If the rib has hinged joints at the ends, as in Fig. 34, obviously
there can be no bending moment at either of those two points, and hence
the two equations of condition which were required in connection with
Fig. 33 to determine them will not be needed. There is, therefore,
no restriction as to the angle of inclination of the centre line of
the rib at those two points. Again, it is obvious that either end _A_
or _B_ may have vertical movement, i.e., deflection in reference to
the other, without affecting the condition of stress in any member of
the rib; but it is equally obvious that neither _A_ nor _B_ can be
moved horizontally, i.e., deflected in reference to the other, without
producing bending in the rib and developing stresses in the various
members. The unknown quantities in this case are, therefore, only the
horizontal thrust _H_ exerted at the two springing points _A_ and
_B_, and the two vertical reactions, making a total of three unknown
quantities, equations for two of which will be given by equations
(36) and (37). The other equation required is the third expression in
equation (57), expressing the condition that the horizontal deflection
of either of the points _A_ or _B_ in respect to the other is zero,
since the span _AB_ is supposed to remain unchanged. By the application
of the graphical method to this case, as to the preceding, the
employment of equations (36), (37), and (58) will afford an easy and
quick determination of the three unknown quantities, whatever may be
the curvature of the rib.
A
⎲
⎳ _nMy_ = 0. (58)
B
If the reactions and horizontal thrust _H_ are found, stresses in every
member may readily be computed and the complete design made.
If the arch is three-hinged, as in Fig. 35, the condition that the
bending moment must be zero at the crown _C_ under all conditions of
loading gives a third statical equation independent of the elastic
properties of the structure which, in connection with equations (36)
and (37), give three equations of condition sufficient to determine the
two vertical reactions and the horizontal thrust _H_. In this case, as
has already been stated, no elastic equations of condition are required.
The determination of the end reactions, bending moments, and horizontal
thrust _H_, in these various cases, is all that is necessary in order
to compute with ease and immediately the stresses in every member of
the rib. These computations are obviously the final numerical work
required for the complete design of the structure. These procedures are
always followed, and in precisely the manner indicated, in the design
of arched ribs by civil engineers, whether the rib be articulated,
i.e., with open bracing, or with a solid plate web, like those of the
Washington Bridge across the Harlem River.
CHAPTER XI.
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