π 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
π Quick Formula Sheet at the bottom β all RC WSD formulas in one placeJump β
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.
π§ 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.
β‘ SIM 1 β MATERIAL TESTER: COMPRESSION vs TENSION β WATCH CONCRETE CRACK & STEEL YIELD
LOAD INTENSITY:0%
No load applied. Both materials at rest.
πͺ¨
Concrete β Compression β
Handles crushing loads like stone. All concrete above the neutral axis in a beam is in compression.
f'c = 3,000β5,000 psi
β οΈ
Concrete β Tension β
Brittle. Tensile strength β 7.5βf'c β f'c/10. Cracks instantly. Cannot be relied upon for tension.
Rebar placed in the tension zone carries what concrete cannot. High strength, ductile, bonds perfectly.
fy = 40,000β60,000 psi
π
Bond β The Secret
Same thermal expansion coefficient. Both strain identically β the fundamental compatibility assumption.
Ξ± β 6Γ10β»βΆ/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.
π«οΈ
Air (1β2%)
Voids from mixing. Too much reduces strength.
π«
Cement
Adhesive binder. Portland cement. Hydrates with water.
π§
Water
Triggers hydration. w/c = most critical ratio.
ποΈ
Aggregate
Fine sand + coarse. 70β75% of volume.
β‘ SIM 2 β w/c RATIO EXPLORER: CHANGE THE WATER/CEMENT RATIO β WATCH f'c CHANGE ON THE CURVE
w/c RATIO:0.50STRUCTURAL RC
USE
RATIO C:FA:CA
f'c APPROX
Mass concrete
1:2:4
2,500 psi
Structural RC (standard)
1:1.5:3
3,000β4,000 psi
High strength
ACI 211 design
>5,000 psi
π§±
Plain Concrete
No steel rebar.
wc = 145 pcf
ποΈ
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.
β¬οΈ
Dead Load (DL)
Permanent: self-weight, finishes. Calculated from unit weights.
πΆ
Live Load (LL)
Occupancy: people, furniture. Specified by BNBC/ASCE 7.
40β100 psf typical
π¨
Wind / Seismic
Lateral loads. Govern tall structures.
WSD PHILOSOPHY
$$f_{actual} \leq f_{allowable} = \frac{f_{ultimate}}{\text{Factor of Safety}}$$
π§ Why n? Steel is ~8β10Γ 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
$$n = \frac{E_s}{E_c} = \frac{29{,}000{,}000}{57{,}000\sqrt{f'_c}} \quad \text{(round to nearest integer)}$$
β‘ SIM 3 β MODULAR RATIO VISUALIZER: SEE HOW n CHANGES WITH f'c AND WHAT IT MEANS PHYSICALLY
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 0.375" (#3), bar radius = db/2. Standard assumption: d β h β 2.375"
STEEL RATIO
$$\rho = \frac{A_s}{b \cdot d}$$
Ο typically 0.005β0.018 for structural RC. Οmin = 200/fy (psi). Οmax = 0.75Οb (ACI).
β‘ 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.
βοΈ CALCULATOR 1 β COMPUTE d AND Ο 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.
If computed fct > fr, the section is cracked β use Stage II (k & j) analysis
β‘ SIM 5 β LOADING STAGES: INCREASE LOAD β WATCH CRACKS FORM AND STRESS ZONES EVOLVE
LOAD LEVEL:0.00 k/ftSTAGE 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 Ο = My/I assumes homogeneous material. RC has two materials. The Transformed Section converts steel into equivalent concrete so we can use the standard formula.
π§ 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
$$\frac{b(kd)^2}{2} = n A_s (d - kd) \quad\Longrightarrow\quad k = \sqrt{(\rho n)^2 + 2\rho n} - \rho n$$
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.
π§ 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.
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 β kd/3 = d(1 β 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.
fc = 2Γ200,000/(0.365Γ0.878Γ12Γ21.5Β²) = 254 psi β < 1,350 psi
β Section OK. Both stresses well below allowables.
β‘ SIM 7 β NEUTRAL AXIS VISUALIZER: CHANGE Ο AND n β WATCH kd MOVE AND SEE HOW STRESS PROFILE CHANGES
Ο:0.010
n:9
Key insight: More steel (βΟ) or stiffer steel (βn) pulls the neutral axis deeper. Deeper N.A. = larger compression zone = smaller jd = more force needed for same moment.
β‘ SIM 8 β C = T FORCE BALANCE: WATCH COMPRESSION AND TENSION FORCES GROW TOGETHER IN EQUILIBRIUM AS MOMENT INCREASES
M (kΒ·in):0Apply 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.
π§ 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.