The destruction of the Wheeling bridge by a high wind on the 17th of May last year, the greatest disaster of the kind on record, has naturally given rise to doubts as to the safety of suspension bridges generally. One of the scientific journals remarked at the time, that the failure of this bridge would appear to be conclusive evidence against the practicability of large spans. Although I would much prefer to leave this subject alone, I cannot conscientiously do so. It is my duty to establish the safety of the Niagara Bridge, which has already, and in the brief space of one month, become one of the greatest thoroughfares on this continent. I cannot do so without drawing a comparison with other works, and without pointing out the defects which caused the destruction of the Wheeling bridge, and on the other hand explaining the means of safety which have been employed in the Niagara Bridge.
The Wheeling bridge formed a span of
1010 feet from centre to centre of towers; the floor was 960 feet
long, and 26 feet wide outside of railings, its weight, including
cables, was about 440 tons. The number of cables was 12, containing
in all 6600 wires of No. 10. With the exception of two small stays
under the floor at each tower, which appeared to be put up after
the completion of the work, and were in a loose and ineffective
condition at the time I examined it, there was no provision in
the whole structure, aside from the inherent stiffness of the
floor, which could have had an effect in checking vibrations.
Owing to the provisions made for resting the cables on the towers
by means of large rollers, and to the wire being arranged in a
number of small cables in place of one large one, is to be attributed
the fact of the ready communication of vibratory motion from the
suspension cables to the land cables. The motion caused by the
transit of a single team was readily communicated to the land
cables. In consequence of this sensitiveness the great force to
which the suspension cables were subjected on the 17th of May,
was fully transferred to their connection with the anchor chains:
the result was their failure on the Wheeling side. A competent
eyewitness stated, that the waves of the floor, caused by the
wind, rose to a height of over 20 feet. This may have been an
exaggeration, but no ordinary strength of cables can resist the
momentum produced by such a weight falling even 15 feet. The destruction
of that bridge was clearly owing to a want of stability, and not
to a want of strength. This want of stiffness could have been
supplied by over-floor stays, truss railings, under-floor stays,
or cable stays. If by these means no high degree of sufficient
could have been obtained, they would at any rate have proved quite
sufficient to check oscillations, and to keep them within safe
limits. In the Niagara Bridge most ample provisions for stability
have been made. The superstructure, forming a hollow box or beam,
of 24 feet wide by 20 feet deep, with solid girders of five feet
depth, and effective trusses, possesses enough of stiffness to
resist the action of any gale. To be prepared, however, for the
greatest emergency, there are 56 wire rope stays or guys attached
to the lower floor, which are firmly anchored either to the solid
rock of the cliffs, or to large masses of detached rock. Each
of these ropes has an ultimate strength of 30 tons, they would
therefore resist with an aggregate force of 1680 tons. But, owing
to their inclinations, they would probably not oppose a greater
resistance than 1000 tons, if that pressure was vertically applied
against the lower floor. The ordinary tension of these stays does
not exceed from two to three tons.
| Now the weight of the bridge without the cables and stays is. | 600 tons. |
| To this add the anchorage at each end of the lower floor, which is estimated at . . . . . . . . . | 300 " |
| Resistance of cables in centre . . . . . . . | 100 " |
| Resistance of stays is . . . . . . . . . | 1000 " |
| Total . . . . . . . . . . . . . | 2000 tons. |
Let us suppose a hurricane expending
its power upon the whole extent of both floors, and at the rate
of 50 lbs. per superficial foot uplifting force.
| The surface of the upper floor is . . . . | 20,000 feet. |
| The surface of the lower floor is . . . . | 18,000 feet. |
| Total . . . . . . . . . . | 38,000 feet. |
| Pressure at 50 lbs . . . . . . . | 1,900,000 lbs. |
| Or . . . . . . . . . . . | 950 tons. |
to which a resistance is opposed of 2000 tons. No tornado, however, will act with equal force upon both floors at the same time, nor uniformly throughout their whole extent. Before the two floors were connected I noticed, that while the lower one was sensibly affected by a gale the upper one showed no motion at all, its force appeared to be expended below. Owing to the bend of the river the Canada shore is well protected, while the opposite side is exposed from all quarters. Not the slightest motion from high winds was ever noticed since the two floors were connected. The work has been frequently tested by the strongest gales that blow in this vicinity. I am also convinced that it will be proof against a hurricane.
The tornado which recently made such
havoc at the town of Niagara, and was also severely felt at Lockport
and Rochester, did not expend its full force upon the bridge.
Its vortex was either too much elevated, or too far north east.
Only a severe momentary shock, accompanied by great darkness was
experienced, and lasted but a few seconds. This shock did not
produce the slightest perceptible motion. Tornadoes are believed
to be whirlwinds on a large scale, produced by the struggle of
two u7inds moving in opposite directions in the upper regions
of the air. Impelled in the directions of the strongest wind,
the two contending forces move on within the sphere of a double
cone, the most violent action being at the union of the two bases.
This view being correct, the Niagara Bridge can never experience
the full force of a hurricane. The towers may come within the
sphere of its action, but not the bridge itself; certainly not
enough to experience a great uplifting force.