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Clark-Nielsen (Wood-Armer for in plane forces)
The Wood-Armer
equations
resolve bending and twisting moments for the purpose of RC slab
design. Similar equations may be derived to resolve the
forces required to resist an in plane force triad consisting
of two in plane forces per unit length (Nx, Ny) and an in plane
shear force per unit length (Nxy). These equations are
generally known as the Clark-Nielsen equations.
For a full explanation and derivation of the formulae, the
reader is referred to either:
- "Concrete slabs: analysis and design" L.A Clark
and R.J Cope (Elsevier Applied Science)
- "Concrete Bridge Design to BS5400" L.A Clark
(Construction Press) Chapter 5 (section entitled
"Reinforced Concrete Plates") and Appendix A
By reference to
"Concrete Bridge Design to BS5400" Appendix A, the
Clark-Nielsen calculation may be carried out by
following the procedure below.
All calculations proceed after the determination of the
in-plane stress field Nx, Ny, Nxy.
For an elastic section subject only to in-plane forces, the
stress field is:
Top:
NxT=Nx/2, NyT=Ny/2, NxyT=Nxy/2
Bottom: NxB=Nx/2, NyB=Ny/2, NxyB=Nxy/2
Note that although the
sign convention for Nxy differs between LUSAS and "Concrete
Bridge Design to BS5400", Nxy always appears in the equations
below as a squared or an absolute value and thus no amendment is
required to take account of the sign convention.
The equations are described in a form that can be
translated directly to a spreadsheet format:
Top
reinforcement
-
Determine
the generalized Clark-Nielsen forces:
NxT1=NxT+2*NxyT*cotø+NyT*(cotø)^2+ABS((NxyT+NyT*cotø)/sinø)
NøT1=NyT/((sinø)^2)+ABS((NxyT+NyT*cotø)/sinø)
-
Suppose NxT1<0; top layer
is in X-direction compression
NxT2=0
NøT2=(1/(sinø)^2)*(NyT+ABS((NxyT+NyT*cotø)^2/(NxT+2*NxyT*cotø+NyT*(cotø)^2)))
-
Suppose NøT1<0;
top layer is in ø-direction compression
NxT3=NxT+2*NxyT*cotø+NyT*(cotø)^2+ABS((NxyT+NyT*cotø)^2/NyT)
NøT3=0
-
Select
the appropriate values from the above for output.
Note that if NxT1<0 and NøT1<0,
then no top reinforcement is required
Nx(T)=IF(NøT1<0,IF(NxT3<0,0,NxT3),IF(NxT1<0,0,NxT1))
Nø(T)=IF(NxT1<0,IF(NøT2<0,0,NøT2),IF(NøT1<0,0,NøT1))
Bottom
reinforcement
Concrete
forces (top)
-
Determine
the generalized Clark-Nielsen concrete force
FcT1=IF(FcTI<0,-2*FcTI*(cotø-cscø),-2*FcTI*(cotø+cscø))
where FcTI=NxyT+NyT*cotø
-
Suppose
NxT1<0; top layer is in X-direction compression
FcT2=((NxT+NxyT*cotø)^2+(NxyT+NyT*cotø)^2)/(NxT+2*NxyT*cotø+NyT*(cotø)^2)
-
Suppose
NøT1<0; top layer is in ø-direction compression
FcT3=NyT+(NxyT^2/NyT)
-
Suppose
NxT1<0 and NøT1<0,
there is no cracking and "concrete force parallel to the
crack" has no meaning.
Reasonable value to give is the second (most
compressive) principle stress:
FcTP=(NxT+NyT)/2-SQRT(((NxT-NyT)/2)^2+NxyT^2)
-
Select
the appropriate values from the above for output.
Fc(T)=IF(AND(NøT1<0,NxT1<0),FcTP,IF(NøT1<0,FcT3,IF(NxT1<0,FcT2,FcT1)))
Concrete
forces (bottom)
A simple example may be used to demonstrate the Clark-Nielsen
calculation for orthogonally placed (minimised area)
reinforcement.
The example used here is a a shell subjected to an
unsymmetrical tensile load; a thin rectangular slab fixed in
translation at one edge and with a point load applied to an
opposing corner. No
bending field (Mx, My, Mxy) will be generated, while a stress
field will be generated where various combinations of positive
and negative stresses for Nx, Ny and Nxy exist, enabling the
verification of the Clark-Nielsen calculations for a variety of
conditions. The
calculations for Top and Bottom face reinforcement will produce
the same result and so a single hand calculation will verify
both results.
- Rectangular
surface, plan dimensions length 16 units, width 10 units
- Mesh attributes: Any quadrilateral shell element (QSI4
elements used in subsequent calcs) regular mesh of element size 1 unit
- Geometric attributes: thickness 0.2 units
- Material attributes: E=1E6, poissons ratio=0.3
- Supports:
fixed
in translation on bottom edge
- Loading attributes: Structural
load, Concentrated in Y direction 100 units total
Download
Clark Nielsen example model (LUSAS mdl file)
Stress field from LUSAS Modeller, extracted at 4 nodes for
calculations to be checked explicitly:
|
Node
|
29
|
161
|
129
|
183
|
|
Nx
|
-87.673
|
4.765
|
2.804
|
-11.192
|
|
Ny
|
-29.469
|
47.202
|
7.529
|
-0.574
|
|
Nxy
|
-31.530
|
-9.839
|
0.321
|
4.694
|
Calculation of Clark-Nielsen stresses by hand, determined
from the stress field (Nx, Ny, Nxy) using the procedure
explained above. Download
spreadsheet calculations (MSExcel format)
|
Node
|
29
|
161
|
129
|
183
|
|
|
0.000
|
7.302
|
1.563
|
0.000
|
|
Ny(T)=Ny(B)
|
0.000
|
28.520
|
3.925
|
0.698
|
|
Fc(T)=Fc(B)
|
-49.506
|
-9.839
|
-0.321
|
-6.581
|
Clark-Nielsen stresses from LUSAS
Modeller, extracted at the
same 4 nodes for comparison to the hand calculations undertaken:
|
Node
|
29
|
161
|
129
|
183
|
|
Nx(B)
|
0.000
|
7.302
|
1.563
|
0.000
|
|
Ny(B)
|
0.000
|
28.520
|
3.925
|
0.698
|
| Fc(B) |
-50.740 |
-9.839 |
-0.321 |
-6.581 |
By inspection the results tabulated above agree closely with
those derived by hand calculation and demonstrate that the Clark-Nielsen
calculations for this example are satisfactory.
Other Wood Armer
related topics
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