2-9 Bearing and Shear

Overview of Chapter One Concepts

Stress Types

  • Normal Stress:

    • Results when loads are applied perpendicular to the material surface.
    • If there is breaking, it is often under normal stress conditions.
  • Shear Stress:

    • Results when loads are applied parallel to the material surface.
    • Understanding shear stress is crucial when discussing structural integrity.
    Types of Shear Stress
    • Single Shear:
    • A condition where the shear force is applied at one section of the material.
    • Double Shear:
    • A condition where the shear force is divided among two sections of the material.

Example Problems

  • Example 1 (Chapter 1.4): Determining Minimum Acceptable Diameter for a Pin

    • Setup: Two chain members are connected by a shackle and a pin.
    • Given:
    • Axial force in the chain, F=28extkNF = 28 ext{ kN}.
    • Allowable shear stress in the pin, auextmax=90extMPaau_{ ext{max}} = 90 ext{ MPa}.
    • Objective: Determine the minimum effective diameter for the pin.
    • Calculation Steps:
    1. Identify shear forces acting on the pin:
      • Apply load (P=28extkNP = 28 ext{ kN}) enters the shear area.
    2. Each shear carries half the applied load in double shear:
      • P2=14extkN\frac{P}{2} = 14 ext{ kN} for each shear surface.
    3. Calculate shear area required:
      • V = rac{P}{A}
        ightarrow A = rac{P}{ au_{ ext{max}}}.
    4. Use the cross-sectional area equation for circular sections:
      • A=extDiameter2imesextπ4A = \frac{ ext{Diameter}^2 imes ext{π}}{4} to back-calculate the diameter.
    • Important Note: Ensure any assumptions made, such as defining the mode of loading (single vs double shear).
  • Free Body Diagram:

    • Useful for visualizing the forces acting on the pin and determining reaction forces.

Addressing Forces in Example

  • For evaluating reaction forces along points, necessary to account for various forces affected by the system.
  • Define unknowns and relationships between them using equilibrium equations:
    • Equilibrium in X direction:
    • C<em>x+F</em>ab=0C<em>x + F</em>{ab} = 0 (sum of horizontal forces)
    • Equilibrium in Y direction:
    • CyT15=0C_y - T - 15 = 0 (sum of vertical forces)
    • Moment about point C:
    • Calculate clockwise moments for determining forces applied.
  • After identifying forces, use derived equations to solve for unknowns systematically.

Punching Example

  • Punching Setup:
    • Downward punching force required to remove material from a steel plate.
    • Given data:
    • Punching force: 32exttons32 ext{ tons}.
    • Punch diameter: 0.75extin0.75 ext{ in}.
    • Thickness of plate: 0.25extin0.25 ext{ in}.
    • Acknowledge the relationship between force applied, area of the punch, and the resultant shear stresses:
    • extShearStress=FAext{Shear Stress} = \frac{F}{A},
    • with area denoted as A=extPunchDiameter2imesextπ4A = \frac{ ext{Punch Diameter}^2 imes ext{π}}{4}.

Transition to Bearing Stress

  • Concept of Bearing Stress:
    • Similar to normal stress but focuses on the area of contact between two materials under normal load.
    • Defined as:
    • extBearingStress=FAextcontactext{Bearing Stress} = \frac{F}{A_{ ext{contact}}}.
  • Characteristics of Bearing Stress:
    • Contact area must be correctly identified to ensure accurate calculations.
    • Different types of materials may yield different resistance to bearing stress.

Future Topics

  • Next discussion will focus on:
    • Inclined Stress: How it relates to shear and normal stress under load conditions.
    • Revisit concepts of bearing stress, illuminating its applications in different contexts.

Important Reminders

  • Final Exam Date: May 13, from 8 AM to 10 AM in the classroom.
  • Always refer to specific equations for calculations and reinforce with practical examples.
  • Maintain accuracy in hand calculations and application of theoretical frameworks to practical situations.