izmir institute of technology department of architecture ar231 fall12/13 15.01.2015 dr. engin aktaş...

21
IZMIR INSTITUTE OF TECHNOLOGY IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture Department of Architecture AR23 AR231 Fall12/13 Fall12/13 16.06.22 Dr. Engin Aktaş 1 Distributed Forces: Distributed Forces: Centroids and Centers of Gravity Centroids and Centers of Gravity

Upload: armani-hay

Post on 02-Apr-2015

225 views

Category:

Documents


3 download

TRANSCRIPT

Page 1: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 1

Distributed Forces: Distributed Forces: Centroids and Centers of GravityCentroids and Centers of Gravity

Page 2: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 2

Introduction

• The earth exerts a gravitational force on each of the particles forming a body. All these forces can be represented by a single equivalent force equal to the weight of the body and applied at the center of gravity for the body.

• The centroid of an area is similar to the center of gravity of a body. The concept of the first moment of an area is used to locate the center of gravity.

Page 3: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 3

Center of Gravity of a 2D Body• Center of gravity of a plate

dWy

WyWyM

dWx

WxWxM

x

y

• Center of gravity of a wire

Page 4: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 4

Centroids and First Moments of Areas and Lines

x

QdAyAy

y

QdAxAx

dAtxAtx

dWxWx

x

y

respect toh moment witfirst

respect toh moment witfirst

• Centroid of an area

dLyLy

dLxLx

dLaxLax

dWxWx

• Centroid of a line

Page 5: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 5

First Moments of Areas and Lines• An area is symmetric with respect to an axis BB’

if for every point P there exists a point P’ such that PP’ is perpendicular to BB’ and is divided into two equal parts by BB’.

• The first moment of an area with respect to a line of symmetry is zero.

• If an area possesses a line of symmetry, its centroid lies on that axis

• If an area possesses two lines of symmetry, its centroid lies at their intersection.

• An area is symmetric with respect to a center O if for every element dA at (x,y) there exists an area dA’ of equal area at (-x,-y).

• The centroid of the area coincides with the center of symmetry.

Page 6: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 6

Centroids of Common Shapes of Areas

Page 7: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 7

Centroids of Common Shapes of Lines

Page 8: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 8

Composite Plates and Areas• Composite plates

WyWY

WxWX

• Composite area

AyAY

AxAX

Page 9: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 9

Sample Problem 5.1

For the plane area shown, determine the first moments with respect to the x and y axes and the location of the centroid.

SOLUTION:

• Divide the area into a triangle, rectangle, and semicircle with a circular cutout.

• Compute the coordinates of the area centroid by dividing the first moments by the total area.

• Find the total area and first moments of the triangle, rectangle, and semicircle. Subtract the area and first moment of the circular cutout.

• Calculate the first moments of each area with respect to the axes.

Page 10: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 10

Sample Problem 5.1

33

33

mm10758

mm10506

y

x

Q

Q• Find the total area and first moments of the triangle, rectangle, and semicircle. Subtract the area and first moment of the circular cutout.

Page 11: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 11

Sample Problem 5.1

23

33

mm1013.828

mm107.757

A

AxX

mm 8.54X

23

33

mm1013.828

mm102.506

A

AyY

mm 6.36Y

• Compute the coordinates of the area centroid by dividing the first moments by the total area.

Page 12: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 12

Determination of Centroids by Integration

ydxy

dAyAy

ydxx

dAxAx

el

el

2

dyxay

dAyAy

dyxaxa

dAxAx

el

el

2

drr

dAyAy

drr

dAxAx

el

el

2

2

2

1sin

3

2

2

1cos

3

2

dAydydxydAyAy

dAxdydxxdAxAx

el

el• Double integration to find the first moment

may be avoided by defining dA as a thin rectangle or strip.

Page 13: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 13

Sample Problem 5.4

Determine by direct integration the location of the centroid of a parabolic spandrel.

SOLUTION:

• Determine the constant k.

• Evaluate the total area.

• Using either vertical or horizontal strips, perform a single integration to find the first moments.

• Evaluate the centroid coordinates.

Page 14: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 14

Sample Problem 5.4SOLUTION:

• Determine the constant k.

2121

22

22

2

yb

axorx

a

by

a

bkakb

xky

• Evaluate the total area.

3

30

3

20

22

ab

x

a

bdxx

a

bdxy

dAA

aa

Page 15: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 15

Sample Problem 5.4• Using vertical strips, perform a single integration

to find the first moments.

1052

2

1

2

44

2

0

5

4

2

0

22

2

2

0

4

2

0

22

abx

a

b

dxxa

bdxy

ydAyQ

bax

a

b

dxxa

bxdxxydAxQ

a

a

elx

a

a

ely

Page 16: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 16

Sample Problem 5.4• Or, using horizontal strips, perform a single

integration to find the first moments.

10

42

1

22

2

0

2321

2121

2

0

22

0

22

abdyy

b

aay

dyyb

aaydyxaydAyQ

badyy

b

aa

dyxa

dyxaxa

dAxQ

b

elx

b

b

ely

Page 17: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 17

Sample Problem 5.4• Evaluate the centroid coordinates.

43

2baabx

QAx y

ax4

3

103

2ababy

QAy x

by10

3

Page 18: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 18

Distributed Loads on Beams

• A distributed load is represented by plotting the load per unit length, w (N/m) . The total load is equal to the area under the load curve. AdAdxwW

L

0

AxdAxAOP

dWxWOP

L

0

• A distributed load can be replaced by a concentrated load with a magnitude equal to the area under the load curve and a line of action passing through the centroid of the area.

Page 19: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 19

Sample Problem 5.9

A beam supports a distributed load as shown. Determine the equivalent concentrated load and the reactions at the supports.

SOLUTION:

• The magnitude of the concentrated load is equal to the total load or the area under the curve.

• The line of action of the concentrated load passes through the centroid of the area under the curve.

• Determine the support reactions by summing moments about the beam ends.

Page 20: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 20

Sample Problem 5.9SOLUTION:

• The magnitude of the concentrated load is equal to the total load or the area under the curve.

kN 0.18F

• The line of action of the concentrated load passes through the centroid of the area under the curve.

kN 18

mkN 63 X m5.3X

Page 21: IZMIR INSTITUTE OF TECHNOLOGY Department of Architecture AR231 Fall12/13 15.01.2015 Dr. Engin Aktaş 1 Distributed Forces: Centroids and Centers of Gravity

IZMIR INSTITUTE OF TECHNOLOGYIZMIR INSTITUTE OF TECHNOLOGY Department of ArchitectureDepartment of Architecture AR23AR2311 Fall12/13Fall12/13

11.04.23 Dr. Engin Aktaş 21

Sample Problem 5.9• Determine the support reactions by summing

moments about the beam ends.

0m .53kN 18m 6:0 yA BM

kN 5.10yB

0m .53m 6kN 18m 6:0 yB AM

kN 5.7yA