Load/Force
•Two kind of external load/forces which
may act on a body i.e
•Surface force: Force distributed over the
surface of the body e.g hydrostatic
pressure.
•Body force: Force distributed over the
volume of the body. e.g. Gravitational
force, Magnetic force, inertia force.
Force
•The action on a body which tends to make
it move, such as push or pull is called
force.
•Magnitude, direction, point of application
fully describe a force. B
•Graphically: A
•A, point of application, and arrow
indicates the direction and AB denotes
magnitude
Force
Force F can be written as the vector sum of
three independent component.
Fx, Fy, Fz,
I,j,k are the unit vector associated with the
coordinates x, y, z
F= Fxi+ Fyj+ Fzk
F
Stress
•Stress is a measure of force per unit area within
a body. (Intensity of such a force)
•It is a body's internal distribution of force per
area that reacts to external applied loads.
• Stress is often broken down into its shear and
normal components as these have unique
physical significance.
•In short, stress is to force as strain is to
elongation.
Force
Force F can be written as the vector sum of
three independent component.
Fx, Fy, Fz,
I,j,k are the unit vector associated with the
coordinates x, y, z
F= Fxi+ Fyj+ Fzk
F
Intensity of a force (stress)
If a solid sustaining forces were to be cut ,a
force F would have to act on the exposed
face to maintain equilibrium..
For a cut perpendicular to the x-axis.
The resultant contribution of these internal
forces on the area element
A to be F
Component of F along x,y, z axis are
the intensities of these force component are
termed as stress
Component.
Normal and Shear stress
•
Normal Stress: Intensity of force
perpendicular to a cut.
•
Normal stress that pull away from the cut
are tensile stress
•
Normal stress that push against the face
are compresive stress
•
Shear stress Parellel to the plane of the
element
•
The first subscript denotes the axis
prependicular to plane on which the stress
acts
•
The second designates the direction of the
stress
Torsion
where shear stresses across the
diagonal are identical
(i.e. sxy = syx, syz = szy, and szx =
sxz) as a result of static equilibrium
(no net moment).
This grouping of the nine stress
components is known as the stress
tensor (or stress matrix).