🌊 Dynamic Viscosity Conversion Calculator
Convert between pascal seconds, poise, centipoise, mPa·s, reyn and 20+ dynamic viscosity units — SI, CGS & Imperial — with Poiseuille & Navier–Stokes formulas
🔄 Dynamic Viscosity Converter
📊 All Units at Once
📖 How to Use the Dynamic Viscosity Converter
-
1Filter by Unit System (Optional)
Click SI Units, CGS (Poise), or Imperial to narrow the dropdown to units from that system. Click "All Units" to see every available viscosity unit across all systems.
-
2Enter Your Viscosity Value
Type your viscosity number into the "Enter Value" field. Both very small values (e.g., 0.0182 for air in cP) and very large values (e.g., 250,000 for peanut butter in cP) are supported. Results update live.
-
3Select Source & Target Units
Choose your input unit from "From Unit" and the desired output unit from "To Unit." The exact conversion result and multiplication factor appear instantly in the dark result panel.
-
4Use Quick-Convert Buttons
Click a preset button (Pa·s→P, cP→Pa·s, P→Pa·s, etc.) for the most common viscosity conversions. Both dropdowns are pre-set and the answer appears immediately.
-
5View All Units & Copy
The "All Units at Once" panel displays your viscosity value simultaneously in every supported unit. Click "📋 Copy Result" to copy the primary conversion to your clipboard.
📐 Dynamic Viscosity Conversion Factors
| From | To | Multiply By | Math Expression |
|---|---|---|---|
| 1 Pa·s | Poise (P) | 10 | \( 1\,\text{Pa·s} = 10\,\text{P} \) |
| 1 Pa·s | Centipoise (cP) | 1,000 | \( 1\,\text{Pa·s} = 10^3\,\text{cP} \) |
| 1 Pa·s | mPa·s | 1,000 | \( 1\,\text{Pa·s} = 10^3\,\text{mPa·s} \) |
| 1 Poise (P) | Pa·s | 0.1 | \( 1\,\text{P} = 10^{-1}\,\text{Pa·s} \) |
| 1 Centipoise (cP) | Pa·s | 0.001 | \( 1\,\text{cP} = 10^{-3}\,\text{Pa·s} \) |
| 1 cP | mPa·s | 1 (exact) | \( 1\,\text{cP} = 1\,\text{mPa·s} \) |
| 1 kg/(m·s) | Pa·s | 1 (exact) | \( 1\,\text{kg/(m·s)} = 1\,\text{Pa·s} \) |
| 1 lb/(ft·s) | Pa·s | 1.48816 | \( 1\,\text{lb/(ft·s)} \approx 1.488\,\text{Pa·s} \) |
| 1 lbf·s/ft² | Pa·s | 47.8803 | \( 1\,\text{lbf·s/ft}^2 \approx 47.88\,\text{Pa·s} \) |
| 1 reyn | Pa·s | 6,894.76 | \( 1\,\text{reyn} = 1\,\text{lbf·s/in}^2 \approx 6{,}895\,\text{Pa·s} \) |
| 1 kgf·s/m² | Pa·s | 9.80665 | \( 1\,\text{kgf·s/m}^2 = g_n \approx 9.807\,\text{Pa·s} \) |
🌊 Understanding Dynamic Viscosity — A Complete Guide
Dynamic viscosity — also called absolute viscosity — is one of the most important physical properties of any fluid. It quantifies a fluid's internal resistance to deformation under an applied shear stress: in simple terms, how "thick" or "resistant to flow" a fluid is. Understanding viscosity is fundamental to fluid mechanics, chemical engineering, petroleum engineering, food science, biomedical applications, and countless other disciplines.
The challenge for engineers, scientists, and technicians is that viscosity is expressed in a variety of units across different measurement systems — pascal seconds (Pa·s) in SI, poise (P) and centipoise (cP) in the CGS system, and several obscure imperial units like the reyn. Our Num8ers dynamic viscosity converter handles over 20 units instantly, with all conversion factors traceable to internationally defined physical constants.
This equation, formulated by Isaac Newton in 1687, defines what we mean by dynamic viscosity. A fluid with high \(\mu\) requires a large shear stress to produce a given shear rate — it resists flow. A fluid with low \(\mu\) flows easily under small stresses. The SI unit of shear stress is the pascal (Pa = N/m²) and the shear rate is in s⁻¹, so the SI unit of dynamic viscosity is Pa·s = N·s/m² = kg/(m·s).
📐 SI Dynamic Viscosity Units
Pascal Second (Pa·s)
The SI base unit of dynamic viscosity. Water at 20°C ≈ 0.001 Pa·s. Honey: 2–10 Pa·s. Motor oil SAE 30: 0.15–0.20 Pa·s. Glass (at room temperature): ≈ \(10^{21}\) Pa·s!
Millipascal Second (mPa·s)
1 mPa·s = 0.001 Pa·s = 1 cP (exactly). Convenient for low-viscosity fluids. Water ≈ 1 mPa·s at 20°C. Used in clinical/pharmaceutical contexts alongside cP.
kg/(m·s)
Identical to Pa·s by dimensional analysis: \(\text{Pa} = \text{kg/(m·s}^2)\), so \(\text{Pa·s} = \text{kg/(m·s)}\). Sometimes written in fundamental SI base units to make dimensional analysis explicit.
kgf·s/m² — Technical Unit
Uses kilogram-force instead of newton: \(1\,\text{kgf·s/m}^2 = 9.80665\,\text{Pa·s}\) (exactly, using standard gravity \(g_n\)). Used in older German and Italian engineering literature.
🧪 CGS Viscosity Units — Poise & Centipoise
Before SI, the CGS (centimetre-gram-second) system was the dominant scientific measurement system. In CGS, the unit of dynamic viscosity is the poise (P), named after the French physicist Jean Léonard Marie Poiseuille (1797–1869), whose experimental and theoretical work on viscous flow through capillary tubes laid the groundwork for modern fluid mechanics.
The poise is defined in CGS units as \(1\,\text{P} = 1\,\text{g/(cm·s)} = 1\,\text{dyn·s/cm}^2\). Since 1 Pa = 10 dyn/cm², and 1 m = 100 cm, the relationship is: \(1\,\text{P} = 0.1\,\text{Pa·s}\). The centipoise (cP) — one hundredth of a poise — became vastly more common because it gives water a convenient viscosity of approximately 1 cP at 20°C.
🔧 Imperial & Engineering Viscosity Units
Several imperial viscosity units remain in use in American engineering practice, particularly in the petroleum, aerospace, and mechanical engineering sectors. These units are based on the pound-force (lbf), pound-mass (lb), foot (ft), inch (in), and second (s) — and their conversions to SI involve the exact 1959 inch definition and standard gravity \(g_n = 9.80665\,\text{m/s}^2\).
\( 1\,\text{lb/(ft·s)} = 1.48816\,\text{Pa·s} \quad \text{(slug-related, used in aerodynamics)} \)
\( 1\,\text{lbf·s/ft}^2 = 47.8803\,\text{Pa·s} \quad \text{(force-based)} \)
\( 1\,\text{reyn} = 1\,\text{lbf·s/in}^2 = 6{,}894.76\,\text{Pa·s} \quad \text{(named after Osborne Reynolds)} \)
🌀 Navier–Stokes Equations & Viscosity
Dynamic viscosity \(\mu\) appears directly in the Navier–Stokes equations — the governing equations of fluid motion, which were developed by Claude-Louis Navier (1827) and George Gabriel Stokes (1845). For an incompressible Newtonian fluid:
⚖️ Dynamic vs Kinematic Viscosity
Dynamic viscosity \(\mu\) and kinematic viscosity \(\nu\) are closely related but measure different aspects of fluid flow. Dynamic viscosity (also called absolute viscosity) measures the force required to shear a fluid at a given rate — it is relevant when external forces drive flow (e.g., pump pressure). Kinematic viscosity additionally accounts for the fluid's density — it is relevant for flows driven by gravity or inertia.
Given: Water at 20°C: \(\mu = 1.002\,\text{mPa·s} = 1.002 \times 10^{-3}\,\text{Pa·s}\), \(\rho = 998.2\,\text{kg/m}^3\)
\[ \nu = \frac{\mu}{\rho} = \frac{1.002 \times 10^{-3}}{998.2} = 1.004 \times 10^{-6}\,\text{m}^2/\text{s} = 1.004\,\text{cSt (centistokes)} \]
Answer: Water at 20°C has a kinematic viscosity of approximately 1.004 cSt — very close to 1 centistoke, which makes water the calibration reference for kinematic viscosity.
🌀 Reynolds Number — Viscosity in Flow Regime Classification
The Reynolds number (Re) is a dimensionless quantity that characterises whether a flow is laminar (smooth, orderly) or turbulent (chaotic). It is a ratio of inertial forces to viscous forces, and dynamic viscosity \(\mu\) appears in its denominator — meaning more viscous fluids are more likely to flow laminarly for the same velocity and geometry.
Re < 2,300 → Laminar · 2,300 < Re < 4,000 → Transitional · Re > 4,000 → Turbulent
Problem: Water flows at 2 m/s through a 5 cm (0.05 m) diameter pipe at 20°C. Is it laminar or turbulent?
\[ Re = \frac{\rho v D}{\mu} = \frac{998.2 \times 2 \times 0.05}{1.002 \times 10^{-3}} = \frac{99.82}{0.001002} \approx 99{,}620 \]
Answer: Re ≈ 99,620 ≫ 4,000, so the flow is highly turbulent. Reynolds number is the reason viscosity matters for pipe sizing and pump design.
🌡️ How Temperature Affects Dynamic Viscosity
One of the most practically important — and often counterintuitive — aspects of viscosity is its temperature dependence. For liquids, viscosity decreases with increasing temperature (heating makes them flow more easily). For gases, viscosity increases with temperature (more molecular collisions increase internal friction). These opposing trends arise from completely different molecular mechanisms.
📊 Real-World Fluid Viscosity Reference (at 20°C unless noted)
| Fluid | Viscosity (cP) | Viscosity (Pa·s) | Viscosity (P) |
|---|---|---|---|
| Air (20°C) | 0.0182 | \(1.82 \times 10^{-5}\) | \(1.82 \times 10^{-4}\) |
| Ethanol (20°C) | 1.074 | 0.001074 | 0.01074 |
| Water (0°C) | 1.791 | 0.001791 | 0.01791 |
| Water (20°C) | 1.002 | 0.001002 | 0.01002 |
| Water (40°C) | 0.653 | 0.000653 | 0.00653 |
| Water (100°C) | 0.282 | 0.000282 | 0.00282 |
| Milk (20°C) | 2–3 | 0.002–0.003 | 0.02–0.03 |
| Olive oil (20°C) | 84 | 0.084 | 0.84 |
| Motor oil SAE 10 (40°C) | 65–90 | 0.065–0.090 | 0.65–0.90 |
| Motor oil SAE 30 (40°C) | 90–110 | 0.090–0.110 | 0.90–1.10 |
| Motor oil SAE 40 (40°C) | 140–170 | 0.140–0.170 | 1.40–1.70 |
| Castor oil (25°C) | 985 | 0.985 | 9.85 |
| Honey (25°C) | 2,000–10,000 | 2–10 | 20–100 |
| Chocolate syrup | 10,000–25,000 | 10–25 | 100–250 |
| Peanut butter | 150,000–250,000 | 150–250 | 1,500–2,500 |
| Glass (25°C) | ≈ \(10^{24}\) | ≈ \(10^{21}\) | ≈ \(10^{22}\) |
🔬 Newtonian vs Non-Newtonian Fluids
Newton's law of viscosity (\(\tau = \mu\,du/dy\)) assumes that \(\mu\) is constant regardless of the applied shear rate. Fluids obeying this assumption are called Newtonian fluids. Those that don't are non-Newtonian, and their apparent viscosity changes with shear rate. This distinction is critical in food engineering, polymer processing, cosmetics, pharmaceuticals, and biological fluid mechanics.
| Type | Behaviour | Examples | Model |
|---|---|---|---|
| Newtonian | Constant μ at any shear rate | Water, air, most oils, ethanol | \(\tau = \mu \dot{\gamma}\) |
| Shear-thinning (pseudoplastic) | μ decreases with shear rate | Ketchup, paint, blood, shampoo | Power-law: \(\tau = K\dot{\gamma}^n\), \(n < 1\) |
| Shear-thickening (dilatant) | μ increases with shear rate | Cornstarch in water (oobleck) | Power-law: \(\tau = K\dot{\gamma}^n\), \(n > 1\) |
| Bingham plastic | Yield stress required to flow | Toothpaste, mayonnaise, drilling mud | \(\tau = \tau_y + \mu_p\dot{\gamma}\) |
| Thixotropic | μ decreases with time at const. shear | Gels, some paints, yogurt | Time-dependent |