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Mechanics
science which describes and predicts the conditions of rest or motion of bodies under the action of forces
categories of mechanics
rigid bodies, deformable bodies, fluids
mechanics
foundation of most engineering sciences and is an indispensable prerequisite to their study
length
needed to locate the position of a point in space.
Distance
is described in terms of a standard unit of length
SI unit of length
meter (m)
english unit of length
foot (ft)
space
associated with the notion of the position of a point P given in terms of three coordinates measured from a reference point or origin
coordinates
x,y,z
time
definition of an event requires specification of the time and position at which it occurred
SI and english unit of time
seconds (s)
mass
used to characterize and compare bodies, e.g., response to earth's gravitational attraction and resistance to changes in translational motion
SI unit of mass
kilogram (kg)
english unit of mass
slug (sl)
force
represents the action of one body on another. It is characterized by its point of application, magnitude, and direction
SI unit of force
N (Newton)
english unit of force
pound (lb)
1 lb is equal to _N
4.4482N
1 slug is equal to _kg
14.5983kg
1ft is equal to _m
0.3048m
Weight
expressed in Newton since it is also a force
Weight formula
W = mg (mass x gravity) gravity = 9.81m/s² (32.2ft/s²) mass = mass of the body in kg
Force Formula
F = ma (mass x acceleration)
Classification of forces on rigid bodies
external force, internal force, applied force, reaction force, and distributed force
external force
force generated outside the body
internal force
force generated inside the body (to keep the body together)
applied force
is an external force on the body that tries to change the state of movement of the body
reaction force
an external force that inhibits change in the state of movement of a body when acted on by an applied force
distributed force
is a force density
free-body diagram (FBD)
1st step of solving
space diagram
A sketch showing the physical conditions of the problem.
Free Body Diagram (FBD)
A sketch showing only the forces on the selected particle
external forces
shown in a free-body diagram
Force systems according to the line of action
concurrent forces, parallel forces, non-concurrent forces
concurrent forces
forces whose lines of action pass through a common point
parallel forces
forces whose lines of actions are parallel
non-concurrent forces
forces whose lines of actions are neither parallel nor intersect in a common point
Newton's First Law
If the resultant force on a particle is zero, the particle will remain at rest or continue to move in a straight line.
Newton's Second Law
A particle will have an acceleration proportional to a nonzero resultant applied force
Newton's Third Law
The forces of action and reaction between two particles have the same magnitude and line of action with opposite sense
Principle of Transmissibility
the external effect of a force on a body is the same for all points of application along its line of action
scalar
A quantity that has only magnitude
vector
A quantity that has magnitude and direction
scalar
mass, speed, volume, temperature
vector
dorce, displacement, velocity, acceleration
Fixed or Bound Vectors
have well defined points of application that cannot be changed without affecting an analysis.
free vector
may be freely moved in space without changing their effect on an analysis
sliding vectors
may be applied anywhere along their line of action without affecting an analysis.
equal vectors
have the same magnitude and direction
negative vectors
same magnitude and the opposite direction.
sign convention of components
QUADRANT = X COMPONENT | Y COMPONENT 1st = + | + 2nd = - | + 3rd = - | - 4th = + | -
components of the resultant
equal to the sum of the corresponding scalar components of the given forces
direction of the resultant formula
θ= tan-1 (Ry / Rx)
magnitude of the resultant formula
R = √(R²x + R²y)
resultant
is equivalent to the diagonal of a parallelogram which contains the two forces in adjacent legs
Law of Cosines Formula
R² = P² + Q² - 2PQcosB
Law of Sines Formula
sinA/a = sinB/b = sinC/c
X and Y component Formula
Fx= FCosθ Fy= Fsinθ
Moment of a Force
e measure of the tendency of a force F to make the rigid body rotate about a fixed axis perpendicular to the plane of the force F
Moment arm
larger the force or the longer the moment arm (d) , the greater the moment or turning effect
Magnitude formula
M = Fd M= moment F = force d= moment arm perpendicular to line of action of force F
Varignon's Theorem
moment about a given point O of the resultant of several concurrent forces is equal to the sum of the moments of the various forces about the same point O.
couples
Sometimes the resultant of a force system will be zero in magnitude and yet have a resultant moment sum
couples
s made up of two equal, parallel, oppositely directed forces
statics
deals primarily with the calculation of external forces which act on rigid bodies in equilibrium
rigid body
combination of a large number of particles occupying fixed positions with respect to each other
force is developed if..
If a support prevents the translation of a body in a given direction
a couple moment is exerted on a body if..
If rotation is prevented
cables
no. of unknown= 1
contacting surface
no. of unknown= 1
roller support
no. of unknown= 1
pin support
no. of unknown= 2
pin connections allow..
it allows rotation
considered as FORCES not moments
reactions at pins
slider / constrained pin
no. of unknown= 1
fixed support
no. of unknown= 3
∑Fx and ∑Fy
represent sums of x and y components of all the forces
∑Mo
represents the sum of the couple moments and moments of the force components
truss
a structure composed of slender members joined together at their end points.
planar trusses
lie in a single plane and are often used to support roofs and bridges
truss members
connected at their extremities only; thus no member is continuous through a joint.
Plane Truss assumptions
the weight of the members are negligible
all joints are smooth pins
the applied forces act at the joints
tension
member reaction due to pulling forces at both ends and is denoted by (T); lengthening force
compression
member reaction due to pushing forces at both ends denoted by (C); shortening force
members of a truss
are slender and not cappable of supporting large lateral loads. Loads must be applied at the joints
method of joints
To calculate the forces in the members of a truss, the equilibrium equations are applied to individual joints (or pins) of the truss
method of sections
Consist of cutting a truss into two sections at a point where the bar force is required.
Rigid truss
will not collapse under the application of a load
simple truss
constructed by successively adding two members and one connection to the basic triangular truss
m = 2n-3
Trusses are statically determinant, rigid, and completely constrained
m > 2n-3
Truss contains a redundant member and is statically indeterminate
Joints Under Special Loading Conditions
Forces in opposite members intersecting in two straight lines at a joint are equal
forces in two opposite members are equal when a load is aligned with a third member. The third member force is equal to the load (including zero load)
The forces in two members connected at a joint are equal if the members are aligned and zero otherwise
Compound trusses
are statically determinant, rigid, and completely constrained
2 members are zero force members if..
If a joint has only two non-collinear members and there is no external load or support reaction at that joint
third noncollinear member is a zero force member if..
If three members form a truss joint for which two of the members are collinear and there is no external load or reaction at that joint, then the third noncollinear member is a zero force member
strength of materials
aka mechanics of materials
strength of materials
the study of the internal effect of external forces applied to structural members
stress
internal loads cause ______ in a body/material
deform
stresses cause a body to ____
stress
defined as the strength of a material per unit area