outline: centres of mass and centroids

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Outline: Centres of Mass and Centroids Centre of Mass Centroids of Lines, Areas and Volumes Composite Bodies Beams – External Effects Beams – Internal Effects ENGR 1205 Chapter 5 1

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Page 1: Outline: Centres of Mass and Centroids

Outline:

Centres of Mass and Centroids ◦ Centre of Mass

◦ Centroids of Lines, Areas and Volumes

◦ Composite Bodies

Beams – External Effects

Beams – Internal Effects

ENGR 1205 Chapter 5 1

Page 2: Outline: Centres of Mass and Centroids

Up to now all forces have been concentrated forces (force applied at single point)

But forces are actually applied over some contact area

If contact area is significant compared to the other dimensions we must account for it

Sum the effects of the distributed force over the contact region using mathematical integration

ENGR 1205 Chapter 5 2

Page 3: Outline: Centres of Mass and Centroids

Three types of Force Distribution (see fig. 5/2):

◦ Line Distribution - vertical load supported along a cable

Intensity is in N/m

◦ Area Distribution - hydraulic water pressure against dam face

Intensity is in 𝑁/𝑚2 or Pascal (Pa)

Called pressure for the action or fluid forces

Called stress for internal distribution in solids

◦ Volume Distribution - gravitational attraction

Intensity is in N/m3

For gravity the intensity is the specific weight (density times gravitational field strength ρg)

ENGR 1205 Chapter 5 3

Page 4: Outline: Centres of Mass and Centroids

For external forces a concentrated load can be used to replace a distributed load

Need to find the position for a concentrated load that will give an equivalent system

Typically, we are dealing with weight

Need to find Centre of Gravity/Mass for rigid bodies (for location of load)

Also, we need to be able to analyze the internal forces caused by distributed loads

ENGR 1205 Chapter 5 4

Page 5: Outline: Centres of Mass and Centroids

Integration is the inverse of differentiation

The integral of a function is a measure of the area between it and the x-axis

The symbol of integration is ∫ , an elongated S (stands for "sum").

The integral is written as

and is read "the integral of f-of-x with respect to x."

ENGR 1205 Chapter 5 5

b

a

dxxf )(

Page 6: Outline: Centres of Mass and Centroids

Example:

If we know that (dy/dx)=3x2 and we need to know the function this derivative came from, then we "undo" the differentiation process.

y = x3 is ONE antiderivative of 3x2 (since the derivative of any constant is zero)

In general: y = x3 + C, is the indefinite integral, C is called the constant of integration

Indefinite integrals deal with algebraic quantities (define an entire function)

ENGR 1205 Chapter 5 6

Page 7: Outline: Centres of Mass and Centroids

Integrals with a definite bound are definite integrals

The definite integral is written as

and is read "the integral from a to b of f-of-x with respect to x."

a and b are the lower limit and upper limit, respectively, of integration, defining the domain of integration;

f is the integrand, to be evaluated as x varies over the interval [a,b];

and dx is the variable of integration.

ENGR 1205 Chapter 5 7

b

a

dxxf )(

Page 8: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 8

Back to the example:

to evaluate the integral of 3x2 between x=1 and x=5:

Some integration rules and properties

124)1()5(3

5

1

335

1

32 xdxx

Cn

xdxx

dvdxdvdx

dxaadx

Cxdx

nn

1

1

Page 10: Outline: Centres of Mass and Centroids

Rigid Body

◦ The center of mass is a unique point whose location is a function of the distribution of mass throughout the body

◦ It is the point through which the total weight vector acts

ENGR 1205 Chapter 5 10

G G

A B B A

Page 11: Outline: Centres of Mass and Centroids

Consider a 2D body: Divide the plate into n small elements each with weight DW and coordinates x & y

ENGR 1205 Chapter 5 11

Page 12: Outline: Centres of Mass and Centroids

W

zdWz

W

ydWy

W

xdWx

dWW

ENGR 1205 Chapter 5 12

co-ordinates for the

center of gravity:

Page 13: Outline: Centres of Mass and Centroids

For a Wire:

gA

LgAW

gALW

DD

ENGR 1205 Chapter 5 13

W

zdWz

W

ydWy

W

xdWx

L

zdLz

L

ydLy

L

xdLx

ρ (density), g, and A (the cross-

sectional area) are constant over the

length (L)

Page 14: Outline: Centres of Mass and Centroids

For an Area:

gt

AgtW

gtAW

DD

ENGR 1205 Chapter 5 14

W

zdWz

W

ydWy

W

xdWx

A

zdAz

A

ydAy

A

xdAx

ρ (density), g, and t (the thickness)

are constant over the surface area (A)

Page 15: Outline: Centres of Mass and Centroids

For a Volume:

g

VgW

gVW

DD

ENGR 1205 Chapter 5 15

V

zdVz

V

ydVy

V

xdVx

ρ (density), and g are constant over

the volume (V)

W

zdWz

W

ydWy

W

xdWx

Page 16: Outline: Centres of Mass and Centroids

Steps to solve:

Choose a differential element for integration

Express dA, dL or dV in terms of 1 variable

Express x, y or z (location of centroid of element) in terms of 1 variable

Substitute into equations and integrate

Use axes of symmetry whenever possible

ENGR 1205 Chapter 5 16

zdLzL

ydLyL

xdLxL

zdAzA

ydAyA

xdAxA

zdVzV

ydVyV

xdVxV

Page 17: Outline: Centres of Mass and Centroids

Find the centroid of the area under y=x2 ?

ENGR 1205 Chapter 5 17

Page 18: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 18

Expression for differential element

(tiny rectangle)

Integrate to get expression for A

Page 19: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 19

ANSWER: The centroid of the area is 3

4 ,3

10 m

Page 20: Outline: Centres of Mass and Centroids

Find the centroid of the cone, with radius “a” and height “h” ?

ENGR 1205 Chapter 5 20

Page 21: Outline: Centres of Mass and Centroids

An irregularly shaped area may be divided into the smaller shapes with known G’s

Summing moments as before:

For plates and wires with uniform thickness and homogeneous material:

ENGR 1205 Chapter 5 21

ii

ii

ii

AzAZ

AyAY

AxAX

ii

ii

ii

LzLZ

LyLY

LxLX

332211321 )( xWxWxWXWWW

Page 22: Outline: Centres of Mass and Centroids

An irregularly shaped body may be divided into smaller shapes with known G’s (see Appendix D for centroids of common shapes)

As before:

ENGR 1205 Chapter 5 22

ii

ii

ii

WzWZ

WyWY

WxWX

ii

ii

ii

VzVZ

VyVY

VxVX

Page 23: Outline: Centres of Mass and Centroids

Steps to solve a composite body:

Choose a reference frame

Divide the composite area/volume into parts whose centroids you know (APPENDIX D) or can easily determine

Determine the coordinates of the centroids and the volume/ area/ length for each part

Watch for cases of symmetry that can simplify calculations

ENGR 1205 Chapter 5 23

Page 24: Outline: Centres of Mass and Centroids

Find the centroid of the L-shaped bar of negligible thickness.

ENGR 1205 Chapter 5 24

1 m

1 m

Page 25: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 25

Page 26: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 26

Page 27: Outline: Centres of Mass and Centroids

Find the centroid of the irregularly-shaped plate below. All dimensions in cm.

ENGR 1205 Chapter 5 27

50

40

20

30 40 80

y

x

r=10

Page 28: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 28

Page 29: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 29

PART A x Y xA yA

1

2

3

4

Sum

Page 30: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 30

Page 31: Outline: Centres of Mass and Centroids

Locate the center of mass of the composite body made of a conical frustrum and a hemisphere, shown below.

ENGR 1205 Chapter 5 31

Page 32: Outline: Centres of Mass and Centroids

Beams are bars of material that support lateral loads (perpendicular to the axis of the beam)

Beams are probably the most important structural member

Beams can support both concentrated and distributed loads

Analyze load carrying capacity of beams for:

◦ Equilibrium and external reactions

◦ Internal Resistance (strength characteristics)

ENGR 1205 Chapter 5 32

Page 33: Outline: Centres of Mass and Centroids

We will only analyze statically determinate beams in this class

ENGR 1205 Chapter 5 33

Page 34: Outline: Centres of Mass and Centroids

Distributed loads: intensity w of a distributed load is expressed as force per unit length of the beam (can be constant or variable)

The resultant of the distributed load is equal to the area formed by the intensity w and the length

The resultant of the distributed load passes through the centroid of the area

ENGR 1205 Chapter 5 34

Page 35: Outline: Centres of Mass and Centroids

For a more general load distribution:

ENGR 1205 Chapter 5 35

𝑅 = 𝒘𝑑𝑥

𝑅𝑥 = 𝑥𝒘𝑑𝑥

Page 36: Outline: Centres of Mass and Centroids

To Determine External Reactions for Beams:

Reduce each distributed load to an equivalent concentrated load (find total force applied and location)

Use given concentrated loads and equivalent concentrated loads with 2-D equations of equilibrium

ENGR 1205 Chapter 5 36

Page 37: Outline: Centres of Mass and Centroids

A beam is subjected to the loads shown. Determine the reactions at the supports A & B.

ENGR 1205 Chapter 5 37

Page 38: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 38

TOTAL AREA (RESULTANT FORCE) CENTROID (POINT OF ACTION)

1 12 ∗ 2 m ∗ 300 N/m = 300 N 2

3∗ 2 m =

4

3 m = 1.33 m

2 6 m ∗ 300 N/m = 1800 N 1

2∗ 6 m + 2 m = 5 m

3 12 ∗ (4 m) ∗ (300 N/m) = 600 N 1

3∗ 4 m + 8 m = 9.33 m

Given: See FBD

Find: Ax, Ay, By

Page 39: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 39

For Equilibrium 𝚺𝑴 = 𝟎 & 𝚺𝑭 = 𝟎

𝚺𝑴𝑨 = −𝟑𝟎𝟎 𝟏. 𝟑𝟑 − 𝟏𝟖𝟎𝟎 𝟓 − 𝟔𝟎𝟎 𝟗. 𝟑𝟑 + 𝑩𝒀 𝟏𝟐 = 𝟎 𝑩𝒀 = 𝟏𝟐𝟓𝟎 𝑵

𝚺𝑭𝑿 = 𝟎 𝑨𝑿 = 𝟎 N

𝚺𝑭𝒀 = 𝟎 𝑨𝒀 − 𝟑𝟎𝟎 − 𝟏𝟖𝟎𝟎 − 𝟔𝟎𝟎 + 𝑩𝒀 = 𝟎 𝑨𝒀 = 𝟏𝟒𝟓𝟎 𝑵

ANSWER: The reactions at the supports are 𝐀𝐘 = 𝟏𝟒𝟓𝟎 𝐍 [𝐮𝐩] & 𝐁𝐘 = 𝟏𝟐𝟓𝟎 𝐍 [𝐮𝐩]

Page 40: Outline: Centres of Mass and Centroids

Beams can resist:

Tension/ Compression

Shear force (V)

Bending moment (M)

Torsional moment (T)

The amount of each kind of internal load can change throughout the length of the beam, depending on external loads

ENGR 1205 Chapter 5 40

Page 41: Outline: Centres of Mass and Centroids

We can ‘cut’ the beam at any point along its length to analyze the internal forces at that point

It is often difficult to tell the direction of the shear and moment without calculations so represent V and M in their positive directions and let the result tell you (+/-) whether you drew it the right way

CONVENTION

ENGR 1205 Chapter 5 41

Page 42: Outline: Centres of Mass and Centroids

The maximum bending moment is often the primary consideration in the design of a beam

Variations in shear and moment are best shown graphically

ENGR 1205 Chapter 5 42

Page 43: Outline: Centres of Mass and Centroids

Use equilibrium of whole beam to find reaction forces

Then cut beam ___________ concentrated loads, replace any distributed loads with _________________ and solve for unknown shear and moment at _________________.

Plot V (shear vs x) and M (moment vs x) along the beam

ENGR 1205 Chapter 5 43

Page 44: Outline: Centres of Mass and Centroids

Solve for R1 and R2

Isolate left section & solve for V and M between the left support & 4kN load

Isolate right section and solve for V and M between the right support & 4kN load

Isolate a section between every change in an external load, but DO NOT CUT the section at the concentrated load

The area under a shear curve between two points is equal to the change in bending moment between the same two points.

ENGR 1205 Chapter 5 44

Page 45: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 45

Given: See Diagram

Find: Maximum bending moment

Draw shear force and bending moment diagrams

Solve: For Equilibrium 𝐹 = 0 and 𝑀 = 0

Page 46: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 46

Page 47: Outline: Centres of Mass and Centroids

ENGR 1205 Chapter 5 47

Page 48: Outline: Centres of Mass and Centroids

Draw the shear and bending moment diagrams for the beam and loading shown and determine the location and magnitude of the maximum bending moment.

ENGR 1205 Chapter 5 48

Page 49: Outline: Centres of Mass and Centroids

Draw the shear and bending moment diagrams for the beam and loading shown.

ENGR 1205 Chapter 5 49