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Bending theory of beams and plates

  • 03-06-2009 6:30am
    #1
    Closed Accounts Posts: 882 ✭✭✭


    Hi guys,

    the question is "explain the difference between the behaviour of a plate and a beam in bending with the help of the moment-curvature relationship"

    I originally thought plate theory was the same as beam theory--i.e. viewing a thin section of a plate or slab as a beam, but plates/slabs have more ductility than a beam which allows for better moment distribution than a beam, with the moment curvature relationship still holding for a plate as it does for a beam.

    I've got a sample answer from someone else from a previous year and they say the opposite - that beams have the ability to deform plastically whilst slabs don't and that the moment curvature relationship for a plate is just linear and then failure, whereas for a beam it's linear elastic and then plastic. I thought it was the other way around???

    If anyone could help I'd be most grateful (exam's at 2 today! :eek:). No one seems to have a definitive answer on this.

    Thanks!


Comments

  • Posts: 16,720 ✭✭✭✭ [Deleted User]


    Pop into your lecturer in the next few hours. They expect a few people to drop in with paniced questions :)


  • Registered Users, Registered Users 2 Posts: 1,639 ✭✭✭Turbulent Bill


    Don't have a definitive answer on this (or even close to one), but I'd imagine the difference is due to the plate having more than two boundary conditions (it will have at least 3 edges), whereas a beam generally only has 2 if it's supported at its ends. Most beam and plate theory is linear elastic, small-deflection only, so I don't think the failure behaviour should differ - the same failure criteria should apply.

    As Donal said, ask your lecturer, but don't worry if you can't get him/her - it's only a single question. Good luck!


  • Moderators, Science, Health & Environment Moderators Posts: 23,248 Mod ✭✭✭✭godtabh


    Consider it as a concerete slab built in on all sides.

    Take a step back and work it out from first principles


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