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Intersecting Chords: Difference between revisions

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It can be useful when measuring the radius of bending of a deflected beam, for example, if one of the chords is taken to be the length of the beam
It can be useful when measuring the radius of bending of a deflected beam, for example, if one of the chords is taken to be the length of the beam
[[File:DeflectedBeamChords.jpg|400px|right]]
e.g.
e.g.
* set up a strip of material as a simple beam
# set up a strip of material as a simple beam
* note the distance between supports '''''(cd)'''''
# note the distance between supports '''''(cd)'''''
* apply a central load to make it bend - or '''''[[Beam Deflection|‘deflect’(Δ)]]''''' - therefore '''co = od = ½cd'''
# apply a central load to make it bend - or '''''[[Beam Deflection|‘deflect’(Δ)]]''''' - therefore '''co = od = ½cd'''
* measure the deflection '''''(ob)'''''
# measure the deflection '''''(ob)'''''
* Bending Radius (R) can be calculated as follows:
Bending Radius (R) can be calculated as follows:
    ao x ob = co x od
* ao x ob = co x od
(2R-Δ) x Δ = ½cd x ½cd
* (2R-Δ) x Δ = ½cd x ½cd
but, for small deflections, Δ<sup>2</sup> will be negligable
* but, for small deflections, Δ<sup>2</sup> will be negligible
so R = cd<sup>2</sup> ÷ 8 x Δ
* so R = cd<sup>2</sup> ÷ 8 x Δ
''(see ‘Structures’ by J.E.Gordon ISBN  0 14 02.1961 7)''

Revision as of 11:33, 7 November 2014

ChordTheorem.jpg

This theorem relates to a characteristic of a cyclic quadlitateral, the diagonals of which are two intersecting chords of the circumscribing circle.

It can be useful when measuring the radius of bending of a deflected beam, for example, if one of the chords is taken to be the length of the beam

e.g.

  1. set up a strip of material as a simple beam
  2. note the distance between supports (cd)
  3. apply a central load to make it bend - or ‘deflect’(Δ) - therefore co = od = ½cd
  4. measure the deflection (ob)

Bending Radius (R) can be calculated as follows:

  • ao x ob = co x od
  • (2R-Δ) x Δ = ½cd x ½cd
  • but, for small deflections, Δ2 will be negligible
  • so R = cd2 ÷ 8 x Δ

(see ‘Structures’ by J.E.Gordon ISBN 0 14 02.1961 7)