Static Equilibrium

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MEE1004 - Mechanics of Materials 1. Week 14

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40 Terms

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Truss structure forces

Members subjected to tensile / compressive forces.

Material subjected to axial stress.

<p>Members subjected to tensile / compressive forces.</p><p>Material subjected to axial stress.</p>
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Beam structure forces

Members subjected to shear forces and bending moments.

Material subjected to bending stress.

<p>Members subjected to shear forces and bending moments. </p><p>Material subjected to bending stress. </p>
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Shaft structure forces

Members are subjected to torques (moments about the longitudinal axis).

Materials subjected to torsional shear stress.

<p>Members are subjected to torques (moments about the longitudinal axis).</p><p>Materials subjected to torsional shear stress. </p>
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Structural Idealisation

The process of making simplifying assumptions in order to facilitate a basic analysis.

<p>The process of making simplifying assumptions in order to facilitate a basic analysis. </p>
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Standard symbols are used to represent different types of supports, based on:

The types displacement they allow, and

The corresponding reaction forces that develop.

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Other word for moment

Torque.

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Newton’s Second Law

Linear acceleration (a) of an object of mass m is proportional to net force (F) acting upon it:

F = ma

<p>Linear acceleration (a) of an object of mass m is proportional to net force (F) acting upon it:</p><p>F = ma</p>
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Angular acceleration equation

Angular acceleration (α) of an object with mass moment of inertia I is proportional to the net moment (M) acting upon it:

M = Iα

<p>Angular acceleration (<span>α</span>) of an object with mass moment of inertia I is proportional to the net moment (M) acting upon it:</p><p>M = I<span>α</span></p>
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Moment

The turning effect of a force.

When forces tend to cause a rotation, they are exerting a moment. / Moments are the cause of a change in rotation.

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Moments equation

Moment of a force = Force x perpendicular distance

M = Fd

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Moments unit

Newton metre (Nm)

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Distance is the moment equation is termed

The moment arm.

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Moments sign convention

In accordance with the right hand rule, a moment that would tend to cause a counter-clockwise rotation is considered positive.

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Right Hand Rule

Hold hand over point A.

Curl finger of your right hand in the direction of rotation.

Thumbs up = +M (pos.)

Thumbs down = -M (neg.)

<p>Hold hand over point A.</p><p>Curl finger of your right hand in the direction of rotation. </p><p>Thumbs up = +M (pos.)</p><p>Thumbs down = -M (neg.)</p>
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Force couple

A system of two equal and opposite forces with different lines of action.

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Concentrated moment

The equivalent force system for a force couple. It exerts the same about any point.

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Degrees of Freedom

A rigid body has three possible degrees of freedom with respect to motion in two dimensions (three independent ways that the motion of a rigid body can change by accelerating).

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Three degrees of freedom

  1. Horizontal acceleration (x-direction),

  2. Vertical acceleration (y-direction),

  3. Angular acceleration (rotation in the x-y plane (z plane))

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Rigid body

An object that cannot change shape(i.e. a solid object that we assume does not deform).

<p>An object that cannot change shape(i.e. a solid object that we assume does not deform). </p>
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Conditions for Static Equilibrium (2-D)

There are three conditions for static equilibrium of a rigid body in two dimensions (in an x-y plane):

  1. ΣFx = 0 ( the sum of all forces in the x-direction is zero). Therefore there is no acceleration in the x-direction.

  2. ΣFy = 0 (the sum of all forces in the y-direction is zero). Therefore, there is no acceleration in the y-direction.

  3. Σ(Mz)any point = 0 (the sum of all moments in the z-direction about any point is zero). Therefore, there is no rotation about the z-axis (in the x-y plane).

These conditions can be used to calculate up to three unknown forces / moments acting on an object that is in equilibrium (because we can write these three equations).

<p>There are three conditions for static equilibrium of a rigid body in two dimensions (in an x-y plane):</p><ol><li><p><span>ΣF<sub>x</sub> = 0 ( the sum of all forces in the x-direction is zero). <em>Therefore there is no acceleration in the x-direction.</em></span></p></li><li><p><span>ΣF<sub>y</sub> = 0 (the sum of all forces in the y-direction is zero). <em>Therefore, there is no acceleration in the y-direction.</em> </span></p></li><li><p><span>Σ(M<sub>z</sub>)<sub>any point</sub> = 0 (the sum of all moments in the z-direction about any point is zero). <em>Therefore, there is no rotation about the z-axis (in the x-y plane)</em>.</span></p></li></ol><p></p><p><strong>These conditions can be used to calculate up to <u>three </u>unknown forces / moments acting on an object that is in equilibrium</strong> (because we can write these <u>three </u>equations). </p><p></p>
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Free-Body Diagram

A sketch of an isolated objected with its surrounding objects replaced by the forces and / or moments that they exert on the isolated object.

<p>A sketch of an isolated objected with its surrounding objects replaced by the forces and / or moments that they exert on the isolated object. </p>
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In a free-body diagram, when deciding what forces / moments being removed might exert

Consider which degrees of freedom are constrained by the portion removed.

  • Translation resisted in a given direction - there is a reaction force in that direction.

  • Rotation resisted about a given axis - there is a reaction moment about that axis.

Equal and opposite forces / moments are always exerted back on the elements that are removed from a FBD.

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Essential components of FBD

  1. Appropriate identification of the isolated object.

  2. A coordinate system.

  3. Any applied loads.

  4. Reactions from any points of contact with bodies that were removed.

  5. Indicate the assumed direction of all forces / moments with an arrow.

  6. Any necessary information about geometry (i.e. angles).

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Roller connection / supports in a FBD

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Pinned connections / supports in a FBD

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Fixed (or built-in) connections / supports in a FBD

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Roller supports

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Pinned connections

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Fixed supports

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Types of equilibrium

Static and dynamic.

In both cases, there must be a balance of forces acting on the object.

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Static equilibrium

Occurs when an object is at rest.

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Dynamic equailibrium

Occurs when an object is moving with a constant velocity.

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Conditions of equilibrium

  1. The net force acting on the object must be zero,

  2. The net moment acting on the object must be zero.

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Representing forces in a FBD

Forces are represented using arrows.

The direction of the arrows represents the direction of the force.

The length of the arrows depicts the magnitude of the force.

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Common forces represented in a FBD

Weight, normal force, tension, friction and applied force.

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Weight

The force of gravity acting on the object, typically represented by an arrow pointing downward. N

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Normal force

The force between two objects when they come in contact with each other. This force acts in the opposite direction to the weight of the object.

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Tension

Represented by an arrow pointing away from the object in the direction of the force.

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Friction

The force that resists sliding between surfaces.

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Applied force

The force applied to the object by an external agent, such as a push or a pull. Represented by an arrow pointing in the direction of the force.