.no perfect answer, no perfect measure.

A. O. BeckmanA. O. Beckman

Page 4: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Objectives

To introduce the concept of the free-body diagram for a particle

To show how to solve particle equilibrium problems using the equations of equilibrium

4

Page 5: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Equilibrium of a Particle Applications

For a spool of given For a spool of given weight, what are weight, what are the the forcesforces in cables in cables AB and AC ?AB and AC ?

5

Page 6: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Equilibrium of a Particle Applications (continued)

For a given cable For a given cable strength, what is strength, what is the the maximum maximum weight weight that can be that can be lifted ?lifted ?

6

Page 7: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Equilibrium of a Particle Applications (continued)

7

For a given weight For a given weight of the motor, what of the motor, what are the are the forcesforces in in the cables? What the cables? What size of cable must size of cable must you use ?you use ?

Page 8: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Equilibrium of a Particle Applications (continued)

8

Static EquilibriumStatic Equilibrium

Page 9: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Balancing Forks

9

Materials:

Page 10: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Balancing Forks

10

Step 1:

Page 11: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Balancing Forks

11

Step 2:

Page 12: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Balancing Forks

12

Page 13: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Coke Can Balancing

13

Materials:

Page 14: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Coke Can Balancing

14

Step 1:

Page 15: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Coke Can Balancing

15

Step 2:

Page 16: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Coke Can Balancing

16

Step 3:

Page 17: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Coke Can Balancing

17

Page 18: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics 3.1 Condition for the Equilibrium of a Particle.

18

Particle is said to be in EQUILIBRIUMEQUILIBRIUM if: It remains at rest (v=0) if originally at rest.

(Static Equilibrium)(Static Equilibrium) It has a constant velocity if originally in motion.

To maintain EQUILIBRIUMEQUILIBRIUM, it is necessary to satisfy Newton’s first law of motion. Resultant force Resultant force acting on a particle require to be zerozero.

where ∑F is the vector sum of all the forces acting on the particle.

0 FEquation of EquilibriumEquation of Equilibrium

Page 19: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics 3.1 Condition for the Equilibrium of a Particle.

19

Consequently, the particle indeed moves with constant velocity or remains at rest.

For Equilibrium:For Equilibrium:

0maF ==∑ 0a =

0Fx =∑

0Fy =∑

Page 20: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics 3.2 The Free-Body Diagram (FBD)

20

To apply the EQUATION OF EQUILIBRIUMEQUATION OF EQUILIBRIUM, we must account for ALL THE KNOWN ALL THE KNOWN and UNKNOWN FORCESUNKNOWN FORCES which act ONON the particle

In order to account for all the forces that act on the particle, it is necessary to draw its FREE-FREE-BODY DIAGRAMBODY DIAGRAM (FBD). (FBD).

The free-body diagram is simple a SKETCHSKETCH which shows the particle “FREE”“FREE” from its surrounding with ALLALL the forces that act on it.

FBDFBD

Page 21: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Types of Connections

21

Two types of connections often encountered in particle equilibrium SPRINGSSPRINGS and CABLES and CABLES and PULLEYS.PULLEYS.

SPRINGS:SPRINGS: The magnitude of force exerted on a linearly elastic spring is:

ksF =which has a stiffness which has a stiffness kk and is and is deformed (elongate or deformed (elongate or compressed) a distance compressed) a distance ss, , measured from its unloaded measured from its unloaded position.position. ol_ls =WhereWhere l loo the original length and the original length and ll the final the final lengthlength

Page 22: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Types of Connections

22

CABLES and PULLEYS: CABLES and PULLEYS: All cables are assumed to have negligible weight negligible weight and they cannot cannot stretch.stretch.

A cable can support only a tension or “pulling” force, and this force always act in the direction of the cable.

The tension in a cable is constant throughout its length.

Page 23: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Procedure for Drawing a Free-Body Diagram:

23

Draw Outlined Shape: Draw Outlined Shape: Imagine the particle to be isolated or cut “free” from its surrounding with all the forces outlined shape.

Show All Forces: Show All Forces: Indicate on this sketch all the forces that act on the particle.

Identify Each Force: Identify Each Force: The forces which are known should be labeled with their proper magnitudes and directions. Letter are used to represent the magnitudes and directions of forces that are unknown.

Page 24: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Example 1

The sphere has a mass of 6 kg 6 kg and is supported as shown. Draw a free-body diagram free-body diagram of the spheresphere, the cord CEcord CE, and the knot at Cknot at C.

24

Page 25: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Solution 1

Sphere:Sphere: There are two forces acting on the sphere: The weight of the sphere

W=6kg(9.81m/sW=6kg(9.81m/s22)=58.9N)=58.9N The force FCE of the cord CE acting on the sphere

The Free-Body DiagramThe Free-Body Diagram

25

Page 26: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Solution 1

Cord CE: Cord CE: When the cord CE is isolated from its surroundings, its free-body diagram shows only two forces acting on it: The force of the sphere and FCE. The force of the knot FEC

The Free-Body DiagramThe Free-Body Diagram

26

FFCECE=F=FECEC

Page 27: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Solution 1

Knot: Knot: The knot at C is subjected to three forces. They are caused by the cords CBA and CE and the spring CD:

The Free-Body DiagramThe Free-Body Diagram

27

Page 28: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics 3.3 Coplanar Force Systems

28

If a particle is subjected to a SYSTEM OF SYSTEM OF COPLANAR FORCESCOPLANAR FORCES that lie in the x-y plane. Then each force can be resolvedresolved into ii and j j componentscomponents

For EQUILIBRIUMEQUILIBRIUM, these forces must SUMSUM to produce a ZERO RESULTANTZERO RESULTANT. Hence:0=F∑

0=++∑∑ jFiF yx

0=∑ xF

0=∑ yF

Page 29: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Example 2

Determine the tensiontension in cables BABA and BCBC necessary to support the 60-kg60-kg cylinder.

29

Page 30: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Solution 2

Due to EQUILIBRIUMEQUILIBRIUM, the weightweight of the cylinder causes the tensiontension in cable BDBD to be:

The forces in cable BABA and BCBC can be determined by investigating the equilibrium of equilibrium of the ring the ring BB. Its free body diagram is then:

30

N6.588=)81.9(60=TBD

Page 31: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Solution 2

The magnitudes of TA and TC are unknown, but their directions are known.

31

Page 32: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics Solution 2

Equations of equilibrium along the x and y axes:

32

0=Fx∑

0=Fy∑

Page 33: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

33

Page 34: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

Homework3 http://facultad. bayamon.inter.edu/omeza/

Omar E. Meza Castillo Ph.D.Omar E. Meza Castillo Ph.D.

34

Page 35: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

3535

¿Preguntas?¿Preguntas?

Comentarios Comentarios

Page 36: ENGR 3340: Fundamentals of Statics and Dynamics Fundamentals of Statics and Dynamics - ENGR 3340 Professor: Dr. Omar E. Meza Castillo

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

MSP

21

U

nive

rsid

ad In

tera

mer

ican

a -

Baya

món

Baya

món

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

ENGR

334

0: F

unda

men

tals

of S

tatic

s and

Dyn

amics

3636

GRACIASGRACIAS