C16/20 vs C30/37
C30/37 is 1.1 times as stiff as C16/20. Their densities are about the same. Per unit mass C30/37 is 1.1 times as stiff. Strength: f_ck = 16 MPa for C16/20, f_ck = 30 MPa for C30/37.
Side by side
ratio = C30/37 / C16/20 · log scale| Property | C16/20 | C30/37 | Unit | Ratio | ¼×1×4× |
|---|---|---|---|---|---|
| E Young's modulus | 29 | 33 | GPa | 1.14× | |
| G Shear modulus | 12.08 | 13.75 | GPa | 1.14× | |
| ν Poisson's ratio | 0.2 | 0.2 | – | 1× | |
| ρ Density | 2447 | 2447 | kg/m³ | 1× | |
| γ Weight density | 24 | 24 | kN/m³ | 1× | |
| α Coefficient of thermal expansion | 10 | 10 | 10⁻⁶/K | 1× | |
| f_ck Characteristic cylinder strength | 16 | 30 | MPa | 1.88× | |
| f_ck,cube Characteristic cube strength | 20 | 37 | MPa | 1.85× | |
| f_cm Mean cylinder strength | 24 | 38 | MPa | 1.58× | |
| f_ctm Mean tensile strength | 1.9 | 2.9 | MPa | 1.53× | |
| f_ctk,0.05 Tensile strength, 5 % fractile | 1.3 | 2 | MPa | 1.54× | |
| f_ctk,0.95 Tensile strength, 95 % fractile | 2.5 | 3.8 | MPa | 1.52× | |
| ε_c1 Strain at peak stress | 1.9 | 2.2 | ‰ | 1.16× | |
| ε_cu1 Ultimate strain | 3.5 | 3.5 | ‰ | 1× | |
| ε_c2 Strain at peak, parabola–rectangle | 2 | 2 | ‰ | 1× | |
| ε_cu2 Ultimate strain, parabola–rectangle | 3.5 | 3.5 | ‰ | 1× | |
| n Exponent, parabola–rectangle | 2 | 2 | – | 1× | |
| ε_c3 Strain at peak, bilinear | 1.75 | 1.75 | ‰ | 1× | |
| ε_cu3 Ultimate strain, bilinear | 3.5 | 3.5 | ‰ | 1× | |
| E/ρ Specific stiffness E/ρ · derived | 11.85 | 13.48 | MJ/kg | 1.14× | |
| c₀ Bar wave speed √(E/ρ) · derived | 3442 | 3672 | m/s | 1.07× | |
| f/ρ Specific strength f/ρ · derived | 6.538 | 12.26 | kJ/kg | 1.88× |
Values at the first thickness band or product form of each material (EN 1992-1-1; EN 1992-1-1). A minimum and a characteristic value are not the same kind of number — read the ratio as a guide. Each material's page lists every band and every source.