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SOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMESSOLID STRUCTURES 2 PIN-JOINTED FRAMES
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1.155P (C) = 6kN → Pmax = 5.2kN Schedule 2022-23 Semester 1 (revised) Week Thursday 3-5pm (YOLC-LT1) 1 Intro to module (^2) Equilibrium at a point (^3) Equilibrium of a rigid body (^4) Employability (^5) Pin-jointed frames – method of joints (^6) Pin-jointed frames – method of sections (^7) STUDY WEEK (^8) Friction (^9) Stress
(^10) Stress (^11) Axial deformation (^12) Compatibility INTERIM ONLINE ASSESSMENT (20%)
Forces in truss members using the method of sections.
In the method of sections, a truss is divided into two parts by taking an imaginary “cut” (shown here as a-a) through the truss. Since truss members are subjected to only tensile or compressive forces along their length, the internal forces at the cut members will also be either tensile or compressive with the same magnitude as the forces at the joint. This result is based on the equilibrium principle and Newton’s third law.
in compression. (Please note that you can also assume forces to be either tension or compression by inspection as was done in the figures above.)
H B
Given: Loads as shown on the truss and ignoring self-weight. Find: The force in members KJ, KD, and CD. Plan: a) Determine the support reactions at A. b) Take a cut through members KJ, KD and CD. c) Work with the left part of the cut section. Can also work with right part of cut. Try it! d) Apply the E-of-E to find the forces in KJ, KD and CD.
Analyzing the entire truss for the reaction at A, we get FX = 0: AX = 0. A moment equation about G to find AY results in:
56.7 kN
x (+) y (+) M (+)
Now take moments about point D. Why do this?
Now use the x- and y-direction equations of equilibrium.
56.7 kN x (+) y (+) M (+)
Video worked solution on Canvas Determine the force in members BC, CF, and FE. Take P 1 = 480 kN and P 2 = 780 kN.
Supporting reading/reference