(a) Three-hinged arch
FIGURE 52. Prestress moment diagram.
the trajectory has not affected the value OfW 1 and W 2 , the value ofMpb remains constant.
Thus, Mkb = Mpb - (-Fteb) =F,{1 .224 - 2.0) = -0.776F,.
- Evaluate the prestress moment at midspan
Thus, Mpj = -Ffed+ MM = F,(-0.20 - V 2 x 0.776)712 = -4704 ft-lb (-6378.6 N-m); Mpe =
F,(-0.24 - Y 2 x 0.776)712 = -5024 ft-lb (-6812.5 N-m).
These results are identical with those in the previous calculation procedure. The
change in the eccentricity moment is balanced by an accompanying change in the conti-
nuity moment. Since three points determine a parabolic arc, the prestress moment dia-
gram coincides with that in Fig. 52. This constitutes the solution by method 1. - Evaluate the prestress moments
Do this by replacing the prestressing system with two hypothetical systems that jointly in-
duce eccentricity moments identical with those of the true system.
Let e denote the original eccentricity of the prestressing force at a given section and
&e the change in eccentricity that results from the linear transformation. The final eccen-
tricity moment is -Ft(e + ke) = -(F 1 C + F 1 ^e).
Consider the beam as subjected to two prestressing forces of 96 kips (427.0 kN) each.
One has the parabolic trajectory described in the previous calculation procedure; the other
has the linear trajectory shown in Fig. 53, where ea = Q,eb = -0.80 in (-20.32 mm), and ec
Position of unit load
for zero moment
at D
FIGURE 53. Hypothetical prestressing system and forces exerted on concrete.