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Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND STRENGTH OF MATERIALS ENDS 231 DR. ANNE NICHOLS SPRING 2008 three moments lecture

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Page 1: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 1Lecture 3

Architectural Structures IENDS 231

S2008abn

ARCHITECTURAL STRUCTURES I:STATICS AND STRENGTH OF MATERIALS ENDS 231

DR. ANNE NICHOLS

SPRING 2008

three

moments

lecture

Page 2: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 2Lecture 3

Architectural Structures IENDS 231

S2008abn

Moments• forces have the tendency to make a

body rotate about an axis

– same translation but different rotation

Page 3: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 3Lecture 3

Architectural Structures IENDS 231

S2008abn

Moments

Page 4: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 4Lecture 3

Architectural Structures IENDS 231

S2008abn

Moments• a force acting at a different point causes

a different moment:

Page 5: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 5Lecture 3

Architectural Structures IENDS 231

S2008abn

Moments• defined by magnitude and direction• units: N⋅m, k⋅ft• direction:

+ ccw (right hand rule)- cw

• value found from Fand ⊥ distance

• d also called “lever” or “moment” arm

F

AC

B

dFM ⋅=

d

Page 6: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 6Lecture 3

Architectural Structures IENDS 231

S2008abn

Moments• with same F:

21 dFMdFM AA ⋅=<⋅=(bigger)

Page 7: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 7Lecture 3

Architectural Structures IENDS 231

S2008abn

Moments• additive with sign convention• can still move the force

along the line of action

=

+MA = F⋅dMB = F⋅d′

d

F

A

Bd′

MA = F⋅d MB = F⋅d′

d

FA

Bd′

Page 8: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 8Lecture 3

Architectural Structures IENDS 231

S2008abn

Moments• Varignon’s Theorem

– resolve a force into components at a point and finding perpendicular distances

– calculate sum of moments– equivalent to original moment

• makes life easier!– geometry– when component runs through point, d=0

Page 9: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 9Lecture 3

Architectural Structures IENDS 231

S2008abn

Physics & Moments of a Force• moments of a force

– introduced in Physics as“Torque Acting on a Particle”

– and used to satisfy rotational equilibrium

Page 10: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 10Lecture 3

Architectural Structures IENDS 231

S2008abn

Physics and Moments of a Force• my Physics book:

Page 11: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 11Lecture 3

Architectural Structures IENDS 231

S2008abn

• 2 forces– same size– opposite direction– distance d apart– cw or ccw

– not dependant on point of application

Moment Couples

d

F

A

d1

d2

F

21 dFdFM ⋅−⋅=

dFM ⋅=

Page 12: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 12Lecture 3

Architectural Structures IENDS 231

S2008abn

Moment Couples• equivalent couples

– same magnitude and direction– F & d may be different

100 mm300 N

300 N

150 mm200 N

200 N

250 mm

120 N120 N

Page 13: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 13Lecture 3

Architectural Structures IENDS 231

S2008abn

Moment Couples• added just like moments caused by one

force• can replace two couples with a single

couple

+=

100 mm300 N

300 N

150 mm200 N

200 N

250 mm

240 N240 N

Page 14: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 14Lecture 3

Architectural Structures IENDS 231

S2008abn

Moment Couples• moment couples in structures

Page 15: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 15Lecture 3

Architectural Structures IENDS 231

S2008abn

Equivalent Force Systems• two forces at a point is equivalent to the

resultant at a point• resultant is equivalent to two

components at a point• resultant of equal & opposite forces at a

point is zero• put equal & opposite forces at a point

(sum to 0)• transmission of a force along action line

Page 16: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 16Lecture 3

Architectural Structures IENDS 231

S2008abn

• single force causing a moment can be replaced by the same force at a different point by providing the moment that force caused

• moments are shown as arched arrows

Force-Moment Systems

-F

FFd

AA′

F

AA′

Page 17: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 17Lecture 3

Architectural Structures IENDS 231

S2008abn

Force-Moment Systems• a force-moment pair can be replaced by

a force at another point causing the original moment

Fd

-F

F

AA′

F

AA′

F M=F⋅d

AA′

Page 18: three lecturefaculty.arch.tamu.edu/media/cms_page_media/4573/lect3_1.pdf · Moments 1 Lecture 3 Architectural Structures I ENDS 231 S2008abn ARCHITECTURAL STRUCTURES I: STATICS AND

Moments 18Lecture 3

Architectural Structures IENDS 231

S2008abn

Parallel Force Systems• forces are in the same direction• can find resultant force• need to find location for equivalent

moments

R=A+B

C Dx

AB

ab

aA ⋅

bB ⋅

xBA ⋅+ )(

C D