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Lecture 18 November 5, 2018 Statics - TAM 211

Lecture 18 November 5, 2018 - Statics - TAM 211

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Lecture 18

November 5, 2018

Statics - TAM 211

Announcements

Upcoming deadlines:

Tuesday (11/6) Prairie Learn HW 7

Friday (11/9) Written Assignment 7

Chapter 6: Structural Analysis

Note that in Chapter 5, a rigid body could have more than two forces and more than two pin joints. For TRUSS structures in Chapter 6, these structures are made of ONLY links, which are 2FMs with only 2 pin joints.

Goals and Objectives• Determine the forces in members of a truss using the method of

joints

• Determine zero-force members

• Determine the forces in members of a truss using the method of sections

• Determine the forces and moments in members of a frame or machine

Assumption of trusses Loading applied at joints, with negligible weight (If

weight included, vertical and split at joints) Members joined by smooth pins

Pins in equilibrium:∑ 0and ∑ 0Zero-force members

Two situations: Two non-collinear members , no external or support

at jt Both members are ZFM Two collinear member, plus third non-collinear, no

loads on third member Non-collinear member is ZFM.

Method of jointsProcedure for analysis to find forces within links: Determine external support reactions Free-body diagram for each joint Start with joints with at least 1 known force

and 1-2 unknown forces Assume the unknown force members to be in tension

Recap: Truss Analysis

RECAP: Use Method of joints to prove that members attached to A and D should be FZM

The truss, used to support a balcony, is subjected to the loading shown. Approximate each joint as a pin and determine the force in each member. State whether the members are in tension or compression.

A

P1 P2

Cx

Ex

Cy

B C

DE

a

a

y

xa

Solution:Start by setting the entire structure into external equilibrium. Draw the FBD.

1 2

1 2

0 : 0 ,0 : 0 ,

0 : 2 0 .

x x x

y y

C x

F C EF C P P

M aP aP aE

1 2 1 2 1 22 , , (2 ) .x y xC P P C P P E P P

Solving these equations gives the external reactions

Equilibrium requires ∑ and ∑

Next, start with a joint, draw the FBD, set it into force equilibrium only, and move to the next joint. Start with joints with at least 1 known force and 1-2 unknown forces.

11

A

P1

FAB

FAD

12

11 2

0 : 0 ,

0 : 0 .x AB AD

y AD

F F F

F P F

11 1 12

2 , 2 .AD ABF P F P P

P2

BFAB FBC

FBD

For example, start with joint A:

Joint B:

2

0 : 0 ,0 : 0 .

x AB BC

y BD

F F FF P F

1 2, .BC AB BDF F P F P

Joint C:

11 22

11 22

0 : 2 0 ,

0 : 0 .x BC CD

y CD

F F F P P

F F P P

C1

1

FBC

FCD

P1 + P2

2P1 + P2

1 2 1 1 2

1 2

2(2 ) 2( ) ,

2( ) (check) .CD

CD

F P P P P P

F P P

11

11 D

FCD

FDE

FADFBD

E 2P1 + P2FDE

Joint D: only needed for check

Joint E:

1 12 2

1 12 2

0 : 0 ,

0 : 0 .x AD CD DE

y AD BD CD

F F F F

F F F F

1 11 1 2 1 22 2

1 11 2 1 22 2

2 2( ) (2 ) ,

2 2( ) 0 (check) .

DEF P P P P P

P P P P

1 2 1 2 1 22 , , (2 ) .x y xC P P C P P E P P

Note: The checks would not have been satisfied if the external reactions had been calculated incorrectly.

Note: The order in which the joints are set in equilibrium is usually arbitrary. Sometimes not all member loads are requested.

1

1

1

2

1 2

1 2

800 lb (T)800 lb (T)

2 1130 lb (C)0

2( ) 1130 lb (T)(2 ) 1600 lb (C)

AB

BC

AD

BD

CD

DE

F PF P

F PF P

F P PF P P

A

P1 P2

B C

DE

Tens

Compr

Compr

Compr

Tens

Tens

Note that, in the absence of , member BD is a zero-force member

1 800 lbP

2 0P

If provided numerical values:

Note: Seven scalar equations of equilibrium were needed to obtain this answer. Might there be a shorter way?

• Determine external support reactions (if necessary)• “Cut” the structure at a section of interest into two

separate pieces and set either part into force and moment equilibrium (your cut should be such that you have no more than three unknowns)

• Extend lines at cut to find point of intersection• Draw unknown truss forces in cut member

• Determine equilibrium equations (e.g., moment around point of intersection of two lines)• Assume all internal loads are tensile.

Method of sections (Use to solve for specific link force)

Method of sections• Determine equilibrium equations (e.g., moment

around point of intersection of two lines)

• Assume all internal loads are tensile.

Determine the force in member BC of the truss and state if the member is in tension or compression.

Determine the force in member BC of the truss and state if the member is in tension or compression.

400

300

Determine the force in members OE, LE, LK of the Baltimore truss and state if the member is in tension or compression.

Ax

Ay Iy

8a

a

a

0 : 0 ,

0 : 2 2 5 3 0 ,

0 : 2 (2) 3 (2) 4 (5) 5 (3) 8 0 .

x x

y y y

A y

F A

F A I

M a a a a aI

0, 6.375 kN, 5.625 kN.x y yA A I

Ax

Ay Iy

8a

a

a

Cut

Normally, introducing four unknowns would make the problem intractable. However, LEis a zero-force member. Set either remaining section into equilibrium. Here, there is no real preference, but the right half will be fine

(2) Use method of sections, since cutting LK, LE, OE, and DE will separate the truss into two pieces. Note that LE is a zero-force member. Solution:

(1) Draw free-body diagram of entire structure, and set into external equilibrium:

FDE

FEOFEL

FKL

Iy = 5.625 kN

2a

a a a a

12

12

0 : 0 ,

0 : 0 5 3 0 ,

0 : 0(5) ( 3) 4 2 0 .

x DE EO KL

y EO y

E y KL

F F F F

F F I

M a aI aF

Ax

Ay Iy

8a

a

a

+7.38

+3.36

Loads in kN0

7.38 kN (T), 0 (zero-force),3.36 kN (T), 9.75 kN (C).

DE EL

EO KL

F FF F

Ax

Ay Iy

8a

a

a

+7.38

+3.36

Loads in kN0

Notes added after class:At the end of lecture today, students asked why is link LE a ZFM since joint E has an applied load of 5kN?

The answer can be determined by examining the situation definitions of a ZFM, which were given in Lecture 17. These situations allow us to find ZFMs by inspection (i.e., by looking without calculations).Note that these definitions are with respect to the forces and links at a specific joint.

Therefore for the structure to the above-left, there are no external or support reaction forces on joint L; thus LE is a ZFM. We see the same for joints C & D in bottom-middle structure (links DA & CA are ZFM), and joint E in bottom-right structure (link BE is ZFM).