Arches One Part Three
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advantage of the arch over the beam is that the ground is used to oppose
the outward thrust. Near the abutments the ground is in
compression, but under the arch it is in tension. Within a beam
there are both compressive and tensile stresses, and of course shear
stresses and bending moments. The arch avoids these, at least for
the dead load. So it can be made lighter than a beam of the same
span.
Therefore the longest arch is longer than the longest beam (Long spans). The beam does have three advantages; it can carry the deck directly, in principle it can be built as a whole and moved into position, and in a multiple span bridge the beams can be joined, and even stressed together to optimise bending moments. The idea of moving the whole span is possible in the case of a tied arch. An example is given later in this page. The Romans built semicircular arches with very thick piers, so that any arch would remain standing if its neighbour was removed by flood or by enemy action. The thrust was meant to remain entirely within the piers. The Romans were not interested in record-breaking spans, only in utility and durability. That some of their bridges remain after about 2000 years of continuous scouring, in rivers which are subject to frequent heavy flooding, says it all. Military action has removed many that would otherwise have survived. The diagram below, a vertical section, suggests the way that the ground transmits the tension below a two-pinned arch. It is not an exact calculation, only a rough sketch, and the lines would be distorted by variations in the ground. The actual force-field is continuous, and not really along narrow lines. Compare this with the stresses shown in the page on beams, and with Brunel’s Saltash bridge spans. These tensions in the ground are normally unimportant, because they are diffused over a large area. What matters is the stress, or force per unit area, which is large only at the abutments, where the compressive stress is largest. arch bridges 27 |
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In fact, in every type of bridge, except arches and suspension bridges, and beams with sloping struts, the horizontal forces are kept out of the ground, and carried in members that oppose the forces in the rest of the bridge. In those bridges, the forces on the ground are purely vertical. The lines of force are spread sideways and vertically, as if they repel each other. Why do the lines of force not simply run straight along under the bridge? The energy density at a place is proportional to the square of the stress, for elastic material. Therefore the minimum energy state is found when the stress field is diffuse. Halving the stress at a place divides the energy density by four. The distribution is the one that minimises the total energy. Spreading it or shrinking it would increase the strain energy. These diagrams are not unlike the fields around a bar magnet or a pair of electric charges. The stresses near the abutments are more complicated, because the arch induces compressions, which are present along with the tensions already described. These diagrams make clear that the structure includes not only the visible part, but any part of any other object that is subject to significant stresses. Stresses in the ground are perhaps most important in the construction of dams, where not only the dam, but a vast mass of water, creates great pressure on and in the ground, together with lubrication in cracks. See arch dams and gravity dams. The diagrams below are outlines of some bridge types. Compare these with the previous diagrams. arch bridges 29 |
Propped beams become Maillart arch
The next diagram develops one of the shapes seen in an earlier diagram..
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the bottom two beams are propped together. Because, together with
the ground, the system forms a triangle, the beams can be hinged at all
three joints. As explained in the page about beams, the variation
of bending moment suggests that beams should be deeper in the middle, as
in the next diagram up. Above that, a deck has been added, and in
the top diagram it has been integrated into the arch. The beam
would of course be supported at the ends. And so we see that an
arch is not entirely unrelated to a beam.
The diagram at the top is an ugly version of a type of bridge that was beautifully designed by Maillart, and used many times since, though not always with the artistry that he possessed. Actually, Maillart arrived at his designs by a different line of thinking, starting from a normal arch, but the result was about the same. And here are some more ideas. In practice, the depth would probably be varied along the span to take advantage of the arch action when the supports are sloping inwards. Note how the deck is in compression when the struts are sloping. arch bridges 30 |
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In the structures above, there are straight struts and curved struts. Which are correct? If the struts are much lighter than the deck, they should be nearly straight, but if they are much heavier than the deck, they should be curved. Why? Some of the structures on the right resemble a gothic arch, and in fact they represent the true use of this shape. In gothic buildings, the point of the arch seldom corresponds to a load. The same is true of Sydney opera house. An essential result of building an arch is that there will be an outward thrust at each end. This has to be resisted by the abutments. If you don’t believe this, try standing with one foot in a small boat and one foot on the river-bank, or better still, with your hands on the bank and your feet in the boat. You will very soon be in the water. Standing with your legs wide apart on ice will have a similar effect. The two pictures below show Telford’s bridge at Over, near Gloucester, which was completed in 1829. When the centring was removed, the crown sank about ten inches, because the thrust was not properly resisted, but the bridge was used until 1974, when a steel bridge was built nearby, to carry a much wider road, the A40. The only way to avoid the thrust reaching the abutments is to tie the ends of the arch together, using the deck or some cables. This creates a tied arch, or bow-string arch. If the arch design is chosen to provide a passage for ships or traffic underneath then the tie method may not be acceptable, unless the whole thing can be built high enough. Then the road is very high, which creates problems with the approaches, unless the arch spans a deep narrow valley. But in such a case, the rocky sides will probably take the thrust in any case. arch bridges 31 |
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drawings were made by hand. This is not the way to do it for
accurate results. The drawing below was made and drawn by computer
calculation, for a simple deck-stiffened arch.
The horizontal component of the thrust (pale blue) is the same throughout the arch. It must be so, because the spandrel walls exert only vertical forces. The vertical component (green) increases towards the abutment as it is the sum of all the weight from the centre to a given point. The total force (red) of course acts along the arch. |
| In the next picture the height of the structure has been reduced by a half. Look at the effect on the horizontal component of the thrust. |
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the next diagram we see a crude three pin arch.
If the weight of the load is vastly greater than the weight of the arch, the graph represents the horizontal thrust as a function of the slope angle A. As A approaches zero, at the left, the thrust tends to infinity. So an arch cannot have zero rise. What about a beam? A beam is not an arch – it does not have a hinge. The beam is rigid, and in the page about Beams, we see that a solid beam contains within it both an arch and a suspension cable. When you see a mathematical function, it is a good idea to ask what happens for all possible inputs. The next graph includes negative angles as well as positive ones. Negative angles produce negative thrust: the structure is a crude suspension span. The jump from plus infinity to minus infinity would not happen in practice. No structure or supports could provide infinite force. What would happen is that at some very small angle, the compression produced by the thrust would be enough to let the arch fall through the gap and become a string. If we keep the angle just above the critical point, the structure has two stable states, and we can cause a transition to the other state by adding a small extra force. Many latches work on this over-ride principle. Some electronic circuits are based on monostable or bistable systems. The lavatory cistern is a monostable system. If you operate it, the water pours out, leaving the cistern in an unstable temporary state. The water flows in, and eventually stability is reached when the valve stops the flow. The filling takes a considerable time, and in fact monostables are often used to generate timing periods in electronic systems. But for great precision, crystal clocks are more often used. arch bridges 35 |
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Links about Robert Maillart and other pages about arches |
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Tavanasa bridge – pictures Salginatobel – Schwandbach Bridges of Paris |
Book in German Photographs Scientific American – July 2000 Niagara Falls bridges Back to Home Page Back to Bridges |
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