static force analysis - deukisi.deu.edu.tr/saide.sarigul/static_force_analysis.pdf · three-force...

13
STATIC FORCE ANALYSIS WEEK 1

Upload: truongtram

Post on 06-Mar-2018

232 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

STATIC FORCE ANALYSIS

WEEK 1

Page 2: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

COUPLE MOMENT OF COUPLE

Couple: Two equal and opposite forces (F & F’) Moment of Couple: A vector normal to the plane of the couple (M=RBAX F)

Page 3: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The
Page 4: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The
Page 5: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

Conditions of Equilibrium

A system of bodies is in equilibrium, if, and only if:

In 2-D (planar) systems:

Page 6: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

Two-Force Members

Not in equilibrium F0, M0

Not in equilibrium F=0, M0

In equilibrium F=0, M=0

Condition of equilibrium, for any two-force member with no applied torque: The forces are equal, opposite and have the same line of action.

Page 7: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

Three-Force Members

Not in equilibrium M0

In equilibrium F=0, M=0

O

Four-Force Members: The problem is reduced to one of three-force member. Then the approach above is applied.

Condition of equilibrium, for any three-force member with no applied torque: Forces should be coplanar

Page 8: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

Example (Graphical Solution) Link 3 is a two-force member

Page 9: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

b) 1 st approach:

c) 2 nd approach: Since link 4 is is a three-force member; lines of action of forces P, F

34

F14

should intersect at a point . Therefore direction of

d)

F14 is obtained.

Force triangle is used. If 1st approach was used, this triangle gives direction and magnitude of

If 2nd approach was used, this triangle gives magnitudes of F34 ,

F14

Since, graphically

F14

e) Action and reaction forces are equal: and f) F=0

Page 10: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

(Analytical Solution)

= 5(cos68.4i+sin68.4j) X 120(-cos40i-sin40j) +12(cos68.4i+sin68.4j) X F34 (cos 22.4i+sin 22.4j) = 0

F34 = 33.1 lb

Page 11: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

Problem (Analytical Solution) (without friction)

O2A=75 mm P=0.9 kN AB=350 mm M12 =?

F=0 F34+P+F14=0 F34(cos11,95i-sin11,95j)-900i+F14j=0 i: 0.978 F34 = F34x= 900 F34 = 920.25 N j: 0.207 F34 = F34y= F14 F14 = 190.5 N F34 = 920,25 /-11,95 N = 900i-190.5j N F14 = 190.5j N

For the moment balance, all of the force vectors should pass through point B.

Page 12: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

Two-force member F=0 F23=-F43=F34

F=0 F12=-F32=F23=F34

MO2=0 M12 + O2A x F32 = 0 M12k + 0.075(cos105i+sin105j) x (-900i+190.5j) = 0 M12k – 3.69k + 65.2k = 0 M12 = -61.51 N.m M12 = -61.51k N.m

Page 13: STATIC FORCE ANALYSIS - DEUkisi.deu.edu.tr/saide.sarigul/STATIC_FORCE_ANALYSIS.pdf · Three-Force Members Not in equilibrium M 0 In equilibrium F=0, M=0 O Four-Force Members: The

Problem (Analytical Solution) (with friction)

=0.2 (Between piston and cylinder)

F=0 F34+P+F14=0 F34+P+(0.2Ni+Nj)=0 F34(cos11.95i-sin11.95j)-900i+0.2Ni+Nj=0 i: 0.978 F34 -900+0.2N = 0 j: 0.207 F34 + N = 0 N = 0.207 F34 0.978 F34 -900+0.2(0.207F34)= 0 F34 = 882.61 Newton N=182.7 Newton F14 = 36.54i+182.7j Newton

F34 = 882.61 /-11,95 Newton = 863.48i-182.75j Newton

F=0 F12=-F32=F23=F34

MO2=0 M12 + O2A x F32 = 0 M12k + 0.075(cos105i+sin105j) x (-863.48i+182.75j) = 0 M12k – 3.547k + 62.55k = 0 M12 = -59.003 N.m M12 = -59.003k N.m CONCLUSION ?

0.2N