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2.001 - MECHANICS AND MATERIALS I
                                  Lecture #1
                                   9/6/2006
                            Prof. Carol Livermore

  A first course in mechanics for understanding and designing complicated
                                  systems.

PLAN FOR THE DAY:
  1. Syllabus
  2. Review vectors, forces, and moments
  3. Equilibrium
  4. Recitation sections
BASIC INGREDIENTS OF 2.001
  1. Forces, Moments, and Equilibrium → Statics (No acceleration)
  2. Displacements, Deformations, Compatibility (How displacements fit to-
     gether)
  3. Constitutive Laws: Relationships between forces and deformations




                      Use 2.001 to predict this problem.

HOW TO SOLVE A PROBLEM
RULES:


  1. SI inits only.
  2. Good sketches.
        • Labeled coordinate system.
• Labeled dimensions and forces.
  3. Show your thought process.
  4. Follow all conventions.
  5. Solve everything symbolically until the end.
  6. Check answer ⇒ Does it make sense?
        • Check trends.
        • Check units.
  7. Convert to SI, plug in to get answers.
VECTORS, FORCES, AND MOMENTS
Forces are vectors (Magnitude and Direction)




                                     i      j      ˆ
                               F = Fxˆ + Fy ˆ + Fz k
OR


                                   ∗         ∗      ˆ
                          F = Fx∗ iˆ + Fy∗ jˆ + Fz∗ k ∗
Where do forces come from?
   • Contact with another object
   • Gravity
   • Attractive of repulsive forces
Moments are vectors. (Moment is another word for torque.)
   • Forces at a distance from a point
   • Couple
Moments are vectors.
      M = My ˆ
             j.




 EX:




2D:


                                  FB = FBxˆ + FBy ˆ
                                          i       j
                                 rAB = rABxˆ + rABy ˆ
                                           i        j


                MA = rAB × FB     =
                                  =   (rABxˆ + rABy ˆ × (FBxˆ + FBy ˆ
                                           i        j)       i      j)
                                  =   (rAB FB − rAB FB )k  ˆ
                                          x   y         y   x


      OR


                     MA = |rAB | FB sin φ using Right Hand Rule
      3D:


                                       i        j        ˆ
                             rAB = rABxˆ + rABy ˆ + rABz k
                                      i       j       ˆ
                              FB = FBxˆ + FBy ˆ + FBz k


                                          ˆ
      MA = rAB ×FB = (rABx FBy −rABy FBx )k +(rABz FBx −rABx FBz )ˆ
                                                                  j+(rABy FBz −rABz FBy )ˆ
                                                                                         i




                                          3
EX: Wrench


                                  rAB = dˆ
                                         j
                                  FB = FBˆ
                                         i
                                    j     i        ˆ
                   MA = rAB × FB = dˆ × FBˆ = −dFB k




Equations of Static Equilibrium

           ΣFx = 0
    ΣF = 0 ΣFy = 0
           ΣFz = 0
            ΣM0 x = 0
    ΣM0 = 0 ΣM0 y = 0
            ΣM0 z = 0
4
                                            F =0
                                      i=1

                               F1 + F2 + F3 + F4 = 0
                          F1x + F2x + F3x + F4x = 0
                          F1y + F2y + F3y + F4y = 0
                              F1z + F2z + F3z + F4z = 0

                                           Mo = 0

               ⇒ r01 × F1 + r02 × F2 + r03 × F3 + r04 × F4 = 0
             i, j, ˆ
a. Expand in ˆ ˆ k .
b. Group.
c. Get 3 equations (x,y,z).

Try a new point? Try A.


                                   rA1 = rA0 + r01
                                            ...
                                           MA = 0

                rA1 × F1 + rA2 × F2 + rA3 × F3 + rA4 × F4 = 0


(rA0 + r01 ) × F1 + (rA0 + r02 ) × F2 + (rA0 + r03 ) × F3 + (rA0 + r04 ) × F4 = 0

rA0 × (F1 + F2 + F3 + F4 ) + (r0 1 × F1 + r0 2 × F2 + r0 3 × F3 + r0 4 × F4 ) = 0
                        rA0 × (F1 + F2 + F3 + F4 ) = 0

                                            F =0

               (r0 1 × F1 + r0 2 × F2 + r0 3 × F3 + r0 4 × F4 ) = 0
                                           M0 = 0
So taking moment about a new point gives no additional info.




                                            5

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Mechanics and Materials I Lecture 1 Overview

  • 1. 2.001 - MECHANICS AND MATERIALS I Lecture #1 9/6/2006 Prof. Carol Livermore A first course in mechanics for understanding and designing complicated systems. PLAN FOR THE DAY: 1. Syllabus 2. Review vectors, forces, and moments 3. Equilibrium 4. Recitation sections BASIC INGREDIENTS OF 2.001 1. Forces, Moments, and Equilibrium → Statics (No acceleration) 2. Displacements, Deformations, Compatibility (How displacements fit to- gether) 3. Constitutive Laws: Relationships between forces and deformations Use 2.001 to predict this problem. HOW TO SOLVE A PROBLEM RULES: 1. SI inits only. 2. Good sketches. • Labeled coordinate system.
  • 2. • Labeled dimensions and forces. 3. Show your thought process. 4. Follow all conventions. 5. Solve everything symbolically until the end. 6. Check answer ⇒ Does it make sense? • Check trends. • Check units. 7. Convert to SI, plug in to get answers. VECTORS, FORCES, AND MOMENTS Forces are vectors (Magnitude and Direction) i j ˆ F = Fxˆ + Fy ˆ + Fz k OR ∗ ∗ ˆ F = Fx∗ iˆ + Fy∗ jˆ + Fz∗ k ∗ Where do forces come from? • Contact with another object • Gravity • Attractive of repulsive forces Moments are vectors. (Moment is another word for torque.) • Forces at a distance from a point • Couple
  • 3. Moments are vectors. M = My ˆ j. EX: 2D: FB = FBxˆ + FBy ˆ i j rAB = rABxˆ + rABy ˆ i j MA = rAB × FB = = (rABxˆ + rABy ˆ × (FBxˆ + FBy ˆ i j) i j) = (rAB FB − rAB FB )k ˆ x y y x OR MA = |rAB | FB sin φ using Right Hand Rule 3D: i j ˆ rAB = rABxˆ + rABy ˆ + rABz k i j ˆ FB = FBxˆ + FBy ˆ + FBz k ˆ MA = rAB ×FB = (rABx FBy −rABy FBx )k +(rABz FBx −rABx FBz )ˆ j+(rABy FBz −rABz FBy )ˆ i 3
  • 4. EX: Wrench rAB = dˆ j FB = FBˆ i j i ˆ MA = rAB × FB = dˆ × FBˆ = −dFB k Equations of Static Equilibrium ΣFx = 0 ΣF = 0 ΣFy = 0 ΣFz = 0 ΣM0 x = 0 ΣM0 = 0 ΣM0 y = 0 ΣM0 z = 0
  • 5. 4 F =0 i=1 F1 + F2 + F3 + F4 = 0 F1x + F2x + F3x + F4x = 0 F1y + F2y + F3y + F4y = 0 F1z + F2z + F3z + F4z = 0 Mo = 0 ⇒ r01 × F1 + r02 × F2 + r03 × F3 + r04 × F4 = 0 i, j, ˆ a. Expand in ˆ ˆ k . b. Group. c. Get 3 equations (x,y,z). Try a new point? Try A. rA1 = rA0 + r01 ... MA = 0 rA1 × F1 + rA2 × F2 + rA3 × F3 + rA4 × F4 = 0 (rA0 + r01 ) × F1 + (rA0 + r02 ) × F2 + (rA0 + r03 ) × F3 + (rA0 + r04 ) × F4 = 0 rA0 × (F1 + F2 + F3 + F4 ) + (r0 1 × F1 + r0 2 × F2 + r0 3 × F3 + r0 4 × F4 ) = 0 rA0 × (F1 + F2 + F3 + F4 ) = 0 F =0 (r0 1 × F1 + r0 2 × F2 + r0 3 × F3 + r0 4 × F4 ) = 0 M0 = 0 So taking moment about a new point gives no additional info. 5