Bridge Abutment Design
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T Christie, M Glendinning, J Bennetts, S Denton 1
DESIGN ILLUSTRATION – BRIDGE ABUTMENT DESIGN
T Christie, Parsons Brinckerhoff, Bristol, UK M Glendinning, Parsons Brinckerhoff, Cardiff, UK J Bennetts, Parsons Brinckerhoff, Bristol, UK S Denton, Parsons Brinckerhoff, Bristol, UK
Abstract This paper provides a calculation showing how the heel l ength and overall length of the base slab of a conventional cantilever gravity abutment can be determined in accordance with the [1],[2],[3],[4],[5],[6] requirements of the Eurocodes and relevant non-contradictory information . Sliding resistance, bearing resistance and overturning stability are all considered. The calculations illustrate the requirements of the Eurocodes in regard to loading, partial factors, combination of actions and other issues which require a somewhat different approach from that used with pre-Eurocode designs. designs.
Notation The symbols used used in the calculations are as for the Eurocode Eurocode and PD 6694-1. Other symbols are defined in the text of the calculations or identified in the Figure 1.
The Design Problem An 8m high, 12m wide abutment abutment of a multispan continuous bridge bridge is shown in Figure 1. It is required to determine the heel length ( Bheel) and the overall base length ( B) of this abutment necessary to satisfy the requirements of sliding resistance, bearing resistance and overturning stability specified in the Eurocodes. Eurocodes. The abutment is subject to three notional notional 3m wide lanes of traffic surcharge. The characteristic actions and soil parameters applied to the abutment are as follows: Permanent actions Weight of steel beams Weight of concrete deck Weight of surfacing Actions for traffic group gr2 Maximum vertical traffic reaction Uplift due to traffic on adjacent span Braking and acceleration action UDL surcharge (from PD 6694-1 Table 5) Line load surcharge (from PD 6694-1 Table 5)
50 72 36
V traffic 100 traffic U traffic 30 traffic H braking 50 braking h 20Ka F 2 x 330 K a
kN/m kN/m kN/m
kN/m kN/m kN/m kN/m² kN/lane
T Christie, M Glendinning, J Bennetts, S Denton 2
Soil parameters: Granular backfill Weight density Angle of shearing resistance Clay foundations Weight density Undrained shear strength Angle of shearing resistance Critical state angle of shearing resistance Overburden pressure ( q) = γbf x Z q
kN/m²
' bf
18 35
cu ' ' cv q
18 100 27 23 12
kN/m² kN/m²
γbf
kN/m²
The initial dimensions of the foundations are to be based on traffic load group gr2 in which the characteristic value of the multi-component action is taken as the frequent value of Load Model 1 in combination with the frequent value of the associated surcharge model, together with the characteristic value of the braking and acceleration action, (see the UK National Annex to BS EN 1991-2:2003, NA.2.34.2). Wind is not required to be considered in combination with traffic model gr2 and thermal actions are not considered to be significant and are therefore neglected in these preliminary calculations. The water table is well below foundation level and need not be considered, but it is r equired to check sliding resistance and bearing resistance at STR/GEO for both the drained and the undrained condition. As no explicit settlement calculation is to be carried out at SLS it is required to be demonstrated that a sufficiently low fraction of the ground strength is mobilised (see BS EN 1997-1:2004, 2.4.8(4)). This requirement will be deemed to be satisfied if the maximum pressure at SLS does not exceed one third of the characteristic resistance (see PD 6694-1, 5.2.2).
T Christie, M Glendinning, J Bennetts, S Denton 3
Transverse Dimensions
Abutment width W abut = 12m
Y= 1.5
Notional lane widths W lane = 3m X=0.25
The traffic on the third notional lane is subject to a 0.5 lane factor so that the effective number of lanes N lane used in the surcharge calculation is 2.5 (see UK National Annex to BS EN 19912:2003, NA 2.34.2 )
Z
Z q P Bheel B
Figure 1. Base slab design for a gravity cantilever bridge abutment
Methodology for Preliminary Design Calculations are carried out "in parallel" for the SLS characteristic combination of actions and for STR/GEO Combinations 1 and 2, using Design Approach 1 (see BS EN 1997-1:2004, 2.4.7.3.4.2). Partial factors on actions are taken from the UK National Annex to BS EN 1990:2002, Table NA.A2.4 (B) and (C) , partial factors for soil parameters are from the UK National Annex to BS EN 1997-1:2004, Table A.NA.A.4 and ψ factors from the UK National Annex to BS EN 1990:2002, Table NA.A2.1 . The preliminary calculations are carried out on a "metre strip" basis The following procedure was used for the preliminary design: 1. Calculations were carried out "in parallel" for the SLS characteristic combination and for STR/GEO Combinations 1 and 2. This allowed a side-by-side comparison of the three limit states to be made and repetitive calculations to be minimised. 2. The following actions were calculated: (a) The total horizontal action on the wall ( H ) due to active earth pressure, traffic surcharge (factored by ψ 1) and braking and acceleration (see Table 1). . (b) The minimum vertical reaction due to deck reaction ( V DL;inf ) and uplift caused by traffic on remote spans ( U ) (see Table 2). (c) The maximum vertical reaction due to the weight of the deck and traffic (see Table 3).
T Christie, M Glendinning, J Bennetts, S Denton 4
(d) The vertical pressure exerted by the backfill and the base slab ( γbf Z ). (For convenience in these preliminary calculations, the density of the concrete in the base slab and abutment wall was considered to be the same as the density of the backfill (γbf )). 3. The length of the heel ( Bheel) required to provide enough weight to resist sliding for the drained foundation was found as follows: The sliding resistance due to the weight of the deck less traffic uplift ( Rvx) was taken as (V DL;inf - U )tan ' cv. The required sliding resistance due to the weight of the backfill and abutment was therefore H - Rvx. The weight of the abutment and backfill required to provide this resistance was therefore equal to ( H - Rvx)/ tan ' cv and this had to equal Bheelγbf Z . The required value of Bheel therefore equalled ( H - Rvx)/(γbf Ztan ' cv) and this equals ( H - Rvx)/( μγbf Z ) as in Table 2. 4. As it was recognised that the loads on the toe and the use of the correct density of concrete would increase the sliding resistance, the selected figure of Bheel in Table 2 was taken as slightly less than the figure of Bheel obtained from the calculation. 5. For undrained foundations the total overall base length for sliding, ( B1) was taken as H d / cu;d as in Table 2 (see BS EN 1997-1:2004, Equation 6a ). 6. The required overall base length is also dependent on other factors such as the requirement to keep the load within the middle third at SLS and within the middle two-thirds at ULS, the bearing resistance for the drained and undrained condition and in some circumstances (although not for this structure) for resistance to overturning. In all these calculations the eccentricity of the vertical action is required. To obtain this it is convenient to take moments about the back of the heel (point P on Figure 1) rather t han the centre of the base, because the bearing resistance calculations are iterative, but the moments about the back of the heel do not alter with varying toe lengths, provided the value of Bheel is not changed. This allows multiple iterations to be carried out with minimal change to the data. 7. Moments about P were calculated (see Tables 4 and 5). The distance of the line of action from P is eheel, where eheel = M/V and M is the total moment about P and V is the total vertical load. It can be shown that to satisfy the SLS middle third condition (see PD 6694-1, 5.2.2), the overall base length ( B2) must be 1.5 eheel, and to satisfy the ULS middle two-thirds condition (see BS EN 1997-1:2004, 6.5.4), the overall base length ( B3) must be 1.2 eheel (see Table 5). 8. To determine the overall base length ( B) required to provide adequate bearing resistance for the undrained and drained conditions, an iterative calculation with increasing values of B was carried out, starting with the maximum value of the base length found from the sliding calculations (i.e the largest of B1, B2, or B3) and increasing progressively until the bearing resistance for the undrained and drained conditions drained and the toe pressure limitation at SLS were all satisfied.
T Christie, M Glendinning, J Bennetts, S Denton 5
9. The selected value of B and the calculations in Table 6 and 7 are based on the final iteration, that is the minimum value of B necessary to satisfy the bearing resistance requirements. The calculations largely replicate the equations given in BS EN 1997-1:2004, Annex D. Notes
The abutment is assumed to be transversely stiff and so the traffic loads can be distributed over the whole width of the abutment (see PD 6694-1, Table 5 Note C)
For convenience in the preliminary design, the density of the concrete in the base slab and wall is considered to be the same as the density of the backfill ( bf ).
It should be noted that the same partial factor G is applied to the vertical and horizontal earth pressure actions (see PD 6694-1, 4.6). This is only likely to be relevant in a sliding resistance calculation if STR/GEO Combination 1 is more critical than Combination 2.
In these calculations a model factor, Sd;k = 1.2 has been applied to the horizontal earth pressure at ULS in order to maintain a similar level of reliability to previous practice (see PD 6694-1, 4.7).
In Tables 1 to 7 the figures given in the SLS column are the characteristic values of material properties and dimensions and the characteristic or representative values of actions per metre width. The figures in the STR/GEO columns are the design values unless otherwise indicated.
T Christie, M Glendinning, J Bennetts, S Denton 6
Horizontal actions
SLS
Height of abutment Z
STR/GEO Comb. Comb. 1 2
Z
8.00
8.00
8.00
Partial factor on soil weight
G;sup
1.00
1.35
1.00
Backfill density = γbf;k G;sup
bf,d
18.0
24.3
18.0
M
1.00
1.00
1.25
' bf;d
35.0
35.0
29.3
K a
0.27
0.27
0.34
Sd:K
1.00
1.20
1.20
Design active pressure action bf;d K a Sd;K Z² /2 = H ap;d
H ap;d
156
253
237
kN/m
Surcharge UDL = hW lane N lane / Wa but = (20K a) x 3 x 2.5/12 = h;ave
h;ave
3.39
3.39
4.29
kN/m
H sc;udl
27.1
27.1
34.3
kN/m
H sc;F
37.3
37.3
47.2
kN/m
H sc;comb
64.4
64.4
81.6
kN/m
γQ
1.00
1.35
1.15
1
0.75
0.75
0.75
H sc;d
48.3
65.2
70.4
kN/m
H braking;k
50.0
50.0
50.0
kN/m
Q
1.00
1.35
1.15
H braking;d
50.0
67.5
57.5
kN/m
H d
254
386
365
kN/m
' bf;k = 35;
Partial factor M on tan( ' bf;k )
-1
tan (tan( ' bf;k )/ M ) = ' bf;d Active pressure coefficient K a incl. ( M ) (1-sin ' bf;d )/(1+sin bf;d ) Model factor Sd:K
Surcharge UDL action h;ave x Z = H sc;udl
m
kN/m
Surcharge Line Load/m = F K a N lane / W abut = 2 x 330K a x 2.5/12 = H sc;F Combined surcharge/m H sc;udl + H sc;F = H sc;comb Partial factor on surcharge
γQ
1 = 0.75 for surcharge in traffic group grp2 Design surcharge = H sc;d = H sc;comb.ψ.γQ
Characteristic braking action H braking;k Partial factor on braking Q Braking action /m H braking:d = H braking;k Q TOTAL DESIGN HORIZONTAL ACTION H d = H ap;d + H sc;d + H braking;d
Table 1. Horizontal actions
3
2
T Christie, M Glendinning, J Bennetts, S Denton 7
Minimum vertical actions and sliding resistance
Height of abutment Z
SLS
STR/GEO Comb. Comb. 1 2
Z
8.00
8.00
8.00
m
Characteristic deck weight 50+72+36 = 158
V DL;k
158
158
158
kN/m
Inferior partial factor on deck weight
G;inf
1.00
0.95
1.00
V DL;inf;d
158
150
158
kN/m
U k
30.0
30.0
30.0
kN/m
Q;sup
1.00
1.35
1.15
1= 0.75 for vertical traffic actions in traffic group grp2
1
0.75
0.75
0.75
Factored uplift from traffic U k. Q = U d
U d
22.5
30.4
25.9
kN/m
Minimum vertical loads from deck and traffic V x;d = V DL;inf;d – U d
V x;d
136
120
132
kN/m
M
1.00
1.00
1.25
d
0.42
0.42
0.34
Rvx;d
57.5
50.8
44.9
kN/m
H d
254
386
365
kN/m
Reqd resistance from backfill [ H d – Rvx;d ]
Rreq
197
335
320
kN/m
Density of backfill (Table 1) bf;d Frictional shear stress due to backfill: [ d bf;d Z ]
b;df
18.0
24.3
18.0
kN/m
3
61.1
82.5
48.9
kN/m
2
Bheel;req
3.22
4.06
6.55
m
B heel
6.25
6.25
6.25
m
Inferior weight of deck Uplift from traffic Superior partial factor on uplift
' cv;k = 23;
Partial factor M on tan( ' cv;k )
= d Coefficient of friction tan( ' cv;k )/ M Sliding resistance due to V x d .V x;d = Rvx;d
Horizontal action from Table 1, H d
Required Bheel= Rreq / ( d bf;d Z ) SELECTED VALUE OF HEEL B heel Rounded down, see Methodology para. (4)
Partial factor M on cu;k
cu
1
1
1.4
Undrained shear strength cu:d = cu;k / c u
cu:d
100.0
100.0
71.4
kN/m
OVERALL BASE LENGTH B1 = H d /c u;d
B1
2.54
3.86
5.11
m
cu;k = 100;
Table 2. Minimum vertical actions and sliding resistance
2
T Christie, M Glendinning, J Bennetts, S Denton 8
Maximum vertical actions
Height of abutment Z
SLS
STR/GEO Comb. Comb. 1 2
Z
8.00
8.00
8.00
m
Selected value of Bheel (Table 2)
Bheel
6.25
6.25
6.25
m
Partial factor on steelwork G;sup
G;sup
1.00
1.20
1.00
50.0
60.0
50.0 kN/m
1.00
1.35
1.00
72.0
97.2
72.0 kN/m
1.00
1.20
1.00
36.0
43.2
36.0 kN/m
V DL;sup;d
158
200
158 kN/m
V traffic;k
100.0
100.0
100.0 kN/m
Partial factor on traffic Q
Q
1.00
1.35
1.15
1 = 0.75 for vertical traffic actions in traffic group grp2
1
0.75
0.75
0.75
V traffic;d
75.0
101
86.3 kN/m
bf;d
18.0
24.3
18.0 kN/m
Bheel
6.25
6.25
6.25 m
V bf;d
900
1215
900 kN/m
V max;d
1133
1517
1144 kN/m
Weight of steelwork = 50 G;sup Partial factor on concrete G;sup
G;sup
Weight of concrete = 72 G;sup Partial factor on surfacing G;sup
G;sup
Weight of surfacing = 36 G;sup Superior weight of deck/m V DL;sup;d
Characteristic vertical action from traffic V traffic;k
Design traffic action/m V traffic;d =V traffic;k Q
Density of backfill bf;d (Table 1) Selected width of heel Bheel (Table 2) Design weight of backfill/m V bf;d = bf;d Z B heel TOTAL MAXIMUM VERTICAL LOAD V max;d = V DL;sup;d + V traffic;d + V bf;d
Table 3. Maximum vertical actions
3
3
3
3
T Christie, M Glendinning, J Bennetts, S Denton 9
Moments about the underside of the base due to horizontal actions
Active Pressure action H ap;d including Sd;K (Table 1)
SLS
H ap;d
Lever arm = Z /3
STR/GEO Comb. Comb. 1 2
156
253
237
kN/m
2.67
2.67
2.67
m
Active Moment M ap;d = H ap;d Z/3
M ap;d
416
674
633
kNm
Surcharge UDL action H sc;udl (Table 1)
H sc;udl
27.1
27.1
34.3
kN/m
4.00
4.00
4.00
m
M sc;udl
108
108
137
kNm
H sc;F
37.3
37.3
47.2
kN/m
Lever arm = Z
Z
8.00
8.00
8.00
m
H sc;F Z = M sc;F
M sc;F
298
298
378
kNm
M sc;comb
406
406
515
kNm
Q for surcharge
Q
1.00
1.35
1.15
1 = 0.75 for surcharge in traffic group grp2
1
0.75
0.75
0.75
M sc;d
305
412
444
kNm
H braking;d
50.0
67.5
57.5
kN/m
La;b
6.50
6.50
6.50
m
325
439
374
kNm
1046
1525
1451
kNm
Lever arm = Z /2 H sc;udl x Z /2 = M sc;udl
Surcharge Line Load H sc;F (Table 1)
Combined surcharge moment M sc;udl + M sc;F
Design surcharge moment M sc;comb Q 1
Braking action/m H braking;d (Table 1) Lever arm for braking ( Z -Y ) = La;b = 8 - 1.5 Braking moment M braking;d = H braking;d x La;b MOMENT DUE TO HORIZONTAL ACTIONS, M hor;d = M ap;d + M sc;d + M braking;d
M brakin
;d
M hor;d
Table 4. Moments about the underside of the base due to horizontal actions
T Christie, M Glendinning, J Bennetts, S Denton10
Moments about the back of the heel
Width of heel Bheel
SLS
STR/GEO Comb. Comb. 1 2
Bheel
6.25
6.25
6.25
m
X
0.25
0.25
0.25
m
La;deck
6.00
6.00
6.00
m
V DL;sup;d
158
200
158
kN/m
Deck Moment V DL;sup;d La;deck = M deck;d
M deck;d
948
1202
948
kNm
Traffic Load V traffic;d (Table 3)
V traffic;d
75.0
101
86.3
kN/m
M traffic;d
450
608
518
kN/m
V bf;d
900
1215
900
kNm
M bf;d
2813
3797
2813
kN/m
Total Moment about heel due to vertical actions M vert;d = M deck;d + M traffic;d + M bf;d
M vert;d
4211
5607
4278
kNm
Moment about base due to horizontal Actions (Table 4)
M hor;d
1046
1525
1451
kNm
Total design moment about heel M vert;d + M hor;d = M heel;d
M heel;d
5257
7131
5729
kNm
V d
1133
1517
1144
kN/m
Line of action in front of heel eheel = M heel / V
eheel
4.64
4.70
5.01
m
Total length B2 required for middle third at SLS = 1.5 eheel (see PD 6694-1 5.2.2)
B2
6.96
Total length B3 for middle two thirds at ULS = 1.2 eheel (see BS EN 1997-1 6.5.4)
B3
Distance of deck reactions behind front of wall X La;deck = Bheel - X
Superior weight of deck V DL;sup;d (Table 3)
Traffic Moment V traffic;d La;deck = M traffic;d Weight of backfill V bf;d (Table 2) Backfill moment V bf;d Bheel /2 = M bf;d
Total vertical load V d (Table 3)
m
5.64
6.01
Table 5. Moments about the back of the heel (Position P on Figure 1)
m
T Christie, M Glendinning, J Bennetts, S Denton11
Bearing Resistance – undrained foundation Geometry of foundation (m) Final B (found iteratively) Heel length Bheel (Table 2) Transverse width of foundation L Inclination Partial factors F applied to M applied to tan M applied to cu M applied to c Properties of foundation material Weight density d (including G) Angle of shearing resistance d Cohesion intercept c d Undrained shear strength cu;d Applied action Horizontal actions H d (Table 1) Vertical action V d (Table 3) Moment about P = M heel;d (Table 4) M heel;d / V = eheel Eccentricity about centre line e = eheel - B /2 Overburden pressure Effective foundation dimensions (m) Effective foundation breadth B = B-2e Effective area for 1m strip design A = B Effective transverse width L = L Undrained bearing resistance (Annex D to BS EN 1997-1 D.3) Bearing parameters for undrained foundations bc = 1-2 /(+2) sc = 1+0.2( B / L ) ic = ½{1+(1- H d / A cu;d )} R/A = (+2)cu;d bc sc ic + qd V d / A Ratio R/V Settlement check 1/3( R/A) at SLS characteristic
Max toe pressure (1+6 e / B)V d / B
SLS
B
STR/GEO Comb. Comb. 1 2
m m m
Bheel L
8.60 6.25 12.0 o 0
8.60 6.25 12.0 o 0
8.60 6.25 12.0 o 0
G cu c
1.00 1.00 1.00 1.00
0.95 1.00 1.00 1.00
1.00 1.25 1.40 1.00
d d c d cu;d
18.0 27.0 0 100.0
17.1 27.0 0 100.0
18.0 22.2 0 71.4
kN/m
H d V d M heel;d eheel e qd
254 1133 5257 4.64 0.34 12.0
386 1517 7131 4.70 0.40 12.0
365 1144 5729 5.01 0.71 12.0
kN/m kN/m kNm/m m m 2 kN/m
B A L
7.92 7.92 12.0
7.80 7.80 12.0
7.19 7.19 12.0
m 2 m m
bc sc ic R/A V d /A R / V d
1.00 1.13 0.91 543 143 3.79
1.00 1.13 0.86 509 195 2.62
1.00 1.12 0.77 328 159 2.06
181
Not critical (see Table 7)
163
Table 6. Bearing Resistance – undrained foundation
3
2
kN/m
2
kN/m 2 kN/m
2
kN/m
2
kN/m
T Christie, M Glendinning, J Bennetts, S Denton12
Bearing Resistance – drained foundation
SLS
STR/GEO Comb. Comb. 1 2
Effective foundation dimensions B from Table 6
B
7.92
7.80
7.19
m
L from Table 6
L
12.0
12.0
12.0
m
A per metre width from Table 6 Other geometry, partial factors, foundation properties and actions are as Table 6
A
7.92
7.80
7.19
m
N q
13.2
13.2
7.96
N c
23.9
23.9
17.1
N
12.4
12.4
5.68
bc
1.00
1.00
1.00
bq , b
1.00
1.00
1.00
sq
1.30
1.29
1.23
2
Bearing parameters for drained foundations tand
N q = e
2
tan (45+ d /2)
N c = ( N q-1)cot d /2 (rough N = 2 ( N q-1) tan , where base) bc = bq – (1-bq)/ N c tan d bq = b = (1 - tan d ) sq = 1 + ( B / L ) sin d , for a rectangular shape s = 1 – 0.3 ( B / L ), for a rectangular shape; sc = (sq N q – 1)/( N q – 1) for rectangular, square or circular shape
s
0.80
0.81
0.82
sc
1.32
1.32
1.26
m = (2+ B / L )/(1+ B / L )
m
1.60
1.61
1.63
iq
0.67
0.62
0.54
ic
0.64
0.59
0.47
i
0.52
0.47
0.36
cd N c bc sc ic
0.00
0.00
0.00
qd N q bq sq iq
137
128
62.7
0.5 d B N b s i
367
311
110
R/A
504
439
172
kN/m
V d /A
143
195
159
kN/m
R / V d
3.52
2.25
1.08
iq = [1 – H /(V + A c d cot d )]
m
ic = iq – (1 – iq)/ N c tan d i = [1 – H /(V + A c dcot d)]
m+1
R/A = (Equation from BS EN 1997-1 D.4)
R / A = sum of above V d / A Ratio R/V
2
Resistance to limit settlement at SLS 2
1/3 ( R/A) at SLS characteristic
168
Limits
kN/m
B Max toe pressure (1+6e/B) V d /
163
satisfied
kN/m
Table 7. Bearing Resistance – drained foundation
2
T Christie, M Glendinning, J Bennetts, S Denton13
Final Design After the preliminary design has been completed a final design should be carried out as given below: 1. Select the final dimensions based on the preliminary values: Bheel = 6.25m and B = 8.6m. As the weight on the toe has not been included in the preliminary design, Bheel has been "rounded down" and the overall length (B) may need to be "rounded up". 2. The final selected base slab dimensions should be verified using the correct concrete densities, the loads on the toe and other relevant combinations of actions. Details of the final design calculations are not included in this paper.
Conclusions It is difficult to generalise about which combination of actions or which limit states are critical on the basis of calculations for a single bridge because the critical combination is often determined by the ratio of the bridge span to the abutment height or the ratio of traffic action to the soil actions . It is however clear that horizontal earth pressures are generally critical for STR/GEO Combination 1 regardless of the bridge proportions because G for soil is higher than K a;d / Ka ;k for most realistic values of ' . Also, for undrained sliding resistance Combination 2 is always likely to be critical because M on cu is higher than K a;d / Ka ;k for all realistic values of ' , and it is also higher than Q on surcharge braking and acceleration. For drained sliding resistance, in the calculations presented in this paper, Combination 2 was more critical than Combination 1, primarily because the effects of G on the weight of soil were favourable for sliding resistance and unfavourable for horizontal pressure and therefore, to some extent, cancelled each other out in Combination 1. It was however apparent from the calculations that Combination 1 could be critical for sliding for low abutments supporting long spans where braking and acceleration actions were large and earth pressures were small. For bearing pressure, Combination 2 was found to be significantly more critical than Combination 1 for both drained and undrained foundations and as M effects tend to predominate in bearing resistance calculations it seems probable that Combination 2 will be critical for bearing resistance in most typical abutments and retaining walls. It was also apparent from supporting calculations that the limitation on toe pressure at SLS is quite severe and that in many cases where it is required to be applied, it will dictate the length of the base. Additional explicit settlement calculations may therefore result in shorter base lengths being required. Overturning was not found to be an issue for the abutment illustrated in this paper and although it needs to be verified, it appears that it is unlikely to affect the proportions of typical gravity abutments as bearing failure under the toe would normally precede overturning.
T Christie, M Glendinning, J Bennetts, S Denton14
References [1] [2] [3]
[4] [5] [6]
PD 6694-1 Recommendations for the design of structures subject to traffic loading to BS EN 1997-1: 2004, BSi, London, UK BS EN 1990:2002+A1:2005 Eurocode - Basis of structural design Incorporating corrigenda December 2008 and April 2010 , BSi, London, UK BS EN 1991-2:2003 Eurocode 1: Actions on structures – Part 2: Traffic loads on bridges, Incorporating Corrigenda December 2004 and February 2010 , BSi, London, UK BS EN 1997-1:2004 Eurocode 7: Geotechnical design – Part 1: General rules, Incorporating corrigendum February 2009 , BSi, London, UK NA to BS EN 1990:2002+A1:2005 UK National Annex for Eurocode – Basis of structural design, Incorporating National Amendment No.1 , BSi, London, UK NA to BS EN 1991-2:2003 UK National Annex to Eurocode 1: Actions on structures – Part 2: Traffic loads on bridges, Incorporating Corrigendum No. 1 , BSi, London, UK
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