⚖️ Density Conversion Calculator
Convert between kg/m³, g/cm³, g/mL, lb/ft³, lb/gal, oz/in³, t/m³, mg/L and 50+ density units — with fundamental density formula ρ=m/V, specific gravity, Archimedes' principle, buoyancy, API gravity & material density table rendered in MathJax
🔄 Density Unit Converter
🌍 All Units at Once
📖 How to Use This Density Conversion Calculator
-
1Filter by Unit Category (Optional)
Click SI/Metric (kg/m³, g/cm³, g/L, t/m³, mg/L), Imperial/US (lb/ft³, lb/in³, lb/gal, oz/in³), Grain-Based (gr/gal, gr/ft³), or Water Reference (relative to water at 4°C, 20°C, ice) to narrow the dropdowns.
-
2Enter Your Density Value
Type the numeric density value. Accepts any range — from µg/L (trace contaminant analysis) to kg/cm³ (ultra-dense materials like osmium or neutron star crusts).
-
3Select From and To Units
Choose your source unit and target unit. The result and exact conversion factor appear instantly in the lime-green result box.
-
4Use Quick-Convert Buttons
Click presets — kg/m³↔g/cm³, kg/m³↔lb/ft³, g/cm³→lb/ft³, kg/m³→lb/gal, lb/in³→kg/m³ — for the most common density conversions in engineering and laboratory use.
-
5View All Units & Copy
"All Units at Once" shows your density in every supported unit simultaneously. Click "📋 Copy Result" to copy for engineering reports, material datasheets, or quality control documentation.
📐 Density Unit Conversion Reference Table
| From | To | Multiply By | Mathematical Expression |
|---|---|---|---|
| 1 g/cm³ | kg/m³ | 1,000 | \( 1\,\text{g/cm}^3 = 10^3\,\text{kg/m}^3 \) |
| 1 kg/m³ | g/cm³ | 0.001 | \( 1\,\text{kg/m}^3 = 10^{-3}\,\text{g/cm}^3 \) |
| 1 lb/ft³ | kg/m³ | 16.01846 | \( 1\,\text{lb/ft}^3 = 16.01846\,\text{kg/m}^3 \) |
| 1 kg/m³ | lb/ft³ | 0.062428 | \( 1\,\text{kg/m}^3 = 0.062428\,\text{lb/ft}^3 \) |
| 1 lb/in³ | kg/m³ | 27,679.9 | \( 1\,\text{lb/in}^3 = 27{,}679.9\,\text{kg/m}^3 \) |
| 1 lb/gal (US) | kg/m³ | 119.826 | \( 1\,\text{lb/gal (US)} = 119.826\,\text{kg/m}^3 \) |
| 1 t/m³ | kg/m³ | 1,000 | \( 1\,\text{t/m}^3 = 10^3\,\text{kg/m}^3 \) |
| 1 g/L | kg/m³ | 1 | \( 1\,\text{g/L} = 1\,\text{kg/m}^3 \) (exact) |
| 1 mg/L | kg/m³ | 0.001 | \( 1\,\text{mg/L} = 10^{-3}\,\text{kg/m}^3 \) |
| 1 oz/in³ | kg/m³ | 1,729.99 | \( 1\,\text{oz/in}^3 = 1{,}730.0\,\text{kg/m}^3 \) |
⚖️ Understanding Density — A Complete Science & Engineering Guide
Density is one of the most practically important physical properties in science and engineering. It tells you exactly how much mass is packed into a given volume — and this single number determines whether objects float or sink, how structures bear load, whether alloys meet specification, how pharmaceutical tablets dissolve, how petroleum products are graded, and even how oceanographic water masses circulate around the globe driving the entire climate system.
Converting between density units accurately is essential across many disciplines: a materials engineer comparing aluminium alloys in kg/m³ and lb/in³, a chemist measuring solution concentrations in g/mL, a petroleum engineer using API gravity, a water treatment specialist working in mg/L and grains per gallon, and a food scientist measuring ingredient densities in lb/ft³ all need reliable, precise unit conversion. This calculator covers all of them.
📦 Density Unit Systems — SI, CGS, & Imperial Explained
Density is expressed in fundamentally different units depending on the field and region. Understanding what each unit means — and exactly how they relate — prevents costly errors in engineering specifications, chemical formulations, and material procurement.
\( 1\,\text{g/cm}^3 = 1\,\text{g/mL} = 1\,\text{kg/L} = 1\,\text{t/m}^3 = 1000\,\text{kg/m}^3 \quad \text{(all exact)} \)
\( 1\,\text{lb/ft}^3 = 16.01846337...\,\text{kg/m}^3 \quad \text{(from 1 lb = 0.45359237 kg, 1 ft = 0.3048 m)} \)
\( 1\,\text{lb/in}^3 = \frac{0.45359237}{(0.0254)^3} = 27{,}679.904...\,\text{kg/m}^3 \)
\( 1\,\text{lb/gal (US)} = \frac{0.45359237}{3.785411784 \times 10^{-3}} = 119.826\,\text{kg/m}^3 \)
\( 1\,\text{g/L} = 1\,\text{kg/m}^3 = 1\,\text{mg/mL} \quad \text{(exact: 1 L = 10}^{-3}\text{ m}^3\text{)} \)
Problem: AISI 1020 carbon steel has density 7.87 g/cm³. Convert to kg/m³, lb/ft³, and lb/in³.
kg/m³: \( 7.87\,\text{g/cm}^3 \times 1000 = \mathbf{7{,}870\,\text{kg/m}^3} \)
lb/ft³: \( 7{,}870 \div 16.01846 = \mathbf{491.3\,\text{lb/ft}^3} \)
lb/in³: \( 7{,}870 \div 27{,}679.9 = \mathbf{0.2843\,\text{lb/in}^3} \)
Practical use: A steel I-beam with volume 0.05 m³: \( m = \rho V = 7{,}870 \times 0.05 = \mathbf{393.5\,\text{kg}}\). An engineer using lb/ft³ calculates: \(491.3 \times 1.766\,\text{ft}^3 = 867.5\,\text{lb} = 393.5\,\text{kg}\). Same answer — unit conversion done right.
💧 Specific Gravity — Dimensionless Density Ratio
Specific gravity (SG), also called relative density, is the ratio of a substance's density to the density of a reference substance — usually water at 4°C (1,000 kg/m³ = 1 g/cm³) for liquids and solids. Because it is a pure ratio, SG is dimensionless — it has no units. This makes it especially convenient for quick material identification, quality control, and international communication where unit systems differ.
\( SG = \frac{\rho_{\text{substance}}}{\rho_{\text{water at 4°C}}} = \frac{\rho}{1000\,\text{kg/m}^3} \)
\( \rho\,[\text{kg/m}^3] = SG \times 1000 \qquad \rho\,[\text{g/cm}^3] = SG \times 1\,\text{g/cm}^3 \)
\( \text{API gravity} = \frac{141.5}{SG_{60°F}} - 131.5 \qquad \Leftrightarrow \qquad SG = \frac{141.5}{\text{API} + 131.5} \)
\( \text{Baumé (heavy): } {}^{\circ}\text{Bé} = 145 - \frac{145}{SG} \qquad \text{Baumé (light): } {}^{\circ}\text{Bé} = \frac{140}{SG} - 130 \)
🌊 Archimedes' Principle — Buoyancy & Density Measurement
Archimedes' Principle (c. 250 BCE) is the fundamental theorem connecting density and buoyancy: any object immersed in a fluid experiences an upward buoyant force equal to the weight of the fluid it displaces. This principle not only explains floating and sinking but is also the basis of some of the most accurate density measurement techniques used today — including hydrostatic weighing and pycnometry.
\( F_b = \rho_{\text{fluid}} \cdot V_{\text{displaced}} \cdot g \qquad \text{(buoyant force)} \)
\( \text{Object floats if: } \rho_{\text{object}} < \rho_{\text{fluid}} \qquad \text{Object sinks if: } \rho_{\text{object}} > \rho_{\text{fluid}} \)
\( \text{Fraction submerged} = \frac{\rho_{\text{object}}}{\rho_{\text{fluid}}} \qquad \text{(floating equilibrium)} \)
\( \rho_{\text{solid}} = \frac{m_{\text{air}}}{m_{\text{air}} - m_{\text{fluid}}} \cdot \rho_{\text{fluid}} \qquad \text{(hydrostatic weighing — density measurement)} \)
Problem: An iceberg has density 917 kg/m³. What fraction is submerged in seawater (ρ = 1,025 kg/m³)?
\[ \text{Fraction submerged} = \frac{\rho_{\text{ice}}}{\rho_{\text{seawater}}} = \frac{917}{1{,}025} = \mathbf{0.8946} \approx 89.5\% \]
Interpretation: Only ~10.5% of an iceberg protrudes above the ocean surface. The famous "iceberg tip" phenomenon is a direct consequence of density ratios. In fresh water (1,000 kg/m³): fraction = 917/1,000 = 91.7% submerged, so 8.3% above — slightly more visible than in saltwater.
💧 Water Density — Temperature Dependence & the 4°C Maximum
\( \rho_{\text{water}}(4°\text{C}) = 999.9720\,\text{kg/m}^3 \approx 1000\,\text{kg/m}^3 \quad \text{(maximum density)} \)
\( \rho_{\text{water}}(20°\text{C}) = 998.204\,\text{kg/m}^3 \qquad \rho_{\text{water}}(100°\text{C}) = 958.4\,\text{kg/m}^3 \)
\( \rho_{\text{ice}}(0°\text{C}) = 916.8\,\text{kg/m}^3 \qquad \text{(water expands }\approx 9\%\text{ on freezing)} \)
\( \rho_{\text{seawater}} \approx 1020\text{–}1029\,\text{kg/m}^3 \qquad \text{(salinity 33–37 g/kg)} \)
🪨 Material Density Reference Table
| Material | kg/m³ | g/cm³ | lb/ft³ | Notes |
|---|---|---|---|---|
| 🌡️ Air (20°C, 1 atm) | 1.204 | 0.001204 | 0.0752 | Composition-dependent |
| 🌊 Fresh water (4°C) | 999.97 | 1.000 | 62.43 | Maximum density |
| 🌊 Seawater (15°C) | 1,025 | 1.025 | 64.0 | Salinity ~35 g/kg |
| 🧊 Ice (0°C) | 917 | 0.917 | 57.25 | Floats due to low density |
| 🛢️ Petroleum (crude) | 800–900 | 0.80–0.90 | 50–56 | API 25–45° |
| 🪵 Oak wood | 600–900 | 0.6–0.9 | 37–56 | Varies with moisture content |
| 🏗️ Concrete | 2,300–2,400 | 2.30–2.40 | 144–150 | Reinforced: ~2,400 |
| 🧱 Aluminium (pure) | 2,702 | 2.702 | 168.7 | Most-used structural metal |
| 🔩 Iron | 7,874 | 7.874 | 491.5 | Body-centred cubic |
| 🔩 Steel (carbon) | 7,750–8,050 | 7.75–8.05 | 484–503 | Alloy composition varies |
| 🪙 Copper | 8,960 | 8.96 | 559.5 | High conductivity metal |
| 🏗️ Lead | 11,340 | 11.34 | 708.0 | Radiation shielding |
| 🏅 Gold | 19,282 | 19.28 | 1,204 | Denser than most metals |
| ⚫ Osmium (densest element) | 22,590 | 22.59 | 1,410 | Densest naturally occurring element |
🔬 Density Measurement Methods & Applications
Pycnometry — Laboratory Standard
Measures density using a precisely calibrated volume vessel (pycnometer). Accuracy: 0.001–0.0001 g/cm³. Used for liquids (ASTM D1217), solids (ASTM D792), and powders. Formula: \(\rho = m_s \rho_f / (m_s + m_f - m_{sf})\)
Hydrometer — Field & Process Use
Floats in liquid at equilibrium where buoyancy = weight. Reads specific gravity or Baumé scale directly. Used in winemaking (must density), brewing (Plato scale), battery acid (sulfuric acid SG), anti-freeze (ethylene glycol), and seawater salinity.
Vibrating Tube — Process Control
Measures resonant frequency of a U-tube containing the fluid; frequency changes with density. Digital density meters (Anton Paar, Mettler Toledo) achieve ±0.00001 g/cm³. Used in pharmaceutical QC, beverage production, petroleum refining.
X-ray / Gamma Densitometry
Radiation transmission through materials inversely related to density: \(I = I_0 e^{-\mu \rho x}\). Non-invasive; used for measuring concrete density, food product consistency, and pipeline particulate concentration without contact.
💨 Gas Density — Ideal Gas Law
\( PV = nRT \qquad \Rightarrow \qquad \rho_{\text{gas}} = \frac{PM}{RT} \)
\( \rho_{\text{air, STP}} = \frac{101{,}325 \times 0.02897}{8.314 \times 273.15} = \mathbf{1.293\,\text{kg/m}^3} \quad \text{(0°C, 1 atm)} \)
\( \rho_{\text{air, NTP}} = \frac{101{,}325 \times 0.02897}{8.314 \times 293.15} = \mathbf{1.204\,\text{kg/m}^3} \quad \text{(20°C, 1 atm)} \)
\( \rho_2 = \rho_1 \cdot \frac{P_2 T_1}{P_1 T_2} \qquad \text{(scaling gas density with P and T)} \)