FIGURE 48
lively, are ea = 1 in (25.4 mm); em, = 30 in (762.0 mm); eb = -3 in (-76.2 mm). Evaluate
the prestress shear and prestress moment at section C (a) by applying the properties of the
trajectory at C; (b) by considering the prestressing action of the steel on the concrete in
the interval A C.
Calculation Procedure:
- Compute tfie eccentricity and slope of the trajectory at C
Use Eqs. 66 and 67. Let m denote the slope of the trajectory. This is positive if the trajec-
tory slopes downward to the right. Thus ea - 2em + eb = I - 60 - 3 = -62 in (1574.8 mm);
2>ea - 4em + eb, = 3 - 120 - 3 = -120 in (-3048 mm); em = 2(-62)(20/100)^2 + 120(20/100)
- 1 = 20.04 in (509.016 mm); mc = 4(-62/12)(20/100^2 ) - (-120/12 x 100) = 0.0587.
- Compute the prestress shear
and moment at C
Thus Vp 0 = -mcFt = -0.0587(860,000) =
-50,480 Ib (-224,535.0 N); Mpc = -Fte
= -860,000(20.04) = -17,230,000 in-Ib
(-1,946,645.4 N-m). This concludes the solu-
tion to part a. - Evaluate the vertical
component w of the radial force
on the concrete in a unit
longitudinal distance
An alternative approach to this problem is to
analyze the forces that the tendons exert on
the concrete in the interval AC, namely, the FIGURE 49. Free-body diagram of
prestressing force transmitted at the end and concrete.
the radial forces resulting from curvature of
the tendons.
Consider the component w to be positive
if directed downward. In Fig. 49, Vpr-Vpq =
-Ft(mr - mq); therefore, A^/Ajc = -F,Am/Ax. Apply Eq. 68: dVpldx = -Fjdm/dx =
-(4FJL^2 )(ea ~ 2em + eb)\ but dVpldx = -w. Therefore,
w = Fi ^L = / ' \ fe _ 2em + Cb) (71)
OX \ L, /
-Trajectory
Trajectory