Top Banner
EQUILIBRIUM APPLICATION OF THE FIRST LAW
31
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Equilibrium

EQUILIBRIUM

APPLICATION OF THE FIRST LAW

Page 2: Equilibrium

STATIC EQUILIBRIUM• A state of balance of an object at

rest.• A condition in which all forces

acting on the body are balanced, causing the body to remain at rest.

What is equilibrium?

HOW DO WE KNOWIF THE OBJECT IS

IN EQUILIBRIUM?

Page 3: Equilibrium

CENTER OF GRAVITY

Page 4: Equilibrium

Center of Gravity

•The location where all of the weight of an object seemed to be concentrated.

Page 5: Equilibrium

How do we locate the C.G?

• For a regularly-shaped object, it is at its geometric center.

Page 6: Equilibrium

Center of Gravity

Height, h

C.G.

1/3 h1/4 h

C.G.

Solid cone Triangle

Page 7: Equilibrium

• Sometimes the C.G. is found outside the body.

How do we locate the C.G?

C.G

Page 8: Equilibrium

• For an irregularly-shaped object,• it could be determined by balancing it by

trial and error method or by the plumb bob method

Locating the C.G. of Irregularly-shaped object

Assignment: In one long folder, draw the island of Luzon. Cut it out and locate its center of gravity. Mark it with a pen. At the back of the cut-out folder, write how you determined the location of the C.G.

Page 9: Equilibrium

STATES OF EQUILIBRIUM

Any object at rest may be in one of three states of equilibrium.

• STABLE• UNSTABLE and• NEUTRAL

Page 10: Equilibrium

STABLE EQUILIBRIUM

• the C.G. is at lowest possible position.• the C.G. needs to be raised in order to topple

the object.• they are difficult to topple over.

For stable objects:

Page 11: Equilibrium

UNSTABLE EQUILIBRIUM

• the C.G. is at the highest possible position.• the C.G. is lowered in order to topple the object.• They are easy to topple down.

For unstable objects:

Page 12: Equilibrium

NEUTRAL EQUILIBRIUM

• the C.G. is neither lowered nor raised when the object is toppled.

• they roll from one side to another.

For objects with neutral equilibrium:

Page 13: Equilibrium

TOPPLING

Physics

by A

lvea Jo

i Sika

t

Physics by Alvea Joi Sikat

Physics

by A

lvea Jo

i Sika

t

Toppling the upright book requires only a slight raising of C.G.

Page 14: Equilibrium

TOPPLING

Physi

cs b

y A

lvea Joi Sik

at

Physics by Alvea Joi Sikat Phys

ics

by

Alv

ea Joi Sik

atToppling the flat book

requires a relatively large raising of its C.G.

Page 15: Equilibrium

TOPPLINGToppling the cylinder does not change the height of its C.G.

Page 16: Equilibrium

3 FACTORS FOR STABILITY1. Mass of the object2. Location of the center of gravity3. Area of the base of support

Page 17: Equilibrium
Page 18: Equilibrium

The First ConditionOf Equilibrium

Page 19: Equilibrium

EQUILIBRIUM

• What force/s are acting on the block of wood? Draw a free-body diagram.

Page 20: Equilibrium

STATIC EQUILIBRIUM

Fg

FNNormal force

Gravitational Force

F F F F F F F F FΣFTable

ΣFWood

Weight of the wood, W = mg

Page 21: Equilibrium

STATIC EQUILIBRIUM• A state of balance of an object at

rest.• A condition in which all forces

acting on the body are balanced, causing the body to remain at rest.

Page 22: Equilibrium

F1 F2

F3

F4

The Ring Four forces are acting on the ring.

If the ring is to remain at rest:

Page 23: Equilibrium

F1 F2

F3

F4

+x

+y

-y

-x

Draw the free-body diagram.

Page 24: Equilibrium

ΣF = ma =0ΣF = F1 + F2 + F3 + F4 = 0ΣF x = (-F1) + F2 = 0ΣF = F3 + (-F4) = 0

F1 F2

F3

F4

+x

+y

-y

-x

Page 25: Equilibrium

STATIC EQUILIBRIUM• The body must be in translational

equilibrium or the body does not accelerate along any line.

• If the acceleration is zero, then the resultant of the forces acting on the body is also zero.

Page 26: Equilibrium

The First Condition of Equilibrium:If the sum of all forces acting

concurrently on a body is equal to zero, then the body must be in static equilibrium. Mathematically:

ΣF = Fnet = 0

ΣFx = 0 and ΣFy = 0

Page 27: Equilibrium

T

Fg

Tension

Gravitational force

The chandelier has a mass of 3.0 kg. What is the tension in the cord?

Example no.1

W

Page 28: Equilibrium

Free-body Diagram

T

W= mg

Given: m= 3.8kgFind: T = ?

ΣF = 0 ΣFx = 0ΣFy = T – W = 0T – mg = 0T = mg = (3.0 kg)(9.8m/s2)T = 29.4 N

Page 29: Equilibrium

Find F1 and F2

Jaztene’s Internet Café

F1F2

W = 600 N

60°

Page 30: Equilibrium

Free-body diagramΣF = 0ΣFX = -F1x + F2x = 0

-F1 cos 60°+F2cos60°= 0

F1 = F2 ----- eq. 1

x

y F2F1

W = 600 N

60°60°60°

F1X F2X

F1y F2y ΣFy = F1y + F2x = 0

F1 sin60°+F2sin60°-W = 0

2F1 sin60°= 600N F1 = 600N

2 sin60°600N1.73

=

F1 = F2 = 347 N

Page 31: Equilibrium

60°

T1

T2

W = 2000N

3. Determine the tension in the cords supporting the 2000-N load?

ΣF = 0ΣFX = -T1x + T2 = 0

-T1 cos 30°+ T2= 0

T2 = T1 cos 30° ---- eq. 1ΣFy = T1y - W = 0

T1 sin30°-W = 0

T1 sin30°= 2000N

T1 = 4000 N

T2 = 2000 N