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139 Terms

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Mechanics

science which describes and predicts the conditions of rest or motion of bodies under the action of forces

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categories of mechanics

rigid bodies, deformable bodies, fluids

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mechanics

foundation of most engineering sciences and is an indispensable prerequisite to their study

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length

needed to locate the position of a point in space.

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Distance

is described in terms of a standard unit of length

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SI unit of length

meter (m)

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english unit of length

foot (ft)

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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

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coordinates

x,y,z

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time

definition of an event requires specification of the time and position at which it occurred

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SI and english unit of time

seconds (s)

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mass

used to characterize and compare bodies, e.g., response to earth's gravitational attraction and resistance to changes in translational motion

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SI unit of mass

kilogram (kg)

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english unit of mass

slug (sl)

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force

represents the action of one body on another. It is characterized by its point of application, magnitude, and direction

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SI unit of force

N (Newton)

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english unit of force

pound (lb)

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1 lb is equal to _N

4.4482N

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1 slug is equal to _kg

14.5983kg

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1ft is equal to _m

0.3048m

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Weight

expressed in Newton since it is also a force

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Weight formula

W = mg (mass x gravity) gravity = 9.81m/s² (32.2ft/s²) mass = mass of the body in kg

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Force Formula

F = ma (mass x acceleration)

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Classification of forces on rigid bodies

external force, internal force, applied force, reaction force, and distributed force

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external force

force generated outside the body

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internal force

force generated inside the body (to keep the body together)

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applied force

is an external force on the body that tries to change the state of movement of the body

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reaction force

an external force that inhibits change in the state of movement of a body when acted on by an applied force

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distributed force

is a force density

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free-body diagram (FBD)

1st step of solving

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space diagram

A sketch showing the physical conditions of the problem.

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Free Body Diagram (FBD)

A sketch showing only the forces on the selected particle

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external forces

shown in a free-body diagram

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Force systems according to the line of action

concurrent forces, parallel forces, non-concurrent forces

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concurrent forces

forces whose lines of action pass through a common point

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parallel forces

forces whose lines of actions are parallel

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non-concurrent forces

forces whose lines of actions are neither parallel nor intersect in a common point

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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.

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Newton's Second Law

A particle will have an acceleration proportional to a nonzero resultant applied force

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Newton's Third Law

The forces of action and reaction between two particles have the same magnitude and line of action with opposite sense

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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

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scalar

A quantity that has only magnitude

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vector

A quantity that has magnitude and direction

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scalar

mass, speed, volume, temperature

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vector

dorce, displacement, velocity, acceleration

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Fixed or Bound Vectors

have well defined points of application that cannot be changed without affecting an analysis.

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free vector

may be freely moved in space without changing their effect on an analysis

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sliding vectors

may be applied anywhere along their line of action without affecting an analysis.

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equal vectors

have the same magnitude and direction

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negative vectors

same magnitude and the opposite direction.

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sign convention of components

QUADRANT = X COMPONENT | Y COMPONENT 1st = + | + 2nd = - | + 3rd = - | - 4th = + | -

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components of the resultant

equal to the sum of the corresponding scalar components of the given forces

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direction of the resultant formula

θ= tan-1 (Ry / Rx)

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magnitude of the resultant formula

R = √(R²x + R²y)

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resultant

is equivalent to the diagonal of a parallelogram which contains the two forces in adjacent legs

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Law of Cosines Formula

R² = P² + Q² - 2PQcosB

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Law of Sines Formula

sinA/a = sinB/b = sinC/c

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X and Y component Formula

Fx= FCosθ Fy= Fsinθ

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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

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Moment arm

larger the force or the longer the moment arm (d) , the greater the moment or turning effect

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Magnitude formula

M = Fd M= moment F = force d= moment arm perpendicular to line of action of force F

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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.

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couples

Sometimes the resultant of a force system will be zero in magnitude and yet have a resultant moment sum

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couples

s made up of two equal, parallel, oppositely directed forces

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statics

deals primarily with the calculation of external forces which act on rigid bodies in equilibrium

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rigid body

combination of a large number of particles occupying fixed positions with respect to each other

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force is developed if..

If a support prevents the translation of a body in a given direction

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a couple moment is exerted on a body if..

If rotation is prevented

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cables

no. of unknown= 1

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contacting surface

no. of unknown= 1

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roller support

no. of unknown= 1

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pin support

no. of unknown= 2

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pin connections allow..

it allows rotation

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considered as FORCES not moments

reactions at pins

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slider / constrained pin

no. of unknown= 1

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fixed support

no. of unknown= 3

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∑Fx and ∑Fy

represent sums of x and y components of all the forces

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∑Mo

represents the sum of the couple moments and moments of the force components

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truss

a structure composed of slender members joined together at their end points.

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planar trusses

lie in a single plane and are often used to support roofs and bridges

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truss members

connected at their extremities only; thus no member is continuous through a joint.

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Plane Truss assumptions

  1. the weight of the members are negligible

  2. all joints are smooth pins

  3. the applied forces act at the joints

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tension

member reaction due to pulling forces at both ends and is denoted by (T); lengthening force

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compression

member reaction due to pushing forces at both ends denoted by (C); shortening force

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members of a truss

are slender and not cappable of supporting large lateral loads. Loads must be applied at the joints

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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

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method of sections

Consist of cutting a truss into two sections at a point where the bar force is required.

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Rigid truss

will not collapse under the application of a load

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simple truss

constructed by successively adding two members and one connection to the basic triangular truss

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m = 2n-3

Trusses are statically determinant, rigid, and completely constrained

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m > 2n-3

Truss contains a redundant member and is statically indeterminate

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Joints Under Special Loading Conditions

  1. Forces in opposite members intersecting in two straight lines at a joint are equal

  2. 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)

  3. The forces in two members connected at a joint are equal if the members are aligned and zero otherwise

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Compound trusses

are statically determinant, rigid, and completely constrained

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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

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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

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strength of materials

aka mechanics of materials

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strength of materials

the study of the internal effect of external forces applied to structural members

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stress

internal loads cause ______ in a body/material

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deform

stresses cause a body to ____

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stress

defined as the strength of a material per unit area