GL28h vs GL32h
GL32h is 1.1 times as stiff as GL28h. Their densities are about the same. Per unit mass they are about equally stiff (27.39 and 28.98 MJ/kg). Strength: f_m,k = 28 MPa for GL28h, f_m,k = 32 MPa for GL32h.
Side by side
ratio = GL32h / GL28h · log scale| Property | GL28h | GL32h | Unit | Ratio | ¼×1×4× |
|---|---|---|---|---|---|
| E₁ Modulus, direction 1 | 12.6 | 14.2 | GPa | 1.13× | |
| E₂ Modulus, direction 2 | 0.3 | 0.3 | GPa | 1× | |
| E₃ Modulus, direction 3 | 0.3 | 0.3 | GPa | 1× | |
| G₁₂ Shear modulus 1-2 | 0.65 | 0.65 | GPa | 1× | |
| G₁₃ Shear modulus 1-3 | 0.65 | 0.65 | GPa | 1× | |
| G₂₃ Shear modulus 2-3 | 0.065 | 0.065 | GPa | 1× | |
| E₀,₀₅ Modulus parallel to grain, 5 % fractile | 10.5 | 11.8 | GPa | 1.12× | |
| E₉₀,₀₅ Modulus perpendicular to grain, 5 % fractile | 0.25 | 0.25 | GPa | 1× | |
| G₀₅ Shear modulus, 5 % fractile | 0.54 | 0.54 | GPa | 1× | |
| G_r Rolling shear modulus | 0.065 | 0.065 | GPa | 1× | |
| ρ Density | 460 | 490 | kg/m³ | 1.07× | |
| ρ_k Density, characteristic (5 % fractile) | 425 | 440 | kg/m³ | 1.04× | |
| f_m,k Bending strength | 28 | 32 | MPa | 1.14× | |
| f_t,0,k Tension parallel to grain | 22.3 | 25.6 | MPa | 1.15× | |
| f_t,90,k Tension perpendicular to grain | 0.5 | 0.5 | MPa | 1× | |
| f_c,0,k Compression parallel to grain | 28 | 32 | MPa | 1.14× | |
| f_c,90,k Compression perpendicular to grain | 2.5 | 2.5 | MPa | 1× | |
| f_v,k Shear strength | 3.5 | 3.5 | MPa | 1× | |
| f_r,k Rolling shear strength | 1.2 | 1.2 | MPa | 1× | |
| E/ρ Specific stiffness E/ρ · derived | 27.39 | 28.98 | MJ/kg | 1.06× | |
| c₀ Bar wave speed √(E/ρ) · derived | 5234 | 5383 | m/s | 1.03× | |
| f/ρ Specific strength f/ρ · derived | 60.87 | 65.31 | kJ/kg | 1.07× |
Values at the first thickness band or product form of each material (EN 14080:2013; EN 14080:2013). 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.