145 108 THS DEfifiié~i CURVES PM? REiNI‘f-CSRCED CQNCRETE fiflivfiif‘éfifi FifiGT’EMGS ON SC‘E. . f3". 0:111}, ' Q 3.; r K o“. i ‘ ., fi« 5.1". 0 (-¢'.\.‘ U a '3 in ~.-’ g I “N . 5: A x: .":“‘ ~~2:='- 4' t R'- ::- . u‘ofi‘wlh‘du‘ .0 Quilt. $1. ‘2; souls 0-189 -,____ ..._'___ J- l__4.. -..___:_._... ._ ‘J_'._._ _ A _;___.L..., _ L.-- This is to certify that the thesis entitled DESIGN CURVES FOR REINFORCED CONCRETE COMBINED FOOTINGS ON SOIL presented by AVRAM KAZEZ has been accepted towards fulfillment of the requirements for M. 8. CIVIL ENGINEERING degree in WWW Major professglw Date Mfimh 1.13 3 fi1952 "—_ 'I-—‘ —.3'- I.!—~——'1—_v— ' a I ‘ . . 75;» -‘ '4‘ ‘1 g ’;‘-.".".: E _ ' . 'r . -, .1. ' 23$??? ~_ \ «{v’av ‘ . 'xvlg' ‘ ~' .3 - |' - V‘s-«rip. wt 4_ .._. 1,E. “ 3.‘ ".2. ' . . H..- . u . 5‘- . . .’.J\...\. . “mf'fir‘w " ' ‘5 N Aflfifif" 7‘; )' Ul‘.\-g' 5- ‘Y '1‘ 7 " \. z ' ‘39. ‘ .' }. t .. Qn, . (aw _ , ‘ E \ ‘1‘}? t‘ . ‘K’: I; ‘3 I. I :1“: ’5'“ .. I ‘3‘ Av M. J , . . .. .3 ,- l o ' . ‘7‘ .\.. , .1 .. . ‘.. “M’WW5M ' pv ‘ jfleWWM-r'g I.- m " led-‘1'" {If *7 '1 ‘ . .. . _, s —' . .I r‘ s . . ’.., .‘ .7 , . s . -t" .- ‘ ? I ' 6’5.” u,- ¢_ ~o_~ "lay. ”a“. '._o ‘ J T'fi. [if .‘. . .. .4 D I 'I u ‘ - . J ~31. «I’I' \ x ' . . - I e .; ‘ >, . E . . U \ ’~ ‘\ /‘2’\‘. )1 94 - .l . s L DESIGN CURVES FOR REINFORCED CONCRETE COMBINED FOOTINGS ON SOIL Thesis for the Degree of M.S. Michigan State College Avram Kazez 1952 DESIGN CURVES FOR REINFORCED CONCRETE COMBINED FOOTINGS ON SOIL By AVRAM KAZEZ A THESIS Submitted to the School of Graduate Studies of.Michigan State College of Agriculture and Applied Science in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE Department of Civil Engineering 1952 THESlS V/ E. g IrI // 3’ a" '4 ‘V l, \ .5 3' 1! CONTENTS Introduction . A. . . . . Assumptions, Notations and Definitions. Typical Shear and Moment Diagrams. . Condition for Minimum Depth of Footing. Derivation of Equations for Curves: 1. Length of Footing "L" . . 2. Effective Depth of Footing "d" 3. Width of Footing "B" . . 4, area of Steel Required "AS" . 5. Bond "21" . . . . 6. Shear "v" . . . . Explanation of Curves: 1. Length of Footing "L" . . 2. Effective Depth of Footing "d" 3. Width of Footing "B" '. . h. area of Steel Required"AS" . 5. bond "2." . . . . . Numerical Example . . . . . Summary . . . . . . Appendix . . . . . . Bibliography . . . . . . 10 «E f- Y r" '4‘ My“. Z3 10 12 12 13 1h 15 19 23 25 32 33 31. 35 1.1 _ INTRODUCTION 1. Introductory Statement This study describes a simple graphical procedure for de- signing reinforced concrete combined footings. The design curves presented in this studv can be used by a designer or checker. Following the derivation of equations, the curves are drawn and a typiCal example of their use is given to make the method of procedure clear. Derivation of the scale equations used to draw the charts are given in the Appendix. It is hoped that the use of the charts herein will eliminate calculations thereby saving time. 2. Scope With the use of the charts,the length and width of the footing, the effective depth, the steel, bond required and the shear stress are found. This study is not concerned with the selection of the main or web reinforcement bars, nor in their distribution. -2- 3. Acknowledgement. The author wishes to express his indebtedness to Dr. R. H. J. Pian for his valuable advises and suggestions, and also to acknowledge his thanks to Mr. W. A. Bradley who read the study. ASSUMPTIONS, NOTATIONS AND DEFINITIONS 1. Assumptions Adaptation of the nomograms will be made to design a combined _ footing, which will meet the following requirements: a) An area great enough to give the safe allowable soil ‘ pressure. b) A shape such that a uniform net soil pressure is given. c) The two loads acting on each column are equal. d) The footing will have a constant depth. 2. Notations and Definitions The symbols in this study, defined below conform essentially to Letter Symbols for Structural Analysis prepared by the Americai Standards Association, with ASCE participation, and approved by the Association in l9h9. For their significance, where not confor- ming to the standard, is made clear by Fig. l. *1; P Al: .h A ,..___-_ L a D B *4. h; where '0 21 T! i t“ {T w 0.. 0 load on each column in kips. fallowable soil pressure in 1b./ft.sq. weight of footing in lb. 'soil pressure against base of footing resisting column loads in lb./ft. of length. effective depth of the footing in inches. width of the rectangular footing in feet. height of base of footing in inches. length of footing in feet. distance between column loads in feet. distance between outside edge of column and width of footing in feet. size of column along the length of footing in inches. distance between outside edge of the columns in feet. distance between center line of footing and column load in feet. lll\l:'|lll|l|\ ('1 l‘ (I || r Typical Shear and Moment Diagrams. 3 o. l‘b (I) . + Shear /\ b g _i Diagram é \\;//’/, (II) Pu Na + + Moment 9 . Diagram (III) Fig. 2. CONDITION FOR MINIMUM DEPTH OF FOOTING From the moment diagram in Fig.2(II), the moment at point a; Ma - r2? - BKd2 T but, A - BL therefore, f2P - AKd2 . . . . . . . _ (a) Keeping P, A and K constant, the variation of "f" with "d" will be investigated. Then ' d - elf where if is a constant. The equation above represents a family of straight lines through the origin with positive slopes. Plotting "d" as ordinate and "f" as abscissa, the family of lines below is obtained. d‘} Fig. 3. Similarly theexpression for the moment at point b willbe Mb - Py - 12w - BKd2 - . 8 Similarly, the expression for the moment at point b can be written; Mb- Py - L2w/8 - BKd2 Simplifying terms and substituting, B - A/L hyL - L2 - hAKdz/P . . . . . . (b) but, y - (c-b)/2 and L-2febsc therefore, 2(c-b)(2f+b+c) - (hf2+hfb+ufc*b2+2bc+c2) - AAKdz/P simplifying and transposing terms, -c2+4hr.2b2+ur2+arb+b2+2bc+uAKd2/P - 0 Keeping P, A, K,b, and c constant the variation of "f" with "d" will be investigated. Then kldzo 4r2+ 6bf + k2 - o where k1 and k2 are constants. The equation above represents a family of ellipses with center at (-h, 0). Plotting "d" as ordinate and "f" as abscissa the family of ellipses below is obtained: d4L -8- Superimposing a typical curve of each family shown above, at Painf, 0.. ‘__-__~ fix or PO;an b' Fig.5. Investigating the variation of "d" with "f" in Fig. 5 it is concluded that; the depth "d" of the footing is to be designed for the largest value of "d" required at any point. Therefore the smallest value of "d" required for the footing will be when the required depth at points "a" and "b" are equal. From equations (a) and (b), and Fig. 2(III), it is obvious that for the above condition filaJ = II‘ 1 b DERIVATION OF EQUATIONS FOR CURVES 1. Length of Footing "L" An expression for the length of the footing "L" will be derived for the condition IMa|- IMb From the moment diagram in Fig. 2(II); the following equa- tion can be written. lMal ' £2! and ‘Mb' ' Elgihl “'ééfl hence Eéé ' P§n+b2 _ Lg! or Egg * Egg . Ejggbl from Fig. l y - 2&2 therefore Egg + 3%: . py also w - é: therefore ggéi-e 23%: . py simplifying terms 4r2+ Lz- AyL From the above equation it is concluded that the length "L" of the base is independent of the loads "P" on the column. -10- Substituting f = L-§-C and I 2y = c in the above equation (L-b-c)2 + L2 - 2cL (L2+b2+c2-2Lb-2Lc+2bc) + L2 = 20L 2L2 + (b2+2bc+02) - 2Lb -th = o L2 + (b20)2 - L(22+Ac) = O L2 — (b+2c)L + (b+c)2 = 0 __§___ Solving the quadratic equation above for "L" in terms of "b" and "c", or, L = b + 2c + J2c2 — b2 . . , . (1) 2 8.150, f g L "' b - C o e o e o o (2) 2. Effective depth of footing "d" The value "d" is usually calculated by assuming the weight of the footing, then checking the weight. An expression for "d" in terms of the already known values will be derived, thus eliminating the ambiguous method of trial and error. As before, but; hence also; where, For a balanced design; or, '14 and -11.. M = f2w/2 w . 2P/L M - fZP/L - BKd2 B is in feet. f is in feet. d is in inches f2P/L - BKd2 BL a f2P/Kd2 o e o (3) Two eXpressions for the weight of the footing "N" can be written, and, where, Equating equations Substituting equation multiFlying by VJ‘BBPL'ZP o o o (h) w - 150(%+L)LB . 12.5(d+h)LB . . (5) 1 L is in feet. P is in lbs. (A) & (5); BpL - 2P = l2.5(d+h)LB . (3) in (6); f2.P - 2P = 12.2(d&4)f2P EEZ“ Kdz d2 sz; (6) -12- 2 p - 2K? = 12.5(d+h) or, 2Kd2 + 12.5(d+t) = p . . . (7) "d" can be calculated from equation (7), as all other variables are know. 3. Width of footing "B" The value of "d" once known, the width of the footing "B" will be evaluated. As before M = fZP/L also, M = KBd2 for a balanced design, KBd2 = M = f2P/L . . . . (11) "B" can be calculated.from equation (11), as all other variables. are known. L. Area of steel required "AS" The area of steel "AS" will be calculated from equation below PI 2: JdeAS e o e e o (12) -13- 5 . Bond " 20" The shear force "V", at the outside edge of the column from Figs. 1 a 2 is: v a 2Pf/L . . . . . . (13) and at the inside edge is: v = 2Py/L = P(c-b)/L . . . (14) the larger value of V above is of interest, P(c-b) #7 22; . . . . . (15) L L dividing both sides by P/L and substituting equation (2) for"f" c-b f L-b-c or, c # L-c . . . . . . (16) from chart A the.following approximate equation can be written L -(%%;%)c = 1.75c substituting the latter value of L into equation (16); v0 f 1.75c-c c K 0.75c hence; c>0.750 therefore (C - v/Z > f e o o o o o (153) The shear force "V" expressed by equation (It) will have the larger value, which will be used to evaluate"2k" also, V 3 g‘d°u‘200 o o e o e (17) equating equations (14) and (17), 2Py/L = V = %-d~u-ZO . . . . (18) -1g- 6. Shear "v" The shear "v" will be calculated from equation below V 3 VJdB o o o o o e o (19) -15- EXPLANATION OF CURVES 1. Length of footing "L" The first curve will be drawn to evaluate the length of the footing "L" by equation; L - h122_:_122E;£E1 . . . . . . (l) 2 Owing to the fact that the variables in the above equation cannot be separated, a value of "b" will be assigned and thus eliminating one variable. For the same value of "b" different values of "c" will be given and the corresponding values of "L" calculated. The L- and c— scales will be at right angles to each other and will have uniform scales. Hence the nomogram will have the form shown below: Fig.6. -16.. c will vary from 5 to 25 ft. Its scale: 5 ft. = 1 inch. b will vary from 12 to 36 inches. 1 will vary from 9 to A5 ft. Its scale: 10 ft. = 1 inch. (See chart A.) The second curve will be draWn to evaluate "f", by equation L a 2f + b + c . . . . . (2) alignment charts will be used. let L - c = T then L - c a T = 2f + b Let the modulus of L, mL be equal to 1/10, which is the same value as before. The scale length of "c" will be about A inches. m s h" 2 1/5 C "F 3-1... hence, mT = mg . mc mL + me = 1/15 consider equation T = 2f + b ms= .1." = 1/3 3 Inf 8 ml . mb mb - HIT = 1/12 The relative distances of the scales to each other will be calcuhated: -17- mL/md = 5/10 = 1/2 similarly mf/mC - 3/12 = l/A and the scale equations will then be: XL = L/lO (L is measured in feet) Xc = c/S (c is measured in feet) Xb - b/3 (If b is measured in feet) = b/36 (If b is measured in inches) and Xf = f/6 (f is measured in feet.) The general form of the Alignment Chart for the equation, L = 2f + b + c, is shown below: Fig. 7. Since the modulus of L is the same in both charts, Fig. 6 and 7 will be combined. The complete chart thus, and drawn to scale is drawn on next page, (chart A). an»: E 0 5 m 5 m- 5 i 2 FLILILIL21L)h(-gla)L a - - - - _ - - - - _ 3...: v:~ C. ON 5 o 5 x .5. 3 2 K- M .w — * r—- '— T u - 7-).) (_1.(_IJJ((4|.I.)1 4. 414(14)- A mob7s54oalo . “v.* Zak +l r a .h If; C- J 0 b H b h L 5 2 a (O 2 Y T #5 y f . a, .m C 1.0 -19- 2. Effective depth of footing "d" The value of "d" will be found from equation 2kd2 + 12.5(d+l) - p . . . . . (7) let z . substituting equation (8) in (7); zd2 + 12.5(d+t) = p . . . . . (9) First a curve for equation (8) will be drawn. The values of "K" can be taken from "Reinforced Concrete Design Handbook". f varies from 1 to 10 feet. K varies from 125 to #23. therefore 2 varies from 5 to 500. The scaIe lengths are to be approximately 5 inches. equation(8) can be written in the form; log 2k = 2 logf + log 2 -2 log f = - log 2k + log 2 then, mK = 6" = 11.3 log 8A6 - logV25O A more convenient value mK= 10 will be used. and, m = " = 3 Z log SOO - log 5 therefore, mf = mKi. ng = 3x10 = ~20- The relative distances of the scales to each other will be cal- culated: mg = 10 3— the scale equations will then be; XK X z Xf The general form of the Alignment z = 2K , is shown below: T? A /—4 K /-4k/ /// ,c 2 (V/ () ’ Fig. 8. 10 (log2K 3 (log 2 - 30x2 logf 13 log 250) = 10 log (K/125) log 5) = 3 log (2/5) A.62 log (f) Chart for the equation, The value of "d" will now be evaluated. substituting (8) in (9); zd2 or; zd2 solving for d; d + 12.5d + (so-p) = o + 12.5(d+u) - p - 12.5 +~Jl12.5)2 - 4.2 (50 - p)1. . 2.2 (10) -21.. A value of "p" will be assigned and the corresponding values of "d" will be calculated for different values of "2". Same procedure will be repeated for different values of "p" assigned. The general form of the nomogram is shown below: A Fig. 9. The modulus of "z" will have the same value and hence the latter two curves will be combined to give the complete nomogram drawn to scale on next page. Q5 R a .( [3)_1 4) I I —< ( Z i x 1 Y 3 _J I i. 4 4' .1 (hm—a 8“ _, i Z —< k 4 4- ,, ’1 a U A V- —-1 -J 7; 1 C5—( l - d x. E A “ x < \. fl _.}_”4 500——( 3—1 4 h a b_‘ l -\ I .4 ——( - /——( \. a \s» —— —< 8* 400—4 t]-——. .4 i i ’0‘ 425 l E jTIITTllTjTerr,)lellllTrlllT‘l o 5 IO (5 80 25 30 d )n inches Charf B -23- 3. Width of footing "B". First the curve for equation, M - f2P/L will be drawn :2. l M P or, f varies from 0 to about 10 feet. L varies from O to about 50 feet. P varies from 0 to about 1300 kips. M. therefore, [I] I " I 0.05 f TEEECZG m - 5" - 0.1 L “UT—5 mP - ". - 0.00385, Use mp - 0.00h o - ’ varies from 0 to about 3000 ft-kips. therfore, mM - m£.mz m 0.002 mL The scale equations are; X X - 0.051“2 L - 0.1L XP - 0.00hP XM - 0.002M . The general form of the chart for the equation.M - f2P/L is f shown below: Fig. 10. The value of "B" will be evaluated next from, or, therefore then, the scale equations The general form of the chart for the equation M = below: -24- M = KBd q a 32 B I7K p-a varies from fly 0 to 3,000,000 ft-lb. d varies from O to 30 inches. K varies from 125 to 423 psl. B varies from O to 10 feet a 6" 3,000,000 a l/500,000 m. 4‘ N. m = A N 900 . 6.1“! l 125 = 0.004,ll mK - 800 mB - u.m5 - 0.36 md are: a: ll M/500,000 0.00t,ttd2 N O. u 800/K >4 \ ll >4 I _ 0036.8 KBd2 is shown -25- Fig. 11. The M - scale lengths are the same in both equations and hence the twoczharts foreequation (11), will be combined. (See chart B) A. Area of steel required "AS" The value of "as" will be evaluated next from, lbo-ino o o o o (12) I511: 7ofSodoA g S or M = 1 x .f -d-A lb.-ft. ’ rigs“; or, g = 7A 96 d M varies from O to 3,000,000 ft.- lb. d varies from 0 to 30 in. fsvaries from 8,000 to 30,000 psi. Asvaries from 0 to 100 in. mg; "’ " = 1 00 00 W00— /5 ’ O -26- md = h.2" = 0.1h lflfs I: 6" = 14,92,000 172000" m.S = 48,000 x 1/500,000 = 2a/35 11 0.14 the scale equetions are: xM= m/500,000 id = 0.1hd xfsa 48,000/1‘S X. As As/20 The general form of the chart for the eqution M = is shown below: As A k f / / A / ’ifi» M [##I.’ «V’if/ / d v / / J = 1“, Fig. 12. The modulus of "M" will have the same value and hence the latter three curves will be combined to give the complete nomg- gram drawn to scale on next page. feet in 7—4 _.__.. 1-1. __ A 400 , L,__,l g 300 P H) 900 800 _;*l -__1 ___-l l -1. / ’9 I I j I 7' T T I I: I do (’5 L in her 1 I Y 7 , 1 L i. r T I I 3:5 U ' Z .5 3 5 b 7 8 V If 4L. _J_.TI-1 lr_.L.l,__L TL _ 1T _ TL . ‘T l r ex__!i ,_A.,,--L T l- ' I' i -_l,_.l \\ IO 20 JO 4O 50 I 60 I”) fix 1 ' ‘00 ,\\\\ / \\\ \ \\ / r \\ i \ i \ i I i , _ i “ \ l , \ t f \ \ i \ f ‘.. s -\ \ \\ ,\ i. l a f; 1") K]; Ln, 5 to r2 ;4 ' 0 :3 a0 22 24 27 30 I 1 I 1 f ,____,‘J___V_ _ 1cm, _‘L___,l._--,1a+ 33—1—4 l25 130 2"; U 10(1 400 K m psi (:f)ar"f C inchis 1% _50 m d 25~m 20~~¢5 ~L20 inches in d 5. Bond '1 20" The value of "V" will be evaluated from equation V = 2P1. .(lh) L'" or, y varies from 0 to 12 feet. L varies from 0 to 50 feet. P varies from 0 to 1,300,000 lb. 6": 1/2 m y I?“ III 5" = 1/10 30‘ m = 5.2" = 1/500,000 P 2,600,000 therefore mV = mg . mz = l/100,000 NIL the scale equations are: X y/2 Y KL L/10 P/250,000 KP v/100,000 Y 4L V The general form of the chart for the equation V = 2Py/L is shown below: -29- A A, P ‘ W \ A \ 1K\\\ \ V , \\\ \_ \ “‘-\~lfl \ \ V \ L . —.‘: Fig. 13. The value of "2;" will be evaluated next, from, v = 7ud2 . . . ‘ . . . (17) “8'“ or , V = 20 7d73 175 d varies from 0 to 30 inches. u varies from 140 to 350 m . 1/100,000 v m = 2.5" = &_ use m = l/7 d 30 x 773 21 ’ d - m = 5" = 700 u T7TZU‘ therefore m2°= 700 x 1/100,000 = 0.0h9 1/7 XV = v/100,000 ' x = d/8 -30- Xu = 700/u therefore X20= 0.01.9 2. The general form of the chart for equatiai V = 7udzois shown below: Fig. IA. The V - scale length are the same in both equations and the two charts for eqdation (18) will be combined. (See chart D) 6. Shear "v" The value of "v" will be evaluated from equation V g VBjd o o o o o o o (19) or, V = 12.B ‘ 7d7h I7v mV = 1/100,000 md = A" x 8 = 2 50 x 7 13 use, md = 1/7 m m = 205 10 x 12 mn.md mv The scale equations are: Xv = v/100,000 [x 3 >4 II P"; II The general shown below: d/8 B/z. 297.5/v fOrm of the chart for the equation V -31- 1/48 297.5 ijd is ban-b," P In kip: £0 ”7 I woo Q00 I100 1000 000 300 700 too 500 400 .300 200 :00 o 0 x) a. :u\ 4() L0 70 50 90 ’00 I L 1 l A 1 a I l I 1 L 1 l l 1' l l - l 1 I l 1 ' I -«L —< _., g 33 3 Icef '7 Sir—Ci}. U: 1 inches In T ’U‘ in pm. 0 r1 1 Y‘IY v 1 [1"ij [I 1 1111': r1 T! % rvrr I] l T111 111 1 1 11 4— 1 I 1— 0 IO 20 30 40 M0 :0 Am) 250 300 550 L m chf a m PSI Chorf D -33- NUMERICAL EXAMPLE an example of the use of the charts will be given to make the method of procedure clear. Given: Solution: P = 600 kips c = 15 ft. b = 2A" = 2 ft. r = 30,000 psi. f'= 2500 psi. p = 6,000 #/ft? u = 250 psi. (deformed bars, A. C. I. 1951 Code) From chart A. and with values of c and b: L = 27 ft. and f = 5 ft. K 2 156 ( Reinf. Conc. Handbook) From chart B and values of K and f: d = 21 in. From chart 0 and values of P, f, L, d, K, f5: B = 8.1 ft. and AS = 12.1 in2. From chart D and values of P,y,L,d,u,v,B, 2: 63 in. and v = 163psi. -34- S UI‘IH‘II A RY The curves are more flexible and cover a wider range of design conditions than the most comprehensive tables. Their use entails a minimum of calculation and shows clearly the de- sign procedure and the relation between the design conditions. The resultant design will be within the practical limits of loading and soil bearing determination. -35.. APPENDIX An alignment chart in its simplest form consists of three parallel scales so graduated that a straight line cutting the scales will determine three points whose values satisfy the given equation. In general, alignment charts may consist of three or more straight-line scales, of curved scales, or of combinations of both. ALIGNMENT CHARTS FOR EQUATIONS OF THE FORM rl(u) + r2(v) - f3(w) Suppose we have three parallel scales (Figure 16), A, B, and C, so graduated that lines (iSOp1eths) 1 and 2 cut the scales in values which satisfy the equation fl(u) + f2(v) s f3(w). Now, \V‘ , Q1 ) Xu Xw X Fig. 16. -36- >4 I u - mu fl(ul) - fl (no) v mv f2(V1I ' f2IV0I >< I Xw = mw f3(wl) - f3(w0) If no, v0, "0’ represent zero values of the function, and if line 2 is any line, we may drop the subscripts and write simply ‘7 4\ u mufl(U) o o o o o o (1) >4 u mvf2(v) . . . . . . (2) KW Let us agree further that the Spacing of the scales is in the mwf3(W) o o o o o o (3) ratis a/b. If we graduate the scale of f1(u) and f2(v) in accordance with their scale equations (1) and (2), reSpectively, what will be the modulus for the scale equation of f3(w) and what will the ratio a/b equal if the chart satisfies this relation f1(u) + f2(V) = f3(W)? In figure 16 draw lines through points W1 and v1 parallel to line uovo. The shaded triangles are similar by construction, hence, X - X = a ,u___gfl 3 AW ' Av Kub + Xva = Xw(a + b) Xub + Xva = X (a + b) ”11‘. ab ab ab -37- or XI + E! = Kw a b ab a + b since in = mufl(u) Xv = mvf2(v) f - mwf3(w) mufl(u) + mvf2(v) = m f2(w) a b ab a + b 2 mu = a, m = b therefore % - mu mv and m = ab = m m m‘” m + m -33- PROPORTIONAL CHARTS OF THE FORM fl(u) == f3(w) f2(v) fh(QI This equation can be solved in a manner similar to that used in the preceding problem. This simply means transforming the above equation to the form log f1(u) - log f2(v) = log f3(w) — log fh(q) In many cases, however, where the functions are linear, the prOportional type alignment chart has a distinct advantage in that the scales D hplltiL 1’. A 2 ,/ ‘EJL / r m g B u. ‘01 C w' x. Fig. 17. are uniform thus permitting more accurate readings and also simp- lifying the construction of the scales. __A_.l’__ #; _. '_.- .‘L— _'__'__‘.&. .3—_n_' __ -39- Consider the figure shown in Figure 18. Scales A and B are parallel to each other, and graduated in accordance with the scale equations: Xu a mufl(u) and 1v = mvf2(v), respectively In a similar manner, scales 0 and D are parallel to each other, and are graduated in accordance with the scale equations: X = m f w and X = m f c w W3” q qt.” The angle between scales A and C may be of any convenient magnitude. Triangles u uOT and vlvOT are similar, hence l X11 3 . 110T Likewise, triangles w Twl and qOT l are similar, hence q 0 Kw - wOT But lenghts uOT . w T; and vOT = qOT. Therefore 0 or muf (u) = mwf3(w) Since ' f1(u)= f3(W) -40- it follows that m = u S Elia V q This means that three moduli may be determined from the given data, but the fourth modulus will be dependent upon the first three. -41- BIBLIOGRAPHY "heinforced Concrete Structures" by Dean Peabody, Jr. "Reinforced Concrete Design Handbook" of the American Concrete InstitutiOn.. The ACI Building Code 1951. (ACI 318-51) "Recommended Practice and Standard Specifications for Concrete and Reinforced Concrete" Joint Committee on Standard Speci- fications for Concrete, and Reinforced Concrete, l9h0. "Nomography" by A. S. Levens. t 1,, . , b... . , '1 5:;6 3'44? ip'fif; T .4 . I ~ - 5e. 'vl.%';'3”357*?‘r .I‘t. {vi/5? _‘ g. A; ‘ 1 ”£538: a. h .w if ‘ 'J’é'" ‘ 2,4: ‘ ‘V‘u '— ”INN; $33 I ' i n n I n b.1- o ‘/ fl 1'. .‘x. »"’I-‘.-' ~“'. in " 'h.\ ’I