Eurocode 2 (EN 1992-1-1:2004 + A1:2014 ) approaches column design with a degree of mechanical rigor distinct from American (ACI 318) and Indian (IS 456) standards. In particular, EC2 discards the traditional empirical “moment magnifier” in favor of physically grounded second-order methods: the Nominal Stiffness Method (§5.8.7) and the Nominal Curvature Method (§5.8.8).
This technical whitepaper provides a complete, line-by-line derivation for a braced rectangular RC column carrying heavy axial force and eccentric moments, determining whether second-order effects govern and detailing the required longitudinal bars and transverse confinement links.
Parameter Symbol Design Value Code Citation Column Cross-Section b × h b \times h b × h 300 mm × 300 mm 300\text{ mm} \times 300\text{ mm} 300 mm × 300 mm — Clear Story Height L L L 3.50 m 3.50\text{ m} 3.50 m (3,500 mm 3{,}500\text{ mm} 3 , 500 mm )— Effective Length Factor β \beta β 0.75 0.75 0.75 (semi-rigid beam-slab framing)EN 1992-1-1 §5.8.3.2 Concrete Strength Class C30/37 f c k = 30 MPa f_{ck} = 30\text{ MPa} f c k = 30 MPa , f c d = 20.0 MPa f_{cd} = 20.0\text{ MPa} f c d = 20.0 MPa (α c c = 1.0 , γ c = 1.5 \alpha_{cc} = 1.0, \gamma_c = 1.5 α cc = 1.0 , γ c = 1.5 )Table 3.1 & §3.1.6 Steel Reinforcement B500B f y k = 500 MPa f_{yk} = 500\text{ MPa} f y k = 500 MPa , f y d = 434.8 MPa f_{yd} = 434.8\text{ MPa} f y d = 434.8 MPa (γ s = 1.15 \gamma_s = 1.15 γ s = 1.15 )§3.2.7 Design Axial Force N E d N_{Ed} N E d 950 kN 950\text{ kN} 950 kN (compression)— First-Order Top Moment M 02 M_{02} M 02 45.0 kN ⋅ m 45.0\text{ kN}\cdot\text{m} 45.0 kN ⋅ m — First-Order Bottom Moment M 01 M_{01} M 01 22.5 kN ⋅ m 22.5\text{ kN}\cdot\text{m} 22.5 kN ⋅ m (single curvature)— Concrete Cover to Links c n o m c_{nom} c n o m 30 mm 30\text{ mm} 30 mm (XC3 carbonation exposure)EN 1992-1-1 §4.4.1
2. Slenderness Classification & Limit Verification (§5.8.3)
Effective Length & Slenderness Ratio (λ \lambda λ )
ℓ 0 = β ⋅ L = 0.75 × 3.50 m = 2.625 m = 2,625 mm \ell_0 = \beta \cdot L = 0.75 \times 3.50\text{ m} = 2.625\text{ m} = 2{,}625\text{ mm} ℓ 0 = β ⋅ L = 0.75 × 3.50 m = 2.625 m = 2 , 625 mm
Radius of gyration for a square section:
i = h 12 = 300 12 = 86.60 mm i = \frac{h}{\sqrt{12}} = \frac{300}{\sqrt{12}} = 86.60\text{ mm} i = 12 h = 12 300 = 86.60 mm
Slenderness ratio:
λ = ℓ 0 i = 2,625 mm 86.60 mm = 30.31 \lambda = \frac{\ell_0}{i} = \frac{2{,}625\text{ mm}}{86.60\text{ mm}} = 30.31 λ = i ℓ 0 = 86.60 mm 2 , 625 mm = 30.31
Limiting Slenderness (λ l i m \lambda_{lim} λ l im ) per Equation (5.13N)
Second-order effects may be neglected if λ ≤ λ l i m \lambda \leq \lambda_{lim} λ ≤ λ l im :
λ l i m = 20 ⋅ A ⋅ B ⋅ C n \lambda_{lim} = \frac{20 \cdot A \cdot B \cdot C}{\sqrt{n}} λ l im = n 20 ⋅ A ⋅ B ⋅ C
Where:
Relative Axial Force:
n = N E d A c ⋅ f c d = 950 × 10 3 N ( 300 × 300 mm 2 ) × 20.0 N/mm 2 = 950,000 1,800,000 = 0.528 n = \frac{N_{Ed}}{A_c \cdot f_{cd}} = \frac{950 \times 10^3\text{ N}}{(300 \times 300\text{ mm}^2) \times 20.0\text{ N/mm}^2} = \frac{950{,}000}{1{,}800{,}000} = 0.528 n = A c ⋅ f c d N E d = ( 300 × 300 mm 2 ) × 20.0 N/mm 2 950 × 1 0 3 N = 1 , 800 , 000 950 , 000 = 0.528
Creep Factor A A A : If effective creep ratio φ e f \varphi_{ef} φ e f is not explicitly calculated, §5.8.3.1 allows A = 0.7 A = 0.7 A = 0.7 .
Mechanical Reinforcement Factor B B B : If ω \omega ω is unknown, B = 1.1 B = 1.1 B = 1.1 .
Moment Ratio Factor C C C :
r m = M 01 M 02 = 22.5 45.0 = 0.50 ⟹ C = 1.7 − r m = 1.7 − 0.50 = 1.20 r_m = \frac{M_{01}}{M_{02}} = \frac{22.5}{45.0} = 0.50 \implies C = 1.7 - r_m = 1.7 - 0.50 = 1.20 r m = M 02 M 01 = 45.0 22.5 = 0.50 ⟹ C = 1.7 − r m = 1.7 − 0.50 = 1.20
Evaluate λ l i m \lambda_{lim} λ l im :
λ l i m = 20 × 0.7 × 1.1 × 1.20 0.528 = 18.48 0.7266 = 25.43 \lambda_{lim} = \frac{20 \times 0.7 \times 1.1 \times 1.20}{\sqrt{0.528}} = \frac{18.48}{0.7266} = 25.43 λ l im = 0.528 20 × 0.7 × 1.1 × 1.20 = 0.7266 18.48 = 25.43
λ = 30.31 > λ l i m = 25.43 ⟹ Slender Column: Second-order moments MUST be calculated. \lambda = 30.31 > \lambda_{lim} = 25.43 \implies \textbf{Slender Column: Second-order moments MUST be calculated.} λ = 30.31 > λ l im = 25.43 ⟹ Slender Column: Second-order moments MUST be calculated.
3. Second-Order Analysis: Nominal Curvature Method (§5.8.8)
Total design moment along the column length:
M E d = M 0 E d + M 2 M_{Ed} = M_{0Ed} + M_2 M E d = M 0 E d + M 2
First-Order Equivalent Design Moment (M 0 E d M_{0Ed} M 0 E d ) per Eq. (5.32)
M 0 E d = max ( 0.6 M 02 + 0.4 M 01 , 0.4 M 02 ) M_{0Ed} = \max\left(0.6 \, M_{02} + 0.4 \, M_{01}, \; 0.4 \, M_{02}\right) M 0 E d = max ( 0.6 M 02 + 0.4 M 01 , 0.4 M 02 )
M 0 E d = max ( 0.6 ( 45.0 ) + 0.4 ( 22.5 ) , 0.4 ( 45.0 ) ) = max ( 27.0 + 9.0 , 18.0 ) = 36.0 kN ⋅ m M_{0Ed} = \max\left(0.6(45.0) + 0.4(22.5), \; 0.4(45.0)\right) = \max(27.0 + 9.0, \; 18.0) = 36.0\text{ kN}\cdot\text{m} M 0 E d = max ( 0.6 ( 45.0 ) + 0.4 ( 22.5 ) , 0.4 ( 45.0 ) ) = max ( 27.0 + 9.0 , 18.0 ) = 36.0 kN ⋅ m
Nominal Curvature 1 r \dfrac{1}{r} r 1 per Eq. (5.34)
1 r = K r ⋅ K φ ⋅ 1 r 0 \frac{1}{r} = K_r \cdot K_\varphi \cdot \frac{1}{r_0} r 1 = K r ⋅ K φ ⋅ r 0 1
Where:
Effective depth d ≈ h − c n o m − ϕ l i n k − ϕ b a r 2 = 300 − 30 − 8 − 10 = 252 mm d \approx h - c_{nom} - \phi_{link} - \dfrac{\phi_{bar}}{2} = 300 - 30 - 8 - 10 = 252\text{ mm} d ≈ h − c n o m − ϕ l ink − 2 ϕ ba r = 300 − 30 − 8 − 10 = 252 mm .
Basic curvature:
1 r 0 = ε y d 0.45 d = f y d / E s 0.45 d = 434.8 / ( 200,000 ) 0.45 × 252 = 0.002174 113.4 = 1.917 × 10 − 5 mm − 1 \frac{1}{r_0} = \frac{\varepsilon_{yd}}{0.45 \, d} = \frac{f_{yd} / E_s}{0.45 \, d} = \frac{434.8 / (200{,}000)}{0.45 \times 252} = \frac{0.002174}{113.4} = 1.917 \times 10^{-5}\text{ mm}^{-1} r 0 1 = 0.45 d ε y d = 0.45 d f y d / E s = 0.45 × 252 434.8/ ( 200 , 000 ) = 113.4 0.002174 = 1.917 × 1 0 − 5 mm − 1
Axial correction factor K r K_r K r (Eq. 5.36):
K r = n u − n n u − n b a l ≤ 1.0 K_r = \frac{n_u - n}{n_u - n_{bal}} \leq 1.0 K r = n u − n ba l n u − n ≤ 1.0
With n u = 1 + ω ≈ 1 + 0.35 = 1.35 n_u = 1 + \omega \approx 1 + 0.35 = 1.35 n u = 1 + ω ≈ 1 + 0.35 = 1.35 , n b a l ≈ 0.40 n_{bal} \approx 0.40 n ba l ≈ 0.40 :
K r = 1.35 − 0.528 1.35 − 0.40 = 0.822 0.950 = 0.865 K_r = \frac{1.35 - 0.528}{1.35 - 0.40} = \frac{0.822}{0.950} = 0.865 K r = 1.35 − 0.40 1.35 − 0.528 = 0.950 0.822 = 0.865
Creep factor K φ = 1.0 K_\varphi = 1.0 K φ = 1.0 (conservative for standard environmental exposures).
1 r = 0.865 × 1.0 × 1.917 × 10 − 5 = 1.658 × 10 − 5 mm − 1 \frac{1}{r} = 0.865 \times 1.0 \times 1.917 \times 10^{-5} = 1.658 \times 10^{-5}\text{ mm}^{-1} r 1 = 0.865 × 1.0 × 1.917 × 1 0 − 5 = 1.658 × 1 0 − 5 mm − 1
Second-Order Deflection e 2 e_2 e 2 & Moment M 2 M_2 M 2 (Eq. 5.33)
For a constant/parabolic first-order moment diagram, c = 10 ≈ π 2 c = 10 \approx \pi^2 c = 10 ≈ π 2 :
e 2 = 1 r ⋅ ℓ 0 2 c = 1.658 × 10 − 5 mm − 1 × ( 2,625 mm ) 2 10 = 1.658 × 10 − 5 × 689,062.5 = 11.42 mm e_2 = \frac{1}{r} \cdot \frac{\ell_0^2}{c} = 1.658 \times 10^{-5}\text{ mm}^{-1} \times \frac{(2{,}625\text{ mm})^2}{10} = 1.658 \times 10^{-5} \times 689{,}062.5 = 11.42\text{ mm} e 2 = r 1 ⋅ c ℓ 0 2 = 1.658 × 1 0 − 5 mm − 1 × 10 ( 2 , 625 mm ) 2 = 1.658 × 1 0 − 5 × 689 , 062.5 = 11.42 mm
M 2 = N E d ⋅ e 2 = 950 kN × 0.01142 m = 10.85 kN ⋅ m M_2 = N_{Ed} \cdot e_2 = 950\text{ kN} \times 0.01142\text{ m} = 10.85\text{ kN}\cdot\text{m} M 2 = N E d ⋅ e 2 = 950 kN × 0.01142 m = 10.85 kN ⋅ m
Minimum Eccentricity Check (§6.1(4))
e 0 = max ( h 30 , 20 mm ) = max ( 10 mm , 20 mm ) = 20 mm e_0 = \max\left(\frac{h}{30}, \; 20\text{ mm}\right) = \max(10\text{ mm}, \; 20\text{ mm}) = 20\text{ mm} e 0 = max ( 30 h , 20 mm ) = max ( 10 mm , 20 mm ) = 20 mm
M 0 , m i n = N E d ⋅ e 0 = 950 kN × 0.020 m = 19.0 kN ⋅ m M_{0,min} = N_{Ed} \cdot e_0 = 950\text{ kN} \times 0.020\text{ m} = 19.0\text{ kN}\cdot\text{m} M 0 , min = N E d ⋅ e 0 = 950 kN × 0.020 m = 19.0 kN ⋅ m
Total Governing Design Moment
M E d , t o t = M 0 E d + M 2 = 36.0 + 10.85 = 46.85 kN ⋅ m ( > M 0 , m i n ) M_{Ed,tot} = M_{0Ed} + M_2 = 36.0 + 10.85 = \mathbf{46.85\text{ kN}\cdot\text{m}} \quad (> M_{0,min}) M E d , t o t = M 0 E d + M 2 = 36.0 + 10.85 = 46.85 kN ⋅ m ( > M 0 , min )
4. Cross-Section Resistance & P-M Interaction (§6.1)
Dimensionless design coordinates:
ν = N E d A c f c d = 0.528 \nu = \frac{N_{Ed}}{A_c f_{cd}} = 0.528 ν = A c f c d N E d = 0.528
μ = M E d , t o t A c f c d h = 46.85 × 10 6 ( 300 × 300 ) × 20.0 × 300 = 46.85 × 10 6 540 × 10 6 = 0.0868 \mu = \frac{M_{Ed,tot}}{A_c f_{cd} h} = \frac{46.85 \times 10^6}{(300 \times 300) \times 20.0 \times 300} = \frac{46.85 \times 10^6}{540 \times 10^6} = 0.0868 μ = A c f c d h M E d , t o t = ( 300 × 300 ) × 20.0 × 300 46.85 × 1 0 6 = 540 × 1 0 6 46.85 × 1 0 6 = 0.0868
Using Eurocode 2 non-dimensional design charts for symmetrical reinforcement (d 2 / h = 48 / 300 = 0.16 d_2/h = 48/300 = 0.16 d 2 / h = 48/300 = 0.16 ):
At ν = 0.528 \nu = 0.528 ν = 0.528 and μ = 0.0868 \mu = 0.0868 μ = 0.0868 , the required mechanical reinforcement ratio is:
ω r e q ≈ 0.180 \omega_{req} \approx 0.180 ω r e q ≈ 0.180
Total required steel area:
A s = ω r e q ⋅ A c f c d f y d = 0.180 × 90,000 × 20.0 434.8 = 0.180 × 4,140 = 745.2 mm 2 A_s = \omega_{req} \cdot \frac{A_c f_{cd}}{f_{yd}} = 0.180 \times \frac{90{,}000 \times 20.0}{434.8} = 0.180 \times 4{,}140 = \mathbf{745.2\text{ mm}^2} A s = ω r e q ⋅ f y d A c f c d = 0.180 × 434.8 90 , 000 × 20.0 = 0.180 × 4 , 140 = 745.2 mm 2
Code Reinforcement Limits (§9.5.2)
Minimum Steel Area:
A s , m i n = max ( 0.10 N E d f y d , 0.002 A c ) = max ( 0.10 × 950,000 434.8 , 0.002 × 90,000 ) = max ( 218.5 , 180.0 ) = 218.5 mm 2 A_{s,min} = \max\left(\frac{0.10 N_{Ed}}{f_{yd}}, \; 0.002 A_c\right) = \max\left(\frac{0.10 \times 950{,}000}{434.8}, \; 0.002 \times 90{,}000\right) = \max(218.5, \; 180.0) = 218.5\text{ mm}^2 A s , min = max ( f y d 0.10 N E d , 0.002 A c ) = max ( 434.8 0.10 × 950 , 000 , 0.002 × 90 , 000 ) = max ( 218.5 , 180.0 ) = 218.5 mm 2
Maximum Steel Area:
A s , m a x = 0.04 A c = 0.04 × 90,000 = 3,600 mm 2 ( outside lap zones ) A_{s,max} = 0.04 A_c = 0.04 \times 90{,}000 = 3{,}600\text{ mm}^2 \quad (\text{outside lap zones}) A s , ma x = 0.04 A c = 0.04 × 90 , 000 = 3 , 600 mm 2 ( outside lap zones )
Selection:
Provide 4 × ϕ 16 mm 4 \times \phi 16\text{ mm} 4 × ϕ 16 mm bars (one in each corner):
A s , p r o v = 4 × 201.1 = 804.4 mm 2 > 745.2 mm 2 A_{s,prov} = 4 \times 201.1 = \mathbf{804.4\text{ mm}^2} > 745.2\text{ mm}^2 A s , p r o v = 4 × 201.1 = 804.4 mm 2 > 745.2 mm 2
(D/C = 0.93 — Verified Pass ✓)
5. Transverse Confinement Reinforcement (§9.5.3)
Minimum Link Diameter:
ϕ l i n k ≥ max ( 6 mm , ϕ l o n g , m a x 4 = 16 4 = 4 mm ) ⟹ Use ϕ 8 mm \phi_{link} \geq \max\left(6\text{ mm}, \; \frac{\phi_{long,max}}{4} = \frac{16}{4} = 4\text{ mm}\right) \implies \text{Use } \mathbf{\phi 8\text{ mm}} ϕ l ink ≥ max ( 6 mm , 4 ϕ l o n g , ma x = 4 16 = 4 mm ) ⟹ Use ϕ 8 mm
Maximum Longitudinal Spacing (s c l , t m a x s_{cl,tmax} s c l , t ma x ):
s m a x = min ( 20 × ϕ l o n g , m i n , b , 400 mm ) = min ( 20 × 16 = 320 , 300 , 400 ) = 300 mm s_{max} = \min\left(20 \times \phi_{long,min}, \; b, \; 400\text{ mm}\right) = \min(20 \times 16 = 320, \; 300, \; 400) = 300\text{ mm} s ma x = min ( 20 × ϕ l o n g , min , b , 400 mm ) = min ( 20 × 16 = 320 , 300 , 400 ) = 300 mm
Critical Regions (near beam-column joints, §9.5.3(6)):
Reduce spacing by factor 0.6 0.6 0.6 :
s j o i n t = 0.6 × 300 = 180 mm ⟹ Provide ϕ 8 mm @ 150 mm o.c. s_{joint} = 0.6 \times 300 = 180\text{ mm} \implies \text{Provide } \mathbf{\phi 8\text{ mm} @ 150\text{ mm} \text{ o.c.}} s j o in t = 0.6 × 300 = 180 mm ⟹ Provide ϕ 8 mm @150 mm o.c.
Summary of Design Output
Design Metric Governing Value Status Applied Axial Load N E d N_{Ed} N E d 950 kN 950\text{ kN} 950 kN Applied Governing Total Moment M E d , t o t M_{Ed,tot} M E d , t o t 46.85 kN ⋅ m 46.85\text{ kN}\cdot\text{m} 46.85 kN ⋅ m (incl. 10.85 kN ⋅ m 10.85\text{ kN}\cdot\text{m} 10.85 kN ⋅ m second-order)Governs Main Reinforcement 4 × ϕ 16 mm 4 \times \phi 16\text{ mm} 4 × ϕ 16 mm corner bars (A s = 804 mm 2 A_s = 804\text{ mm}^2 A s = 804 mm 2 )PASS (D/C = 0.93) ✓ Transverse Links ϕ 8 mm @ 150 mm \phi 8\text{ mm} @ 150\text{ mm} ϕ 8 mm @150 mm joint / 250 mm 250\text{ mm} 250 mm mid-heightPASS ✓
Run Full Interaction Checks in Civora
Civora generates complete 200-point P-M interaction surfaces, tests biaxial bending under Bresler contour equations, and outputs submission-ready drawings in seconds.
Download 8-Page Sample Engineering Report (PDF)
Open Civora Column Studio in Browser →