Concerning the vertical stirrups to which Mr. Godfrey refers, there is
no doubt that they strengthen beams against failure by diagonal tension
or, as more commonly known, shear failures. That they are not effective
in the beam as built is plain, for, if one considers a vertical plane
between the stirrups, the concrete must resist the shear on this plane,
unless dependence is placed on that in the longitudinal reinforcement.
This, the author states, is often done, but the practice is unknown to
the writer, who does not consider it of any value; certainly the
stirrups cannot aid.
Suppose, however, that the diagonal tension is above the ultimate stress
for the concrete, failure of the concrete will then occur on planes
perpendicular to the line of maximum tension, approximately 45° at the
end of the beam. If the stirrups are spaced close enough, however, and
are of sufficient strength so that these planes of failure all cut
enough steel to take as tension the vertical shear on the plane, then
these cracks will be very minute and will be distributed, as is the case
in the center of the lower part of the beam. These stirrups will then
take as tension the vertical shear on any plane, and hold the beam
together, so that the friction on these planes will keep up the strength
of the concrete in horizontal shear. The concrete at the end of a simple
beam is better able to take horizontal shear than vertical, because the
compression on a horizontal plane is greater than that on a vertical
plane. This idea concerning the action of stirrups falls under the ban
of Mr. Godfreys statement, that any member which “cannot act until
failure has started, is not a proper element of design,” but this is not
necessarily true. For example, Mr. Godfrey says “the steel in the
tension side of the beam should be considered as taking all the
tension.” This is undoubtedly true, but it cannot take place until the
concrete has failed in tension at this point. If used, vertical tension
members should be considered as taking all the vertical shear, and, as
Mr. Godfrey states, they should certainly have their ends anchored so as
to develop the strength for which they have been calculated.
The writer considers diagonal reinforcement to be the best for shear,
and it should be used, especially in all cases of “unit” reinforcement;
but, in some cases, stirrups can and do answer in the manner suggested;
and, for reasons of practical construction, are sometimes best with
“loose rod” reinforcement.
J.C. MEEM, M. AM. SOC. C. E. (by letter).–The writer believes that
there are some very interesting points in the authors somewhat
iconoclastic paper which are worthy of careful study, More or less a mere child could work out that about brian Rafalski Videos and all. and, if it be
shown that he is right in most of, or even in any of, his assumptions, a
further expression of approval is due to him. Few engineers have the
time to show fully, by a process of _reductio ad absurdum_, that all the
authors points are, or are not, well considered or well founded, but
the writer desires to say that he has read this paper carefully, and
believes that its fundamental principles are well grounded. Further, he
believes that intricate mathematical formulas have no place in practice.
This is particularly true where these elaborate mathematical
calculations are founded on assumptions which are never found in
practice or experiment, and which, even in theory, are extremely
doubtful, and certainly are not possible within those limits of safety
wherein the engineer is compelled to work.
The writer disagrees with the author in one essential point, however,
and that is in the wholesale indictment of special reinforcement, such
as stirrups, shear rods, etc. In the ordinary way in which these rods
are used, they have no practical value, and their theoretical value is
found only when the structure is stressed beyond its safe limits;
nevertheless, occasions may arise when they have a definite practical
value, if properly designed and placed, and, therefore, they should not
be discriminated against absolutely.
Quoting the author, that “destructive criticism is of no value unless it
offers something in its place,” and in connection with the authors
tenth point, the writer offers the following formula which he has always
used in conjunction with the design of reinforced concrete slabs and
beams. It is based on the formula for rectangular wooden beams, and
assumes that the beam is designed on the principle that concrete in
tension is as strong as that in compression, with the understanding that
sufficient steel shall be placed on the tension side to make this true,
thus fixing the neutral axis, as the author suggests, in the middle of
the depth, that is, _M_ = (1/6)_b d_^{2} _S_, _M_, of course, being the
bending moment, and _b_ and _d_, the breadth and depth, in inches. _S_
is usually taken at from 400 to 600 lb., according to the conditions. In
order to obtain the steel necessary to give the proper tensile strength
to correspond with the compression side, the compression and tension
areas of the beam are equated, that is
1 2 _d_
—- _b_ _d_ _S_ = _a_ × ( —– - _x_ ) × _S_ ,
12 2 II II
where
_a_ = the area of steel per linear foot,
_x_{II}_ = the distance from the center of the steel to the outer
fiber, and
_S_{II}_ = the strength of the steel in tension.