πŸ“ CEE335 β€” CHAPTER 1 Β· WORKING STRESS DESIGN

Reinforced Concrete:
Math First. Build Second.

Every formula in RC design exists because of a physical reason. This chapter unpacks each one β€” starting with intuition, building through physics, arriving at equations that feel inevitable. 8 interactive simulations to make everything visual.

MethodWSD (Working Stress)
CodeACI 318 / BNBC
Simulations8 Interactive
Calculators3 Live
LEC 1
Why RC?
LEC 2
Mix Design
LEC 3
Loads & n
LEC 4–5
Geometry
LEC 6
3 Stages
LEC 7
Transformed Β§
LEC 8
k & j
LEC 9+
Design
00 β€” LEC 1 β€” FOUNDATION

Why Reinforced Concrete?

One physical truth explains everything: concrete is strong in compression, terrible in tension. Steel handles both. Put them together where each excels β€” that's RC in one sentence.

🧠 The ruler test: Bend a ruler β€” the top compresses, the bottom stretches. A concrete ruler would snap at the bottom tensile zone. Fix: embed steel exactly where snapping would happen.
⚑ SIM 1 β€” MATERIAL TESTER: COMPRESSION vs TENSION β€” WATCH CONCRETE CRACK & STEEL YIELD
LOAD INTENSITY: 0%
No load applied. Both materials at rest.
πŸͺ¨

Concrete β€” Compression βœ“

Handles crushing loads like stone. All concrete above the neutral axis in a beam is in compression.

f'c = 3,000–5,000 psi
⚠️

Concrete β€” Tension βœ—

Brittle. Tensile strength β‰ˆ 7.5√f'c β‰ˆ f'c/10. Cracks instantly. Cannot be relied upon for tension.

ft β‰ˆ 7.5√f'c psi
πŸ”©

Steel β€” Takes the Tension

Rebar placed in the tension zone carries what concrete cannot. High strength, ductile, bonds perfectly.

fy = 40,000–60,000 psi
πŸ”—

Bond β€” The Secret

Same thermal expansion coefficient. Both strain identically β€” the fundamental compatibility assumption.

Ξ± β‰ˆ 6Γ—10⁻⁢/Β°F for both

Brief History

ANCIENT ROME

Pozzolana Cement

Volcanic ash + lime. The Pantheon dome still stands 2,000 years later.

1796

Portland Cement (Aspdin, England)

Patents modern Portland cement. Same formulation used worldwide today.

1867 β€” KEY DATE

Reinforced Concrete (Monier, France)

Gardener Monier patents iron-reinforced concrete flower pots. Idea scales to beams and skyscrapers.

1920s

Working Stress Design (WSD) Codified

Stresses kept below allowable limits at service loads β€” the method in this chapter.

01 β€” LEC 2 β€” MIX DESIGN & UNIT WEIGHTS

The Recipe Defines the Strength

Concrete is a four-component composite. The ratio of water to cement β€” the w/c ratio β€” is the single most important variable controlling strength.

🌫️

Air (1–2%)

Voids from mixing. Too much reduces strength.

🟫

Cement

Adhesive binder. Portland cement. Hydrates with water.

πŸ’§

Water

Triggers hydration. w/c = most critical ratio.

πŸ–οΈ

Aggregate

Fine sand + coarse. 70–75% of volume.

⚑ SIM 2 β€” w/c RATIO EXPLORER: CHANGE THE WATER/CEMENT RATIO β€” WATCH f'c CHANGE ON THE CURVE
w/c RATIO: 0.50 STRUCTURAL RC
USERATIO C:FA:CAf'c APPROX
Mass concrete1:2:42,500 psi
Structural RC (standard)1:1.5:33,000–4,000 psi
High strengthACI 211 design>5,000 psi
🧱

Plain Concrete

No steel rebar.

wc = 145 pcf
πŸ—οΈ

Reinforced Concrete

Includes rebar weight.

wRC = 150 pcf
02 β€” LEC 3 β€” LOADS & MODULAR RATIO

What Forces Act β€” and Who Carries Them?

WSD uses actual service loads. Safety is built through reduced allowable stresses. First, identify every force. Then, bridge the two-material problem with n.

⬇️

Dead Load (DL)

Permanent: self-weight, finishes. Calculated from unit weights.

🚢

Live Load (LL)

Occupancy: people, furniture. Specified by BNBC/ASCE 7.

40–100 psf typical
πŸ’¨

Wind / Seismic

Lateral loads. Govern tall structures.

WSD PHILOSOPHY
$$f_{actual} \leq f_{allowable} = \frac{f_{ultimate}}{\text{Factor of Safety}}$$
fc,allow = 0.45 f'c  |  fs,allow = 20,000 psi (Gr.40) or 24,000 psi (Gr.60)

Modular Ratio n β€” Bridging Two Materials

🧠 Why n? Steel is ~8–10Γ— stiffer than concrete. At equal strain, the stiffer material carries proportionally more stress. n tells you exactly how much more: 1 inΒ² of steel "behaves like" n inΒ² of concrete.
MODULAR RATIO
$$n = \frac{E_s}{E_c} = \frac{29{,}000{,}000}{57{,}000\sqrt{f'_c}} \quad \text{(round to nearest integer)}$$
⚑ SIM 3 β€” MODULAR RATIO VISUALIZER: SEE HOW n CHANGES WITH f'c AND WHAT IT MEANS PHYSICALLY
f'c (psi): 3000 psi
f'c (psi)Ec (psi)nfc,allowfs,allow (Gr.40)
2,5002,850,000101,12520,000
3,0003,122,00091,35020,000
4,0003,605,00081,80020,000
03 β€” LEC 4–5 β€” BEAM GEOMETRY & CROSS-SECTION

Defining the Beam: d, b, and As

Three dimensions define every RC beam cross-section. The most critical is d, the effective depth β€” the distance from the compression face to the centroid of the steel.

EFFECTIVE DEPTH
$$d = h - \text{cover} - d_{stirrup} - \frac{d_{bar}}{2}$$
Typical cover = 1.5", stirrup β‰ˆ 0.375" (#3), bar radius = db/2. Standard assumption: d β‰ˆ h βˆ’ 2.375"
STEEL RATIO
$$\rho = \frac{A_s}{b \cdot d}$$
ρ typically 0.005–0.018 for structural RC. ρmin = 200/fy (psi). ρmax = 0.75ρb (ACI).
⚑ SIM 4 β€” CROSS-SECTION BUILDER: STEP THROUGH EACH LAYER TO SEE HOW d IS COMPUTED
Click the buttons above to step through how d is calculated layer by layer.
βš™οΈ CALCULATOR 1 β€” COMPUTE d AND ρ FROM SECTION DIMENSIONS
04 β€” LEC 6 β€” THREE STAGES OF LOADING

From Zero Load to Collapse

As moment increases, an RC beam passes through three distinct behavioral stages. WSD designs in Stage II β€” after cracking but well before yielding.

β‘ 

Stage I β€” Uncracked

Concrete handles tension. Full section acts. Neutral axis near center. Linear elastic.

M < Mcr
β‘‘

Stage II β€” Cracked Elastic (WSD)

Concrete cracks in tension. Steel carries all tension. Neutral axis shifts up. Still linear.

WSD operates HERE
β‘’

Stage III β€” Inelastic

Steel yields. Large deflections. Nonlinear. ACI strength design (USD) targets this stage.

Near failure
CRACKING MOMENT CRITERION
$$f_r = 7.5\sqrt{f'_c} \quad \text{(psi)} \quad\Rightarrow\quad M_{cr} = f_r \cdot \frac{I_g}{y_{bottom}}$$
If computed fct > fr, the section is cracked β†’ use Stage II (k & j) analysis
⚑ SIM 5 β€” LOADING STAGES: INCREASE LOAD β€” WATCH CRACKS FORM AND STRESS ZONES EVOLVE
LOAD LEVEL: 0.00 k/ft STAGE I β€” UNCRACKED ELASTIC

Stage I Check

fct = MΒ·y_bot/I_tr
If fct < fr β†’ Stage I OK

Stage II (WSD)

Use cracked section:
k, j method below

Transition

fct > fr β†’ cracked
β†’ Use Stage II
05 β€” LEC 7 β€” THE TRANSFORMED SECTION METHOD

Two Materials, One Section

The flexure formula Οƒ = My/I assumes homogeneous material. RC has two materials. The Transformed Section converts steel into equivalent concrete so we can use the standard formula.

🧠 The key: Since strain is equal at the steel location (compatibility), and steel is n times stiffer, steel carries n times the stress. Replace each As with nAs of concrete β€” now we have one material.
UNCRACKED TRANSFORMED SECTION β€” NEUTRAL AXIS FROM TOP
$$\bar{y} = \frac{b h^2/2 + (n-1)A_s \cdot d}{b h + (n-1)A_s}$$
MOMENT OF INERTIA β€” TRANSFORMED UNCRACKED SECTION
$$I_{tr} = \frac{b h^3}{12} + b h\!\left(\bar{y} - \frac{h}{2}\right)^{\!2} + (n-1)A_s(d - \bar{y})^2$$
⚑ SIM 6 β€” STRESS PROBE: HOVER/CLICK ANYWHERE ON THE CROSS-SECTION TO READ THE STRESS AT THAT DEPTH
M (kΒ·in): 200
Hover over the cross-section to probe the stress at any depth.
NEUTRAL AXIS β€” CRACKED TRANSFORMED SECTION (from top)
$$\frac{b(kd)^2}{2} = n A_s (d - kd) \quad\Longrightarrow\quad k = \sqrt{(\rho n)^2 + 2\rho n} - \rho n$$
06 β€” LEC 8 β€” WSD ANALYSIS: THE k & j METHOD

Cracked Section Analysis β€” Two Numbers Do Everything

Two dimensionless numbers β€” k (neutral axis depth ratio) and j (moment arm ratio) β€” completely define the cracked RC stress state. Here's the derivation and two simulations to make them intuitive.

🧠 Start here: After cracking, only two internal forces exist: C (compression in concrete above N.A.) and T (tension in steel). They must balance: C = T. Their separation (jd) times either force = resisting moment.
kd C = Β½fcΒ·bΒ·kd T = AsΒ·fs d jd

The compression resultant C acts at kd/3 from the top (centroid of triangle). The tension resultant T acts at the steel centroid. Their separation = jd = d βˆ’ kd/3 = d(1 βˆ’ k/3).

M = C Β· jd = (Β½ fc Β· k Β· b Β· d) Β· jd = Β½ fc Β· k Β· j Β· b Β· dΒ²
M = T Β· jd = As Β· fs Β· jd = As Β· fs Β· j Β· d

Compatibility β€” equal strain at steel

Since concrete and steel are bonded, they strain together at the steel level.

$$\frac{\varepsilon_s}{\varepsilon_c} = \frac{d - kd}{kd} \quad\Rightarrow\quad \frac{f_s/E_s}{f_c/E_c} = \frac{1-k}{k} \quad\Rightarrow\quad f_s = n \cdot f_c \cdot \frac{1-k}{k}$$

Equilibrium β€” C = T

Internal compression equals internal tension.

$$C = T \quad\Rightarrow\quad \frac{1}{2}f_c \cdot b \cdot kd = A_s \cdot f_s$$

Substitute and simplify

Replace fs from compatibility into C = T:

$$\frac{1}{2}f_c \cdot b \cdot kd = A_s \cdot n f_c \cdot \frac{1-k}{k}$$
$$\frac{bk^2}{2} = \rho n (1-k) \quad\Rightarrow\quad k^2 + 2\rho n \cdot k - 2\rho n = 0$$

Solve the quadratic

$$k = \sqrt{(\rho n)^2 + 2\rho n} - \rho n$$
$$j = 1 - \frac{k}{3}$$
COMPLETE WSD ANALYSIS FORMULAS
$$k = \sqrt{(\rho n)^2 + 2\rho n} - \rho n \qquad j = 1 - \frac{k}{3}$$ $$f_c = \frac{2M}{k \cdot j \cdot b \cdot d^2} \leq 0.45 f'_c \qquad f_s = \frac{M}{A_s \cdot j \cdot d} \leq f_{s,allow}$$
Where: ρ = As/(bd), n = Es/Ec (integer), M in lb·in, b & d in inches.
βš™οΈ CALCULATOR 2 β€” WSD CRACKED SECTION ANALYSIS
WP-1WSD Analysis β€” Find fs and fc in cracked RC beam

GIVEN

b=12", d=21.5"As=3.0 inΒ² (3-#9)
f'c=3,000 psi, n=9M=200 kΒ·in, fy=40ksi

ρ and ρn

ρ = 3.0/(12Γ—21.5) = 0.01163  |  ρn = 0.1047

k and j

k = √(0.1047Β²+2Γ—0.1047)βˆ’0.1047 = 0.365  |  j = 1βˆ’0.365/3 = 0.878

Stresses

fs = 200,000/(3.0Γ—0.878Γ—21.5) = 3,536 psi βœ“ < 20,000 psi
fc = 2Γ—200,000/(0.365Γ—0.878Γ—12Γ—21.5Β²) = 254 psi βœ“ < 1,350 psi
βœ“ Section OK. Both stresses well below allowables.
⚑ SIM 7 β€” NEUTRAL AXIS VISUALIZER: CHANGE ρ AND n β€” WATCH kd MOVE AND SEE HOW STRESS PROFILE CHANGES
ρ: 0.010
n: 9
Key insight: More steel (↑ρ) or stiffer steel (↑n) pulls the neutral axis deeper. Deeper N.A. = larger compression zone = smaller jd = more force needed for same moment.
⚑ SIM 8 β€” C = T FORCE BALANCE: WATCH COMPRESSION AND TENSION FORCES GROW TOGETHER IN EQUILIBRIUM AS MOMENT INCREASES
M (kΒ·in): 0 Apply moment to see C and T forces
07 β€” LEC 9+ β€” WSD DESIGN PROCEDURE

Design from Scratch

Analysis asks "What are the stresses?" Design asks "What beam do I need?" We work backward from required moment M to find b, d, and As.

🧠 Balanced section: The most efficient beam is one where concrete and steel reach their allowable stresses at exactly the same time β€” the balanced design target.
BALANCED DESIGN CONSTANTS
$$k_b = \frac{n \cdot f_{ca}}{n \cdot f_{ca} + f_{sa}} \qquad j_b = 1 - \frac{k_b}{3} \qquad R = \frac{1}{2} f_{ca} \cdot k_b \cdot j_b$$
R is the "resistance coefficient" in psi. Then: $bd^2 = M/R$ and $A_s = M/(f_{sa} \cdot j_b \cdot d)$

Design Procedure β€” Step by Step

Find design moment M from structural analysis

M = wLΒ²/8 (simply supported UDL)

Compute n, fc,allow, fs,allow from material properties

n = 29,000,000 / (57,000√f'c)  |  fc = 0.45f'c  |  fs = 20,000 (Gr.40)

Balanced kb, jb, R

kb = nΒ·fc/(nΒ·fc + fs)  |  jb = 1βˆ’kb/3  |  R = Β½Β·fcΒ·kbΒ·jb

Required bdΒ²

bdΒ² = M/R β†’ choose b (β‰₯12", even) β†’ solve for d = √(bdΒ²/b)

Round up d β†’ compute h

h = d + cover + dstirrup + dbar/2 β†’ round to nearest Β½"

Required As

As = M/(fsΒ·jΒ·d) β†’ select bars from table

Check bar spacing, cover, actual stresses

Verify bars fit in width b, spacing β‰₯ 1", recompute fs and fc with final d.

βš™οΈ CALCULATOR 3 β€” WSD BEAM DESIGN (FIND b, d, As FROM M)
WP-2WSD Design β€” Design beam for M=80 kΒ·ft (f'c=3ksi, Gr.40, b=12")

GIVEN

M=80 kΒ·ft=960 kΒ·inf'c=3,000 psi, n=9
fc,allow=1,350 psifs,allow=20,000 psi, b=12"

Balanced kb and jb

kb = (9Γ—1350)/(9Γ—1350+20000) = 0.378  |  jb = 1βˆ’0.378/3 = 0.874

R factor

R = Β½Γ—1350Γ—0.378Γ—0.874 = 223 psi

Required bdΒ²

bdΒ² = 960,000/223 = 4,305 inΒ³ β†’ b=12" β†’ d = √(358.8) = 18.94" β†’ use d = 19"

h and As

h = 19+1.5+0.375+0.5 = 21.4" β†’ use h = 22" β†’ actual d = 22βˆ’2.375 = 19.625"
As = 960,000/(20,000Γ—0.874Γ—19.625) = 2.80 inΒ² β†’ Use 4-#8 (As=3.16 inΒ²)
βœ“ Result: b=12", h=22", 4-#8 bars (As=3.16 inΒ²)
πŸ“‹ QUICK REFERENCE

Formula Sheet β€” All RC WSD Formulas

Every formula from this chapter, organized by topic.

Materials
Modular Ratio
$n = E_s/E_c = 29{,}000{,}000\,/\,(57{,}000\sqrt{f'_c})$
Round to nearest integer. f'c in psi.
Materials
Allowable Stresses
$f_{ca} = 0.45\,f'_c \quad f_{sa} = 20{,}000$ (Gr.40) or $24{,}000$ psi (Gr.60)
Geometry
Effective Depth
$d = h - \text{cover} - d_s - d_b/2$
Typical: d β‰ˆ h βˆ’ 2.375"
Geometry
Steel Ratio
$\rho = A_s\,/\,(b\cdot d)$
Typical range: 0.005 – 0.018
Cracking
Modulus of Rupture
$f_r = 7.5\sqrt{f'_c}$ (psi)
If fct > fr β†’ section is cracked β†’ use Stage II
Stage II β€” Cracked
Neutral Axis Ratio k
$k = \sqrt{(\rho n)^2 + 2\rho n} - \rho n$
k = kd/d where kd = neutral axis depth from top
Stage II β€” Cracked
Moment Arm Ratio j
$j = 1 - k/3$
jd = internal moment arm (C to T)
Analysis
Concrete Stress
$f_c = 2M\,/\,(k\,j\,b\,d^2)$
Check: fc ≀ 0.45f'c
Analysis
Steel Stress
$f_s = M\,/\,(A_s\,j\,d)$
Check: fs ≀ fsa
Design
Balanced kb
$k_b = n\,f_{ca}\,/\,(n\,f_{ca} + f_{sa})$
Design
Resistance R
$R = \tfrac{1}{2}\,f_{ca}\,k_b\,j_b$ (psi)
jb = 1 βˆ’ kb/3
Design
Required bdΒ²
$b\,d^2 = M\,/\,R$
Choose b β†’ solve for d β†’ round up β†’ find h
Design
Required As
$A_s = M\,/\,(f_{sa}\,j_b\,d)$
Use actual d after rounding h
Bar Sizes (US)
Common Rebars
#3: 0.375" / 0.11 inΒ²   #4: 0.5" / 0.20
#5: 0.625" / 0.31   #6: 0.75" / 0.44
#7: 0.875" / 0.60   #8: 1.0" / 0.79
#9: 1.128" / 1.00   #10: 1.27" / 1.27