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Statics

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Title: Statics


1
Chapter 8
  • Statics

2
Equilibrium
  • An object either at rest or moving with a
    constant velocity is said to be in equilibrium
  • The net force acting on the object is zero (since
    the acceleration is zero)

3
1st Condition for Equilibrium
  • Net force vanishes

4
Method
  • Isolate object of interest
  • Draw picture, label all forces
  • Choose appropriate coordinate system
  • Resolve into components
  • Write equations for equilibrium
  • Solve equations for unknowns

5
Example
  • Mass m on table top
  • 200 lb man hanging from rope

6
Example (ex 2)
  • Find tensions in the ropes.

7
Example 8.4
  • Two objects are in equilibrium. Find the weight
    of the one on the left and tensions.

8
Force vs. Torque
  • Forces cause accelerations
  • Torques cause angular accelerations
  • rotation
  • Force and torque are related

9
Torque
  • The door is free to rotate about an axis through
    O
  • There are three factors that determine the
    effectiveness of the force in opening the door
  • The magnitude of the force
  • The position of the application of the force
  • The angle at which the force is applied

10
Torque, cont
  • Torque, t, is the tendency of a force to rotate
    an object about some axis
  • t is the torque
  • F is the force
  • symbol is the Greek tau
  • l is the lever arm
  • SI unit is N.m
  • Lever Arm Perpendicular distance from the pivot
    point to the line of force

11
Direction of Torque
  • Torque is a vector quantity
  • We will treat only 2-d torque so no need for
    vector notion.
  • If the turning tendency of the force is
    counterclockwise, the torque will be positive ()
  • If the turning tendency is clockwise, the torque
    will be negative (-)

12
Multiple Torques
  • When two or more torques are acting on an object,
    the torques are added
  • with the signs
  • If the net torque is zero, the objects rate of
    rotation doesnt change

13
General Definition of Torque
  • The applied force is not always perpendicular to
    the position vector
  • The component of the force perpendicular to the
    object will cause it to rotate
  • F is the force
  • L is distance between pivot and point of action
  • q is the angle

14
Example (8.20)
  • Torque problem

15
Center of Gravity
  • The weight of an object can cause object to pivot
  • C.G. used as pivot will have no torque due to
    gravity
  • In finding the torque produced by the force of
    gravity, all of the weight of the object can be
    considered to be concentrated at a single point,
    C.G.

16
Center of Gravity of a Uniform Object
  • The center of gravity of a homogenous, symmetric
    body must lie on the axis of symmetry.
  • Often, the center of gravity of such an object is
    the geometric center of the object.

17
Experimentally Determining the Center of Gravity
  • The wrench is hung freely from two different
    pivots
  • The intersection of the lines indicates the
    center of gravity
  • A rigid object can be balanced by a single force
    equal in magnitude to its weight as long as the
    force is acting upward through the objects
    center of gravity

18
2nd Condition for Equilibrium
  • No rotation
  • Net torque vanishes

19
Example
  • 1000 N sign painter on an uniform 250N board
    suspended by two ropes. The board is 5m long. If
    the rope can hold only 900 N, is it safe for him
    to stand 1m from a rope?

20
Example
  • 600 N worker standing 1.5 m from the wall on 5m
    long and 300N beam as show.
  • Find tension in the cable and the force on the
    beam by the wall.

21
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