Advanced Methods of Structural Analysis

(Jacob Rumans) #1

98 4 Three-Hinged Arches


where span for archACB^0 with support points on the same level isLD
lCl 0 D 48 m. ForxD 42 m (supportB) the ordinateyDD3:5m, so


tan ̨D


l

D

3:5
42

D0:0833!cos ̨D0:9965!sin ̨D0:08304:

8m

C
B
A

P=10kN

ZA

ZB

R′A

ac=24m bc=18m R′B
l=42m l^0 =6m

x 12m
k=6m

D=3.5m

k f h
a
f 0 • B′

L=48m

x

y

yk= 3.5m

Fig. 4.14 Design diagram of an askew three-hinged arch


Other geometrical parameters are


f 0 DaCtan ̨D 24 tan ̨D2:0m!fD 8  2 D 6 m!
hDfcos ̨D 6 0:9965D5:979m:

(a)

ForxD 6 m (sectionk), the ordinateykD3:5m.


4.5.1.1 Reactions and Bending Moment at Sectionk


Reactions of supportsIt is convenient to resolve total reaction at pointAinto two
components. One of them,R^0 A, has vertical direction and other,ZA, is directed along
lineAB. Similar resolve the reaction at the supportB. These components areR^0 B
andZB. The vertical forcesR^0 AandR^0 Bpresent apartof the total vertical reactions.
These vertical forces may be computed as for reference beam


R^0 A!

P
MBD 0 WR^0 A 42 CP 12 D 0 !R^0 AD2:857kN;
R^0 B!

P
MAD 0 W R^0 B 42 P 30 D 0 !R^0 BD7:143kN:

(b)

Since a bending moment at crownCis zero then

ZA!

X
MCleft 0 WZAhMC^0 D 0 !ZAD

MC^0
h

D

2:857 24
5:979

D11:468kN;
ZADZBDZ;
(c)
whereMC^0 is a bending moment at sectionCfor reference beam.
ThrustHpresents the horizontal component of theZ, i.e.,


HDZcos ̨D11:4680:9965D11:428kN: (4.15)
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