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Intersecting Chords: Difference between revisions

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* but, for small deflections, Δ<sup>2</sup> will be negligible
* but, for small deflections, Δ<sup>2</sup> will be negligible
* so '''Bending Radius ''(R)'' = cd<sup>2</sup> ÷ (8 x Δ)'''
* so '''Bending Radius ''(R)'' = cd<sup>2</sup> ÷ (8 x Δ)'''
''(see ‘Structures’ by [http://en.wikipedia.org/wiki/J.E._Gordon J.E.Gordon] ISBN  0 14 02.1961 7)'' </span>
''(see '''<dtamazon product="0306812835" type="text">Structures: Or Why Things Don't Fall Down by J.E.Gordon</dtamazon>)''''' </span>
|[[File:BeamChordsTheorem.png|400px|right]]
|[[File:BeamChordsTheorem.png|400px|right]]
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Latest revision as of 16:22, 4 July 2017

ChordTheorem.jpg

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


The Intersecting Chords Theorem states that the relationship (ao x ob = co x od) is true for any two intersecting chords, whether or not one of them is a diameter.

Measuring Beam Deflections

The theorem can be useful when measuring the radius of bending of a deflected beam if one of the chords is taken to be the length of the beam e.g.

  • set up a strip of material as a simple beam
  • note the distance between supports (cd)
  • apply a central load to make it bend - or ‘deflect’(Δ) - therefore co = od = ½cd
  • 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 Bending Radius (R) = cd2 ÷ (8 x Δ)

(see Structures: Or Why Things Don't Fall Down by J.E.Gordon)

BeamChordsTheorem.png