ultimate strength of reinforced concrete in american design practice
TRANSCRIPT
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PORTLAND CEMENT ASSOCIATION
RESEARCH AND DEVELOPMENT LABORATORIES
ULTIMATE STRENGTH OF
REINFORCED
CONCRETE IN
AMERICAN DESIGN PRACTICE
By Eivind Hognestad
Authorized Reprint From
Proceedings of a Symposium on the Strength of
Concrete Structures, London, May, 1956
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Bulletins Published by the
Development Department
Research and Development Division
d the
Portland Cement Association
D1
—“Influence of Soil Volume Change and Vegetation on Highway Engf.
neering,”
by E, J.
FELT.
Reprinted from Twent Sixth Annuat Highuxw Conference of the Universit?j
of Coiorado, May 12S2.
D2 -“Nature of Bond in Pre-Tensioned Prestressed Concrete,”
by
JACK R.
J ANNEY,
Reprinted from JournfIl of the American Concrete Institute (May, 1954);
proceedings, 30, 717 (12S4).
D2A—Discussion of the papw “Nature of Bond in Pre-Tensioned Prestressed
Concrete,”
by P. W.
ABELES, K. HAJNAL-KONYI, N. W. HANSON
and
Author, JACK R. JANNEY.
Reprinted from Journal of the American Concrete Institute (December,
Part 2, 1954): Proceedings, SO, 73S-1 (1254).
D3
_f ~Investigationof M~isture.Vo]ume Stability of Concrete Masonry
Units,” by
JOSEPH
J. SRJDELER,March, 1955.
D4
—“A Method for Determining the Moisture Condition of Hardened Con-
crete in Terms of Relative Humidity,”
by
CARL A. MENZEL.
~le ~ted froml Proceedings, American Soctetv For Testing M@tU’iaiS, 55
D5 —“Factors Influencing Physical Properties of Soil-Cement Mixtures,”
by EARL J.
FELT.
Reprinted from~ Bulletin 108 of the IIigfwav Research Board, p.
123 19S5).
D6 -“Concrete Stress Distribution in Ultimate Strength Design,” by E.
HOONESTAO, N. W. HANSON and D. MCHENRY.
Reprinted from JonrnaI of the American Concrete Institute (December,
1955); Proceedings, 52, 455 (19S6).
D?
-“Ultimate Flexural Strength of Prestressed and Conventionally
Rein-
forced Concrete Beams,” by J. It. JANNEY, E. HOONESTAD and D. Mc-
HENRY.
Reprinted from Journal of the American Concrete Institite (FebruaxT, 19S0;
Proceedings, S2, S01 (12SS).
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SYMPOSIUM ON THE STRENGTH OF CONCRETE STRUCTURES
LONDON MAY 1956
Sessicm E: Paper 1
ULTIMATE STRENGTH OF
REIN FORCE(D CONCRETE IN
AMERICAN IDESIGN PRACTICE
by Eivind Hognestad,
Dr. techn.
Portland Cement Association, U.S.A.
SUMJ4AR Y
Ultimate strength design procedures for reinforced concrete were recom-
mended in an October 1955 report of a joint committee of the American
Society of Civil Engineers and the American Concrete Institute. This paper
discusses the background for and contents of that report, which represents
a signj?cant stage in the development of an American design practice based
on ultimate strength by inelastic action.
Introduction
The past fifty years have been a period of rapid growth and develop-
ment in the use of reinforced concrete as a structural material throughout
the world. The production of Portland cement in the United States rose
twenty-five fold from about 2 million long tons in 1900 to over 50 million
tons in 1955. Similarly, the U.S. production of reinforcing stee[ increased
from a small amount to about 1”8 million tons.
Introduction of new design procedures for reinforced concrete must be
considered with this background of great progress and expansion. Though
the classical straight-line theor:y was evolved when reinforced concrete was
in its infancy some 60 years ago, it has served us well; and it certainly
cannot be put aside on the basis that it has led to unreasonable or unsafe
designs.
On the other hand, through half a century of practical experience and
laboratory experimentation, our knowledge regarding the strength and
behaviour of structural concrete has been vastly improved. To some extent,
such improvements of knowledge have been utilized in design practice by
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periodic adjustments and modifications of the straight-line theory. In this
manner the original sitnplicity of an elastic theory based on a few funda-
mental assumptions has largely been lost.
It is primarily to facilitate further progress, therefore, that many of us
feel that the time has come to introduce a new theory of reinforced con-
crete design based on the actual inelastic properties of concrete and steel.
Such a new theory is needed to realize the full future benefits of such
highly important developments in the field of structural concrete as high-
strength reinforcement,, prestressing, and precasting.
DEFINITIONS
In recent years good progress has been made in the development of
knowledge regarding the properties of all engineering materials. New and
improved concepts of structural behaviour and design have therefore
become significant in the practice of civil engineering. These concepts are
identified by rather reeent additions to engineering terminology such as
rheology, plasticity, inelastic behaviour, plastic analysis, limit strength,
and many others. Definitions for these terms vary to some extent between
countries as well as between groups concerned with the various materials.
It is necessary, therefore, to define common American word usage in
connexion with structural concrete design.
Ultimate strenglh design
Ultimate strength design indicates a method of structural design based
on the ultimate strength by inelastic action of conventionally reinforced or
prestressed structural concrete cross-sections subject to simple bending,
axial load, shear, bond., or combinations thereof. Ultima~e strength design
does not necessarily involve an inelastic theory of structures. Evaluation
of external moments and forces that act in indeterminate structural frame-
works by virtue of dead and live loads may be carried out either by the
theory of elastic displacements or by limit design.
Limit design
Limit design indicates a design method involving an inelastic theory of
structures in which readjustments in the relative magnitude of bending
moments at various sections due to non-linear relationships between loads
and moments at high loads are recognized. Limit design does not by
definition necessarily involve a final design of sections on an inelastic
basis.
Yield line theory
Yield line theory indicates a theory of reinforced concrete slab structures
based on inelastic behaviour occurring in a pattern of yield lines, the
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location of which depends on loading and boundary conditions. Final
design of sections does not necessarily involve inelastic action.
So far, most American work regarding inelastic behaviour of structural
concrete has been devoted to ultimate strength design. A term indicating
,a combination of ultimate strength design, limit design and yield line
theory therefore still remains tc}be adopted. Perhaps the most important
aspect of ultimate strength design is that it represents a significant step
toward a broader consideration of inelastic behaviour in design.
AMERICAN DESIGN SPECIFICATIONS
Two groups have made important contributions to the development of
reinforced concrete design specifications in the United States—the Joint
(Committees on Standard Specifications for Concrete and Reinforced
Concrete, and committees of the American Concrete Institute(1).
The Joint Committees have consisted of delegates from the American
Concrete Institute (ACI), American Institute of Architects (AIA),
American Railway Engineering Association (AREA), American Society
of Civil Engineers (ASCE), American Society for Testing Materials
(ASTM), and the Portland Cement Association (PCA). The first, second
and third Joint Committees were organized in 1904, 1919 and 1930, and
submitted final reports in 1916, 1924 and 1940 respectively. These reports,
which were milestones on the road of progress and had a strong effect
on American concrete usage, were submitted to the constituent organiza-
tions. The sections concerning reinforced concrete design were written in
the form of a recommended practice rather than a design code, so that it
was possible to give a broad reflection of the state of the art as represented
by the best practice of the day.
The first committee on reinforced concrete of the ACI, then the
National Association of Cement Users (NACU), was the Committee on
Laws and Ordinances. The first report of this committee appeared in 1909
and was essentially based on what has later become known as ultimate
strength design. The report was later revised to introduce the concepts of
the straight-line theory, allowable stresses, and service loads; and it was
then adopted as “ Standard Building Regulations for Reinforced Con-
crete “ in 1910. Later a Committee on Reinforced Concrete and Building
Laws was formed, sponsoring ‘
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numerous cities and municipalities throughout the United States. Many
agencies of the U.S. Government also refer to the ACJ Code, though
minor adjustments are often made to suit their particular needs.
In the field of bridge design and construction, specifications have been
developed and periodically revised by the American Association of State
Highway Officials and by the Ameriean Railway Engineering Association.
NOTATION
The letter symbols used are generally defined where they are first
introduced; they are also listed below for convenient reference.
Loads and load factors
B = effect of basic load consisting of dead load plus volume change
due to elastic and inelastic actions, shrinkage and temperature
E =
effect of earthquake forces
Fb
= ultimate strength for balanced condition given by equation (I 5)
FO =
ultimate strength of concentrically loaded column given by
equation (12)
FU =
ultimate strength of eccentrically loaded member
Fu’ =
maximum axial load on long member given by equation (21)
K = load factor equal to 2.0 for columns and members subject to
combined bending and axial load, and equal to 1”8 for beams
and girders subject to bending
L = effect of live load plus impact
MU = ultimate resisting moment
U =
ultimate strength capacity of section
W =
effect of wind load
Cross-sectional properties
AC =
A, ==
A,C =
A,f =
A,, =
b=
b, =
;=
D, =
d, =
gross area of concrete section
total area of IIongitudinal reinforcement
area of compressive reinfcwcement
steel area to develop compressive strength of overhanging flange
in T beams, defined by equation (11)
area of tensile reinforcement
width of a rectangular section, or overall width of flange in
T beams
width of web in T beams
n.dl = depth to neutral axis
total diameter of circular section
diameter of circle circumscribing the longitudinal reinforcement
in circular section
effective depth to centroid of tensile reinforcement
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d, =
effective depth to centroid of compressive reinforcement
e= eccentricity of axial load measured from the centroid of tensile
reinforcement
e’ = eccentricity of axial load measured from plastic centroid of
section
e~’ = eccentricity of loacl
Fb
measured from plastic centroid of section
L =
unsupported Iengtlh of an axially loaded member
nudl =
depth to neutral axis at ultimate strength
A,,
r
=
ratio of tensile reinforcement .= —
bdl
rb =-
ratio of balanced tensile reinforcement defined by equation (6)
A
r’ =
ratio of compressive reinforcement = ~
bd,
A,,
rt =
ratio of total reinforcement = —
AC
t
rW =—
b’d,
t
= flange thickness in T section, or total depth of
section
Properties of’materials
ECU =
=W =
f=
U
f
Y ‘“
k, =
k, =
mu =
mu’ =
maximum strain in concrete at ultimate strength
0“003)
strain in tensile reinforcement at ultimate strength
stress in tensile reinforcement at ultimate strength
:ctangular
limited to
yield point stress of reinforcement (limited to 60,000 lb/in2)
ratio of average compressive stress to 0.85
u.+,
at ultimate
strength
ratio of depth to resultant of compressive stress and depth to
neutral axis at ultimate strength
0“85
U y
mu—l
=
cfy
a—
ucy/
U.yl =
compressive strength of 6
x
12 in. cylinders at 28 days
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Report of ASCE-ACI Joint Committee
on Ultimate Strength Design
Advancement in the field of structural design and analysis must of
necessity proceed with extreme caution and deliberation. This has been
true of the recommendations in the report of the ASCE-ACI Joint
Committee on Ultimate Strength Design which culminates over ten years
of continuous study of the subject. The joint committee was formed as a
sub-committee of the ASCE Committee on Masonry and Reinforced
Concrete under the chairmanship of the late A, J. Boase in 1944. It
immediately commenced a comprehensive study of the adequacy of various
ultimate strength theories and design formulae. As a result of its studies,
it initiated extensive series of both short-time and sustained load tests on
eccentrically loaded columns. These tests have been completed under the
sponsorship of the Reinforced Concrete Research Council of the
Engineering Foundation.
In 1949 L. H. Corning was made chairman of the sub-committee. At
this time, the sub-committee further recommended an extensive test pro-
gramme on the shear resistance of reinforced concrete members. Extensions
of this investigation are still in progress. In 1952 the sub-committee was
made a joint committee o:f AC1 and ASCE and designated as Committee
327 by ACI.
Hand in hand with the :studies made on ultimate strength formulae, the
joint committee has investigated the question of overload factors in terms
of the practice prevailing in countries where design by ultimate strength is
in practical use, and of the factors of safety implied in conventional
straight-line design methods.
During the annual convention of ACI in 1952, the joint committee
sponsored a symposium on ultimate strength design(3). This provided an
opportunity for public discussion of such topics as reasons for changing
design method, fundamental concepts of ultimate strength design, review
of research, practical design, and overload factors.
In 1955 the committee completed its assignment “ to evaluate and
correlate theories and data bearing on ultimate strength design procedures
with a view to establishing them as accepted practice “. A final report was
submitted to ASCE and AC1 4’5). It is the principal purpose of this paper
to discuss the contents of that report, and to present the author’s opinions
and interpretations regard ing the report.
NATURE OF THE REPO RT
The joint committee report presents recommendations and formulae for
ultimate strength design (of reinforced. concrete structures together with
basic supporting and explanatory data. The report is confined to design
of cross-sections; it does not deal with evaluation of external moments
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and forces. The committee recognized limit design as important but did
not recommend practical use thereof at the present time.
The report is based on the assumption, therefore, that structural analysis
will be carried out by the theory of elastic displacements. On the basis of
this assumption stresses will remain within the elastic limits under service
loads when proper load factors are used. For statically determinate mem-
bers, the ultimate capacity equals the computed capacity. For indeter-
minate structures, it is important to note that the maximum moments at
various sections are usually due to different load arrangements. Because
of moment redistribution at high loads, therefore, the maximum load
capacity of the indetermini~te structure may considerably exceed that
indicated by the capacity at a single section. Accordingly, a combination
of ultimate strength design of sections and elastic structural analysis may
be conservative in some cases, but it is not at all unreasonable.
The joint committee report as published by ASCE(4) consists of a brief
section on historical background, and the essence of the report appears
under the heading “ Recommendations for design “ Three appendixes
deal with substantiating test data, design aids, and derivation of formulae.
The report ends with a selected bibliography. The AC I publication (sJ
does not contain the appendixes concerning test data and derivation of
formulae.
LOAD FACTORS
Consideration was given by the joint committee to the circumstance
that ultimate strength design may be carried out in two ways. Moments
and forces acting at various sections may be evaluated for service loads,
Sections may then be designed by “ deducted “ or “ allowable “ ultimate
strength equations, in which chosen safety factors are incorporated.
Another alternative is LOmultiply the, service loads by chosen load factors
before the cross-section forces are evaluated. The design of sections then
takes place by equations expressing actual ultimate strengths.
The joint committee chose to follow the second alternative, principally
because ultimate strength equations are essentially factual in nature, while
the choice of load factors to a considerable extent is a matter of engineering
judgment. By keeping load factors and strength equations separated, the
report should be conveniently useful even to specification-writing bodies
that find it necessary for special applications to change the numerical
values of the load factors recommended by the joint committee. Further-
more, it is believed to be wise for a designer clearly and unmistakably to
keep his load factors in view.
Two criteria were consic[ered as a basis for selecting load factors.
Members should be proport.ioned so that: (l) they should be capable of
carrying service loads with ,ample safety against an increase in live load
beyond that assumed in design and against other uncertainties; (2) the
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strains under service loacls should not be so large as to cause excessive
cracking. The committee found that these criteria are satisfied by the
following formulae.
(1) For structures in the design of which effects of wind and earthquake
forces can properly be neglected:
U=I”2B+2.4L . . . . . . . . . . . . . . . . . . . . . . . ...(1)
and
U= K(B -I- L), . . . . . . . . . . . . . . . . . . . . . . . . ...(2)
in which
U= ultimate strength capacity of section
B ==effect of basic loald consisting of dead load plus volume changes
dueto elastic and inelastic actions, shrinkage, and temperature
L = effect ofliveload plus impact
K = load factor equal to 2“0 for columns and members subject to
combined bending and axial load, and equal to 1”8 for beams and
girders subject to bending
(2) For those structures in which wind loading should be considered:
U~l”2B+ 2”4L+O”6W . . . . . . . . . . . . . . . . ..(la)
U=1”2B+ 0.6L+2”4W . . . . . . . . . . . . .
. . . ..(lb)
and
)
=K B+ I +; . . . . . . . . . . . . . . . . . . . .
)
==K B+:C+W . . . . . . . . . . . . . . . . . . . .
(2a)
(2b)
(3) Forstructures inthe design of which earthquake Ioading must be
considered, substitute for the effect of wind load, W, the effect of earth-
quake forces, E.
GENERAL REQUIREMENTS
The joint committee report does not deal with the many detailed require-
ments involved in reinforced concrete design and construction, such as
spacing and cover of reinforcement, and special considerations regarding
the various typical bui[ding elements. A reference is therefore made to
the ACI Building Code in all matters not otherwise provided for in the
committee report.
It is required” that bending moments should be taken into account in
calculating the ultimate strength of compression members. Analysis of
indeterminate structures should be carried out by the theory of elastic
displacements, though approximate coefficients such as those recom-
mended in the ACI code are acceptable for the usual types of buildings
In structures such as arches, the effect of shortening of the arch axis,
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temperature, shrinkage, and secondary moments due to deflexion should
be considered.
The committee report also calls attention to the need for checking
deflexion of members including effects of creep, especially for high
percentages of reinforcement.
In considering the recommended ultimate strength equations, it is im-
portant to note that the committee assumed that only controlled concrete
will be used in construction of structures designed by ultimate strength.
The quality of concrete should then be such that not more than one test
in ten has an average compressive strength less than the strength assumed
in design, and the average of any three consecutive tests should not be
less than the assumed design strength. In this manner, the design concrete
strength is not an average strength; with a reasonable probability it is a
minimum strength. Similarly, through the general reference to the AC1
code, the joint committee assumed that design values for the yield point
of reinforcing steel are minimum values. Accordingly, the ultimate strength
design equations should express an average and not a minimum relation-
ship between ultimate strengths of the various reinforced concrete members
as observed in tests and the cclrresponding compressive strengths.
BASIC ASSUMPTIONS FOR IJLTIMATE STRENGTH
After a thorough study of many ultimate strength theories presented in
Europe as well as in America, the committee recommended that the
calculation of ultimate strengtlh be based on the following assumptions.
(1) As ultimate strength is approached, stresses and strains are not
proportional, and the distribution of compressive stress in sections subject
to bending is non-linear. The diagram c~f compressive concrete stress
distribution may be assumed a rectangle, trapezoid, parabola, or any other
shape which results in ultimate strength in reasonable agreement with
comprehensive tests. In addition to this broad assumption, the joint
committee recommended a specific set of limiting equations for various
typical design cases as discussed in the following pages. These limiting
equations are in good agreement with comprehensive tests of reinforced
concrete, and calculated ultimate strengths based on a chosen stress
distribution should therefore not exceed these given limits.
(2) Plane sections normal to the axis remain plane after bending. When
deformed reinforcing bars are used,
this assumption has been verified
even for high loads by numerous tests to failure of eccentrically loaded
columns as well as of beams subject to bending only.
(3) Tensile strength in concrete is neglected in sections subject to bend-
ing. When normal percentages of reinforcement are used, this assumption
leads to results in good agreement with tests. For very small percentages
of reinforcement it is on the conservative side.
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4) Maximum concrete strain in ffexure is limited to 0.003. This is a safe
value; most strains observed in tests of reinforced concrete members fall
between 0“003 and 0“0015‘G).
(5) Maximum fibre stress is assumed not to exceed 85~0 of the com-
pressive strength of 6
x 12
in, cylinders, A maximum stress near 100~0 of
the cylinder strength has been found in tests of horizontally cast mem-
bers’7’. In vertically cast members such as columns, however, due to water
gain resulting in a lower strength near the top, and due to effects of size
and shape, a maximum stress of 8.5’~ of the cylinder strength has been
observed ‘8’9’.Since some effect of size and shape probably also is present
in large beams, and since the concrete near the top of beams as well as
columns may be somewhat weaker than control cylinders, it seems
reasonable in all cases to use an 8.50/0 stress.
(6) Stress in tensile and compressive reinforcement at ultimate strength
is assumed not to exceed the yield point of the steel used or 60,000 lb/in2,
whichever is smaller. The purpose of the 60,000 lb/in2 limit is, of course,
to avoid excessive cracking under service loads. This limit is conservative,
considering the high effectiveness of the bar deformations that are now
in use throughout our country. It is also possible, to some extent, to
control cracking by other variables than steel stress.
RECTANGULAR BEAh4S
To establish limiting equations for ultimate strength in the various
cases, the joint committee chose a theoretical approach originated by
F. Sttissi of Switzerland in 1932 and based on the general properties of
the stress distribution shown in Figure 1. The properties of the stress
l-- b l
l
h:
J
c
—.
As,
Figure 1: Flexwd analysis.
block are given by the stress factor O“85kl (German: Volligkeitsgrad) and
the centroid factor
k2
(German: Schwerpunktsbeiwert). Equilibrium of
forces and moments then gives:
-4s,j_,U=0.85 klu@c.. . . . . . . . . . . . . . . . ..(1)
,MU= 0.85kluCY@c(dl—I@ . . . . . . . . . . . . . . . . . .(2)
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When tension controls ultimate strength, the ultimate steel stress f,U
equals the yield point Y;, and the ultimate resisting moment obtained by
solving equations (1) and (2,) is given by:
/
in which
AS, =
d, =
O“85k1 =
k, =
ucy/ =
r
b=
k,
rfy
)
MU= A,lfydl I—-—— . . . . . . . . . . . . . . .
0.85k1 UCY,
}
(3)
area of tensile reinforcement
yield point stress of reinforcement (limited to 60,000 lb/in2)
effective depth
t
centroid of tensile reinforcement
stress factor, ratio of average compressive stress to uCYl
centroid factor,, ratio of depth to resultant of compressive
stress and depth to neutral axis
compressive strength of 6x 12 in. cylinders at 28 days
A,,,
ratio of reinforcement = —–
bdl
width of beam
The quantities kl and k2 are fundamental properties of concrete that
have been determined by direct tests of plain concrete specimens(T).
Equation (3) is then a fully rational equation developed by the equations
of equilibrium from measured properties of the materials steel and
concrete.
Equation (3) may also be developed on a more empirical basis by study-
ing the results of reinforced concrete beam tests. The author recently
determined the coefficient –—
~~k from published data on 364 beam tests
1
by the statistical method c)f least squares, and the value of 0“593 was
0.5
found. A value of— =
0.59 was suggested by C. S. Whitney over ten
0“85
years ago[lO), and this value is also in good agreement with the direct
tests of plain concrete(7’.
It is entirely reasonable, therefore, that the joint committee recom-
mended that the computed ultimate moment of beams should not exceed
that given by
)
W=A,,,fYdl 1-–0.59:/ . . . . . . . . . . . . . ...(4)
CY
which can be re-stated as
Mu
—=q(l-– 0.59q) . . . . . . . . . . . . . .
. . ..(4a)
z, .,,
rfy
in which q ==—.
Y
When compression controls ultimate strength, the steel stress at failure
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may be determined by considering linear distribution of strain (Figure 1):
dl — c
E
U
= Ecu-— . . . . . . . . . . . . . . . . . . . . . .(5)
c
Combining equations (1) and (5) and seeking the balanced reinforcement
ratio for which
f,. = fY, we
obtain
Ecu
U@
‘b= ”85k’k
h“”””””””’”””’”’”””
j-- +
Ecu
~s
6)
The maximum ratio of reinforcement in equation (4) should be some-
what less than the balanced ratio given by equation
(6).
Choosing a
limiting value of
r
equal to about 90’70 of
r~,
the joint committee recom-
mended that
r
should not exceed
r=o.40@’ . . . . . . . . . . . . . . . . . . . . . ...(7)
f
in which the coefficient 0.40 is to be reduced at the rate of 0“025 per
1,000 lb/in2 concrete strength in excess of 5,000 lb/inz. Such reduction
for high concrete strength is desirable on the basis of several experimental
studies that indicate a decrease of the stress factor,
0.85k,,
with increasing
concrete strength (7,11’.
When the ratio of reinforcement exceeds that given by equation (7),
compression reinforcement must be provided. For this case, the joint
committee recommended that the resisting ultimate moment should not
exceed
MU = (AS*— AJj;dl 1— 0.59(r -– r’)~
1
+ f J d,d, ) 8)
Ury(
in which (r — r’) should not exceed the value given by equation (7), and
A C=
area of compressive reinforcement
A
r’ =
ratio of compressive reinforcement = ~
bd,
d2 =
effective depth to centroid of compressive reinforcement
For beams with the usual amounts of reinforcement dictated by economy
and spacing of reinforcing bars,
r
is 0.15 to 0.25 times 4[, and there is
f,
little difference between designs resulting from ultimate strength and
straight-line procedures. The major changes suggested by the committee
therefore concern a more efficient use of reinforcement with yield points
over 40,000 lb/in*. In present American design codes based on straight-
line theory a ceiling allowable stress of 20,000 lb/inz is used for such
reinforcement, while the ultimate strength design method as outlined may
lead to the equivalent of a.n ailowable stress of 60,000/ 1.8 =. 33,300 lb/in2.
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As a second change it is made possible, when economically and practically
feasible, to utilize more fully the strength of the concrete compression
zone.
T SECTIONS
If the neutral axis falls within the flange of a T beam, the equations for
rectangular beams are applicable with r cc~mputed as for a beam with a
width equal to the overall flange width. The depth to the neutral axis, c,
may be estimated by solving equation (1):
1 r~d
c=n@~l=—’—
0“85k1uCYl 1“””””’””””””””””’”
.
.(9)
In this case, the joint committee recommended a conservative value of
c = l“30rfy4.
Ucyl
When c is greater than the depth of the flange, the tensile reinforcement,
A,,, may be considered subdivided into one part, A,f, that will develop
the compressive strength of the overhanging portion of the fldnge and
another part,
(A,f — A,f),
that will develop the compressive strength of a
a portion of the web. Assuming a uniform stress of 0“85uCYZn the flange,
the joint committee recommended:
[
1
u=A, ,At f ) j j i ,— 0.59(r~ — rf) + A,f~(dl — ~“5t). .(10)
CY
in which A,f is the steel area necessary to develop the compressive strength
of the overhanging flange:
A,~=O”85@- lY)~l . . . . . . . . . . .
. . . . . ..(11)
h
and
flange thickness
b = overall width of flange
b’ = width of web
r =2
:dl
AS,
‘w = b’dl
A,f
rf=—
b’dl
In equation (10) the value of (rW— r~) should not exceed that given by
equation (7).
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CONCENTRICALLY LOADED SHORT COLUMNS
The joint committee recognized that the strength of concentrically
loaded short columns is given by
Fo=0.85uC,vlAC +A,~ . . . . . . . . . . . . . . . . . . ..(12)
in which
AC = gross area of concrete section
A, = total area oflcmgitudinal reinforcement
It wasrecommended, however, that all members subject to axial loads
should be designed for at least a minimum eccentricity. For spirally rein-
forced columns the cc)mmittee gave a minimum eccerrtricity measured
from the centroidal axis equaI to 0.05 times the depth of the column
section; for tied columns O.10 times the depth was recommended.
This recommendation involves a change from present practice which
limits the allowable load for a tied column to 80 of that for a spirally
reinforced column. This change seems reasonable since in practice very
few columns are trul~y concentrically loaded, and recent tests(g) have
indicated that for columns with even a small eccentricity of load, no
second maximum Ioad is developed due to spiral action.
ECCENTRIC LOAD, F~ECTANGULAR SECTION
The uItimate strength of members subject to combined bending and
axial load may be computed from tlhe usual two equations of equilibrium,
b
C
——
Figure 2:
Eccentric load analysis.
which, when the neutral axis is within the section, may be expressed as
follows (Figure 2):
FU = ().85klUcY~hnudl+ A.C~Y— ,4.,~,u. . . . . . . . . . . . . . (13)
Fue = 0085kluCY@Ud12(l— k2n.) + A,~L(dI -– dz). . . . . . . (14)
in which
FU =
ultimate eccentric axial load
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e
= eccentricity of the axial load measured from the centroid of
tensile reinforcement
Au = stress in tensile reinforcement which equals ~Y when tension
controls ultimate strength, but is smaller than ~Y when com-
pression controls
nudl = c = depth to neutral axis at ultimate strength
In the above equations, the joint committee recommended that k,
should not be taken as less than
~kl,
and hl should not be greater than
0“85 for UCY1 5,000 lb/in2. The coefficient ().85 should be reduced at the
rate of 0“05 per 1,000 lblinz concrete strength in excess of 5,000 lb/in2.
By solving equations (5) and (,13) forj~U ==f, and ECU= 0.003, it is found
that the ultimate load for the balanced condition is given by
0.003E,
F~ = 0-85k1 ——
0“O03E, + f, )
UQ@dl + (Asc — z4Jfy . . . . . .
(15)
When FU is less than the value of Fb given by equation (15), ultimate
strength is controlled by tensicm and .fiU= fY. Taking into account the
concrete area displaced by the compression reinforcement and solving
equations (13) and (14) for the ultimate strength, we then obtain:
1
) \
FU = 0.85uCYlbd1
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A linear relationship between axial load and moment may be assumed
for values of
FU
between
Fb
as given by equation (15) and the concentric
ultimate load Fo given by equation (12). For this range the ultimate
strength may therefore be computed by
FO
FU=—
()
. . . . . . . . . . . . . . . . . . .
(17)
1+ ;—15
eb’
in which
e’ == eccentricity measured from plastic centroid of section
e~’ = eccentricity of load Fb measured from plastic centroid of section
as computed bly solution of equations (14) and (15).
The plastic centroid of a section is computed with a “ modular ratio “
m“ = ~
For symmetrical reinforcement, the plastic centroid coin-
0.85uCY,“
tides with the geometric centroid.
The joint committee also recognized the equation developed by
C. S. Whitneytl”j for ultimate strength when compression controls:
A,Cu + - btu,,,
Fu= —
. ... . . . . . . . . . . .
(18)
e’
—“
;+1”18
d, — d,
1
in which
total depth of section.
Though we] 1 substantiated by test data, the methods presented above
for the ~esign of eccentrically loaded rectangular sections involve a major
change from present American practice. Even though the principle of the
addition law as expressed by equation (12) is recognized in present design
codes for small eccentricities, the safety factor with respect to ultimate
strength may vary frc~m near one to over four, depending on the com-
bination of variables involved. By the proposed ultimate strength design
procedures, a much more uniform safety factor will be obtained. It should
also be noted that l.he mathematical equations involved are greatly
simplified as compared to a modified straight-line theory.
ECCENTRIC LOAD, CIRCULAR SECTION
The ultimate strength of members of circular cross-section subject to
combined bending and -axial load may be computed on the basis of the
equations of equilibrium taking inelastic deformations into account. The
joint committee also recommended use of a modification of the partially
rational and partially empirical formul~ developed by C. S. Whitney (9.10).
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When tension controls:
FU= 0“85uCYlD~
{/(
0.85e’
)
——0.38 2 + ‘%
D
-(
)
~-O.38 } . . . . . . . . . . . . ..(19)
When compression controls:
4fy _
Fu=—
ACuCYl
. . . . . . . . . .
(20)
:+ 11
9“6De’
(O%D + 0“67D )2
+ 1.18
s
in which
D =
diameter of circular column
D, =
diameter of circle circumscribing longitudinal reinforcement
A,
rt=—
AC
LONG MEMBERS
For cases when the unsupported length., L, of an axially loaded member
is greater than fifteen times its least lateral dimension, t, the joint com-
mittee recommended that the maximum axial load,
FM’,
should be deter-
mined by one of the following two methcjds.
The effect of slenderness on ultimate strength maybe taken into account
by stability determination with an apparent reduced modulus of elasticity
used for sustained loads. A numerical procedure such as that recommended
in the report of ACI Committee 312 on Plain and Reinforced Concrete
Archestlzj may be used.
The maximum axial load may also be determined by
)
U’=ZFO 1“6— O.04~ . . . . . . . . . . . . . . . .
. .(21)
t
in which F. is the concentric load capacity of the section with L/ t
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Practical applications
After one becomes farniiiar with ultimate strength theory for reinforced
concrete, the design equations involved are considerably simpler to use
than those resulting from the straight-line theory, Further simplification
of routine design calculations is nevertheless desirable. The joint com-
mittee report’4 ) contains several charts intended to expedite the propor-
tioning of sections by ultimate strength theory. Development of further
design aids is in progress.
THE AC I BUILDING CC)DE
The joint committee report is an engineering report; it is not a building
code, it is not a standard specification. To gain widespread practical
application, therefore, ultimate strength design must be incorporated into
design and building codes,. Ultimate strength design in America has now,
in the opinion of many of us, been developed so far that extensive practical
experience is necessary to continue progress.
A proposed revision of the ACI Building Code was reported by ACI
Committee 318 in December 1955(Z). This proposed revision incorporates
the ultimate strength method of design as an alternative to tlhe straight-line
theory, and an abstract of the joint committee report on ultimate strength
design is given in an appendix. This proposed revision was unanimously
adopted by the 1956 convention of the ACI.
In this manner, after extensive scientific researches and a decade of
thorough committee work, the ultimate strength design method has been
placed before the engineering profession. The future of ultimate strength
design in American practice is, therefore, now largely in the hands of
our engineers and architects practicing the science and art of reinforced
concrete design and construction.
1.
2.
3,
4.
5.
REFERENCES
KEREKES, F. and
REI I
H. B. Jr. Fifty years of development in building code
requirements for rei ttfoneed concrete. Journal oj”the American Concrete Inst itute.
Vol. 25, No. 6. February 1954.pp. 441-470.
Proposed revision of building code requirements for reinforced concrete (ACI
318-51).
Journal o f the American Concrete Institute.
Vol.
27, No. 4.
December
1955. pp. 401-445.
CORNING, L, H., ANDERSON, B. G,, HOGNESTAD, Ii, SIESS, C. P.,
REESE, R. C. and LIN, T. Y. Symposium on ultimate strength design.
Journal
of the Ainerlcan Concrete Institute. Voll. 23, No. 10. June 1952. pp. 797–900.
Report of ASCE-ACI J,Dint Committee on ultimate strength design. Proceedings
of the American Society of Civil Engineers.
Vol. 81, October 1955. Paper 809.
pp. 68.
ACI-ASCE COMMITTEE 327. Ultimate strength design.
Journal of the American
Concrete Institute. Vol. 27, No. 5. January 1956. pp. 505-524.
1 3
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6. Discussion of a paper by E. Hognestad: Inelast ic behaviour in tests of eccentrically
loaded short reinforced concrete columns. Journal of the American Concrete
Instiiure.
Vol.
25, No. 4.
Dec[:mber 1953. Fig. G. p. 140/13.
7. HOGNESTAD, E., HANSC)N, N. W. and McHENRY, D. Concrete stress
distribution in ultimate strength design. Journal o~the American Concrete Institute.
Part 1. Vol.
27, No. 4.
December 1955. pp. 455-479.
8. RICHART, F. E. and BROWN, R. L. An investigation of reinforced concrete
columns. University of Illinois Engineering Experiment Station. June 1934.
Bulletin No. 267. pp. 91.
9. HOGNESTAD, E. A study Of combined bending and axial loud in reinforced
concrete members. University of Illinois Engineering Experiment Station.
November 1951. Bulletin No. 399. pp. 128.
10. WHITNEY, C. S. Plastic theory in reinforced concrete design. Transactions of
the American Society oj Civil Engineers. Vol. 107. 1942. pp. 25 1–282 . Discussion
pp. 282-326.
11. RUSCH, H. Versuche zw Festigkeit der Biegedruckzone. Deutscher Ausschuss
fur Stahlbeton. No. 120.1955. pp. 94.
12. Report of ACI Committee 31,2: Plain and reinforced concrete arches. Journal o f
the American Concrete Institute. Vol. 22,No. 9.May 1951. pp. 681-.69I.Discussion
Vol. 23, No. 4. December 1951. pp. 692/1-692/11.
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D8
—“Resurfacing and patching Concrete Pavement with Bonded Con-
crete,”
by EARL J. FEL r.
lteprintedfrom Proceedings OJthe H{phuau Research Boar d 5 1956 ,
D9
—“Review of Data on Effect of Speed in Mechanical Testing of Con.
crete,”
by
DOUGLAS MCHENRY and J. J. SIIIDELER.
Reprinted from Speeiat Tectmical PubUcation No, 185, published by Ameri-
can Society for Testing Materials 1S5S).
DIO-’’Laboratory Investigation of Rigid Frame Failure,” by R. C.
ELST-
NER and E. HOGNESTAO.
Reprinted from Jrournulof the Amertcan Concrete
Institute
anuary, 1957);
proceedings, 53, 637 1957).
D12-’’Ultimate Strength of IReinforced Concrete in American Design Prac-
tice,” by EMND HOCNESTAD.
Reprinted from
Proceedings of a S mpos@n on the Strength of Concrete
Structures, Lond,m, May, 1956.