Statics Using 2 index cards Create a structure

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Statics Using 2 index cards: Create a structure or system of structures that will

Statics Using 2 index cards: Create a structure or system of structures that will elevate two textbooks at least 1. 5 cm off your desk

Statics Kentucky & Indiana Bridge Chicago What is Statics? Branch of Mechanics that deals

Statics Kentucky & Indiana Bridge Chicago What is Statics? Branch of Mechanics that deals with objects/materials that are stationary or in uniform motion. Forces are balanced. Examples: 1. A book lying on a table (statics) 2. Water being held behind a dam (hydrostatics)

Dynamics is the branch of Mechanics that deals with objects/materials that are accelerating due

Dynamics is the branch of Mechanics that deals with objects/materials that are accelerating due to an imbalance of forces. Examples: 1. A rollercoaster executing a loop (dynamics) 2. Flow of water from a hose (hydrodynamics)

1. 2. 3. 4. 5. Total degrees in a triangle: 180 Three angles of

1. 2. 3. 4. 5. Total degrees in a triangle: 180 Three angles of the triangle below: A, B, and Three sides of the triangle below: x, y, and r Pythagorean Theorem: B x 2 + y 2 = r 2 E OT P HY A E S U N r x y C C

Trigonometric functions are ratios of the lengths of the segments that make up angles.

Trigonometric functions are ratios of the lengths of the segments that make up angles. sin Q = opp. = hyp. r Q x y y r cos Q = adj. = x hyp. r tan Q = opp. = adj. y x

For <A below, calculate Sine, Cosine, and Tangent: B 2 A 1 C opposite

For <A below, calculate Sine, Cosine, and Tangent: B 2 A 1 C opposite sin A = hypotenuse 1 sin A = 2 opposite tan A = adjacent cos A = hypotenuse tan A = 1 √ 3 cos A = √ 3 2

B c A Law of Cosines: c 2 = a 2 + b 2

B c A Law of Cosines: c 2 = a 2 + b 2 – 2 ab cos C a b C Law of Sines: sin A sin B = a b = sin C c

1. Scalar – a variable whose value is expressed only as a magnitude or

1. Scalar – a variable whose value is expressed only as a magnitude or quantity 1. Height, pressure, speed, density, etc. 2. Vector – a variable whose value is expressed both as a magnitude and direction Displacement, force, velocity, momentum, etc. 3. 4. 3. Tensor – a variable whose values are collections of vectors, such as stress on a material, the curvature of spacetime (General Theory of Relativity), gyroscopic motion, etc.

Properties of Vectors 1. Magnitude 2. Length implies magnitude of vector 2. Direction Arrow

Properties of Vectors 1. Magnitude 2. Length implies magnitude of vector 2. Direction Arrow implies direction of vector 3. Act along the line of their direction 4. No fixed origin 5. Can be located anywhere in space

Bold type and an underline F also identify vectors Vectors - Description Hat signifies

Bold type and an underline F also identify vectors Vectors - Description Hat signifies vector quantity Magnitude, Direction F = 40 lbs 45 o F = 40 lbs @ 45 o magnitude direction s lb 40 45 o

Vectors – Scalar Multiplication 1. 2. We can multiply any vector by a whole

Vectors – Scalar Multiplication 1. 2. We can multiply any vector by a whole number. Original direction is maintained, new magnitude. 2 ½

Vectors – Addition 1. 2. We can add two or more vectors together. 2

Vectors – Addition 1. 2. We can add two or more vectors together. 2 methods: 1. Graphical Addition/subtraction – redraw vectors head-totail, then draw the resultant vector. (head-to-tail order does not matter)

Vectors – Rectangular Components 1. 2. 3. 4. It is often useful to break

Vectors – Rectangular Components 1. 2. 3. 4. It is often useful to break a vector into horizontal and vertical components (rectangular components). Consider the Force vector below. Plot this vector on x-y axis. Project the vector onto x and y axes. y Fy F Fx x

Vectors – Rectangular Components This means: vector F = vector Fx + vector Fy

Vectors – Rectangular Components This means: vector F = vector Fx + vector Fy Remember the addition of vectors: y Fy F Fx x

Unit vector Vectors – Rectangular Components Vector Fx = Magnitude Fx times vector i

Unit vector Vectors – Rectangular Components Vector Fx = Magnitude Fx times vector i F = Fx i + Fy j F x = Fx i i denotes vector in x direction y Vector Fy = Magnitude Fy times vector j Fy F Fx F y = Fy j x j denotes vector in y direction

Vectors – Rectangular Components Each grid space represents 1 lb force. What is Fx?

Vectors – Rectangular Components Each grid space represents 1 lb force. What is Fx? y Fy Fx = (4 lbs)i What is Fy? F Fx Fy = (3 lbs)j x What is F? F = (4 lbs)i + (3 lbs)j

Vectors – Rectangular Components If vector V=ai+bj+ck then the magnitude of vector V |V|

Vectors – Rectangular Components If vector V=ai+bj+ck then the magnitude of vector V |V| =

Vectors – Rectangular Components What is the relationship between Q, sin Q, and cos

Vectors – Rectangular Components What is the relationship between Q, sin Q, and cos Q? cos Q = Fx / F Fx = F cos Qi F Q Fy sin Q = Fy / F Fy = F sin Qj Fx

Vectors – Rectangular Components When are Fx and Fy Positive/Negative? Fy + y F

Vectors – Rectangular Components When are Fx and Fy Positive/Negative? Fy + y F Fx - Fy + F Fy - Fx + F x F Fy - Fx +

Vectors – Rectangular Components Complete the following chart in your notebook: II I III

Vectors – Rectangular Components Complete the following chart in your notebook: II I III IV

Vectors 1. 2. Vectors can be completely represented in two ways: 1. Graphically 2.

Vectors 1. 2. Vectors can be completely represented in two ways: 1. Graphically 2. Sum of vectors in any three independent directions Vectors can also be added/subtracted in either of those ways: 1. 2. F 1 = ai + bj + ck; F 2 = si + tj + uk 3. F 1 + F 2 = (a + s)i + (b + t)j + (c + u)k

Vectors A third way to add, subtract, and otherwise decompose vectors: R 45 o

Vectors A third way to add, subtract, and otherwise decompose vectors: R 45 o F 1 30 o 105 o F 2 Use the law of sines or the law of cosines to find R.

Vectors Brief note about subtraction 1. If F = ai + bj + ck,

Vectors Brief note about subtraction 1. If F = ai + bj + ck, then 2. Also, if 3. F = 4. Then, 5. – F = – ai – bj – ck

Resultant Forces Resultant forces are the overall combination of all forces acting on a

Resultant Forces Resultant forces are the overall combination of all forces acting on a body. 1) find sum of forces in x-direction 2) find sum of forces in y-direction 3) find sum of forces in z-direction 3) Write as single vector in rectangular components R = SFxi + SFyj + SFzk

Resultant Forces - Example A satellite flies without friction in space. Earth’s gravity pulls

Resultant Forces - Example A satellite flies without friction in space. Earth’s gravity pulls downward on the satellite with a force of 200 N. Stray space junk hits the satellite with a force of 1000 N at 60 o to the horizontal. What is the resultant force acting on the satellite? 1. Sketch and label free-body diagram (all external and reactive forces acting on the body) 2. Decompose all vectors into rectangular components (x, y, z) 3. Add vectors

Now on to the point… Statics Newton’s 3 Laws of Motion: 1. A body

Now on to the point… Statics Newton’s 3 Laws of Motion: 1. A body at rest will stay at rest, a body in motion will stay in motion, unless acted upon by an external force This is the condition for static equilibrium In other words…the net force acting upon a body is Zero

Newton’s 3 Laws of Motion: 2. Force is proportional to mass times acceleration: 3.

Newton’s 3 Laws of Motion: 2. Force is proportional to mass times acceleration: 3. F = ma If in static equilibrium, the net force acting upon a body is Zero What does this tell us about the acceleration of the body? It is Zero

Newton’s 3 Laws of Motion: 3. Action/Reaction

Newton’s 3 Laws of Motion: 3. Action/Reaction

Statics Two conditions for static equilibrium: 1. Since Force is a vector, this implies

Statics Two conditions for static equilibrium: 1. Since Force is a vector, this implies Individually.

Two conditions for static equilibrium: 1.

Two conditions for static equilibrium: 1.

Two conditions for static equilibrium: Why isn’t sufficient?

Two conditions for static equilibrium: Why isn’t sufficient?

Two conditions for static equilibrium: 2. About any point on an object, Moment M

Two conditions for static equilibrium: 2. About any point on an object, Moment M (or torque t) is a scalar quantity that describes the amount of “twist” at a point. M = (magnitude of force perpendicular to moment arm) * (length of moment arm) = (magnitude of force) * (perpendicular distance from point to force)

Two conditions for static equilibrium: MP = F * x M P = Fy

Two conditions for static equilibrium: MP = F * x M P = Fy * x F F P P x x M = (magnitude of force perpendicular to moment arm) * (length of moment arm) = (magnitude of force) * (perpendicular distance from point to force)

Moment Examples: 1. Tension test apparatus – unknown and reaction forces? 2. If a

Moment Examples: 1. Tension test apparatus – unknown and reaction forces? 2. If a beam supported at its endpoints is given a load F at its midpoint, what are the supporting forces at the endpoints? Ra 3. Rb Find sum of moments about a or b. Watch your signs – identify positive

Moment Examples: 3. An “L” lever is pinned at the center P and holds

Moment Examples: 3. An “L” lever is pinned at the center P and holds load F at the end of its shorter leg. What force is required at Q to hold the load? What is the force on the pin at P holding the lever? 4. 5. What is your method for solving this problem? Remember,

Trusses: A practical and economic solution to many structural engineering challenges Simple truss –

Trusses: A practical and economic solution to many structural engineering challenges Simple truss – consists of tension and compression members held together by hinge or pin joints Rigid truss – will not collapse

Trusses Joints: Pin or Hinge (fixed)

Trusses Joints: Pin or Hinge (fixed)

Trusses Supports: Pin or Hinge (fixed) – 2 unknowns Reaction in x-direction Reaction in

Trusses Supports: Pin or Hinge (fixed) – 2 unknowns Reaction in x-direction Reaction in y-direction Rax Ray

Trusses Supports: Roller - 1 unknown Reaction in y-direction only Ray

Trusses Supports: Roller - 1 unknown Reaction in y-direction only Ray

Assumptions to analyze simple truss: 1. 2. 3. 4. Joints are assumed to be

Assumptions to analyze simple truss: 1. 2. 3. 4. Joints are assumed to be frictionless, so forces can only be transmitted in the direction of the members. Members are assumed to be massless. Loads can be applied only at joints (or nodes). Members are assumed to be perfectly rigid. 6. 7. 5. 2 conditions for static equilibrium: Sum of forces at each joint (or node) = 0 Moment about any joint (or node) = 0 8. Start with Entire Truss Equilibrium Equations

Truss Analysis Example Problems: 1. A force F is applied to the following equilateral

Truss Analysis Example Problems: 1. A force F is applied to the following equilateral truss. Determine the force in each member of the truss shown and state which members are in compression and which are in tension.

Truss Analysis Example Problems: 2. Using the method of joints, determine the force in

Truss Analysis Example Problems: 2. Using the method of joints, determine the force in each member of the truss shown. Assume equilateral triangles.

Static determinacy and stability: Statically Determinant: All unknown reactions and forces in members can

Static determinacy and stability: Statically Determinant: All unknown reactions and forces in members can be determined by the methods of statics – all equilibrium equations can be satisfied. m = 2 j – r (Simple Truss) Static Stability: The truss is rigid – it will not collapse.

Conditions of static determinacy and stability of trusses:

Conditions of static determinacy and stability of trusses:

Materials Lab Connections: • Tensile Strength = Force / Area • Compression is Proportional

Materials Lab Connections: • Tensile Strength = Force / Area • Compression is Proportional to 1 / R 4 Problem Sheet solutions due Monday