Solid mechanics- Lab report, Essays (university) of Applied Solid Mechanics

Lab report detailing experiment which took place involving bending in beams

Typology: Essays (university)

2018/2019

Uploaded on 01/18/2019

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Bending in Beams
Sheffield Hallam University
Department of Engineering and Mathematics
Faculty of ACES
For the attention of: Mo Islam
Student Name: Daniel Lonergan
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Daniel Lonergan
55-403198 Principles of Solid Mechanics and Dynamics
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Bending in Beams

Sheffield Hallam University

Department of Engineering and Mathematics

Faculty of ACES

For the attention of: Mo Islam

Student Name: Daniel Lonergan

Daniel Lonergan

55-403198 Principles of Solid Mechanics and Dynamics

Student ID: 27041290

Module code & name: 55-403198 Principles of Solid Mechanics and

Dynamics

Course name: Materials Engineering

Date: 26 th^ February 2018

Introduction

Structural beams are one of the most widely used support mechanisms in everyday society, from buildings to bridges to roof structures, they are used in engineering application very frequently, therefore it is vital to understand the concepts of stresses and strains and how these structural beams deflect. Also, it is important to know how the relationships between these concepts, bending moments, elastic modulus and deflection are expressed using the elastic bending theory by using the simple bending formula in practice.

To fully understand these concepts in application, the objective of this lab experiment is to carry out two experiments using two different methods using different supports and fixing conditions to understand how the bending moment distribution (BDM) can be controlled. This will also allow examination of how materials properties and sectional properties will affect bending behaviour of these structural beams.

Background Theory

The theory behind this experiment comes from simple bending taken from the elastic bending theory also known as the ‘Euler- Bernoulli’ theory. Which states that for a uniform cross-section beam segment subjected to a bending moment that this bending Moment at any given position divided by the second area moment is equal to the stress from the bend at a distance from the neutral axis is equal to the Youngs modulus of the material divided by its radius of curvature from deflection.

The equation follows as thus;