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Coefficient of Viscosity Dimensional Formula

Dimensional formulas of physical quantitiesClass 11FluidsUpdated 1 Nov 2026

[η]=[M1L−1T−1][\eta] = [M^{1} L^{-1} T^{-1}]
SI unit
pascal second (Pa s)
Dimensions
[M¹ L⁻¹ T⁻¹]
where
  • M dimension of mass kg
  • L dimension of length m
  • T dimension of time s

The coefficient of viscosity dimensional formula is [M¹ L⁻¹ T⁻¹], or [ML⁻¹T⁻¹] in short form. It tells you that the stickiness of a fluid scales with mass to the first power and falls off with one power of length and one power of time.

The coefficient η (eta) is defined by Newton's law of viscosity: the drag force between fluid layers is proportional to the layer area and to how fast the speed changes from one layer to the next (the velocity gradient). Honey has a large η, water a small one, but both carry the same bracket. Below are the derivation, the unit Pa s and the poise, a Stokes' law check and a list of slips. For numbers, see the coefficient of viscosity formula page.

Quick facts

  • Dimensional formula

    [M¹ L⁻¹ T⁻¹], short form [ML⁻¹T⁻¹]
  • Defining formula

    F=ηAdvdxF = \eta A \frac{dv}{dx}
  • SI unit

    Pa s = N s m⁻² = kg m⁻¹ s⁻¹
  • CGS unit

    poise; 1 Pa s = 10 poise
  • Common symbol

    η (eta)
  • Chapter

    Mechanical properties of fluids, Class 11

Deriving the coefficient of viscosity dimensional formula

Start from the law that defines η, then isolate it.

  1. Viscous force: F=ηAdvdxF = \eta A \frac{dv}{dx}, so η=FA (dv/dx)\eta = \frac{F}{A \, (dv/dx)}.
  2. Force: [F]=[MLT−2][F] = [M L T^{-2}]. Area: [A]=[L2][A] = [L^{2}].
  3. Velocity gradient is speed per distance: [dv/dx]=[LT−1]÷[L]=[T−1][dv/dx] = [L T^{-1}] \div [L] = [T^{-1}].
  4. Area times gradient is [L2T−1][L^{2} T^{-1}]. Flip it and multiply by the force: [η]=[L−2T]⋅[MLT−2]=[ML−1T−1][\eta] = [L^{-2} T] \cdot [M L T^{-2}] = [M L^{-1} T^{-1}].

The velocity gradient step is where most errors start. It is not a velocity; it has units of s⁻¹, the same as a frequency. A minus sign sometimes appears in the force law to show the drag opposes motion, but a sign has no effect on dimensions. The velocity gradient page explains that ratio further.

Pa s, the poise and how they relate

Turn [ML⁻¹T⁻¹] into base units: kg m⁻¹ s⁻¹. Group them another way and you get N s m⁻², which is a pascal second (Pa s). Both are the SI unit of the coefficient of viscosity. Pa s is the form most answer keys print.

Convert 1 Pa s into the CGS unit, the poise

The poise is g cm⁻¹ s⁻¹. Raise each conversion factor to its own power from the bracket.

1 Pa s=(1000 g)(100 cm)−1(1 s)−1=10 g cm−1s−11\ \text{Pa s} = (1000\ \text{g})(100\ \text{cm})^{-1}(1\ \text{s})^{-1} = 10\ \text{g cm}^{-1}\text{s}^{-1}.

So 1 Pa s = 10 poise, and 1 centipoise = 10⁻³ Pa s. Water near room temperature is close to 1 centipoise.

Matching brackets and a look alike

Quantities with the same bracket as viscosity, [M¹ L⁻¹ T⁻¹]
QuantityHow it is builtWhy it matches
Dynamic viscosity of any fluidshear stress ÷ velocity gradientThe definition itself
Pressure × timeP tP \, t[ML⁻¹T⁻²] × [T]
Stress × timeσ t\sigma \, tStress has the pressure bracket

The pressure times time row gives a neat way to remember the result: viscosity is shear stress divided by a rate, s⁻¹, so it is a stress multiplied by a time. Compare that with the dimensional formula of pressure.

Kinematic viscosity is a different quantity. It is η divided by density, ν = η/ρ, with dimensions [ML⁻¹T⁻¹] ÷ [ML⁻³] = [L²T⁻¹] and unit m²/s. Do not mix the two in an answer.

Two fluid laws put to the test

Check Stokes' law, F = 6πηrv, for a sphere falling through a fluid

Right side: [η][r][v]=[ML−1T−1][L][LT−1][\eta][r][v] = [M L^{-1} T^{-1}][L][L T^{-1}].

Collect powers: M¹, L⁻¹⁺¹⁺¹ = L¹, T⁻¹⁻¹ = T⁻². Result [MLT−2][M L T^{-2}].

That is a force, so the law is dimensionally consistent. The 6π is a number and cannot be tested.

Check the flow rate relation Q = πPr⁴/(8ηl)

Top: [ML−1T−2][L4]=[ML3T−2][M L^{-1} T^{-2}][L^{4}] = [M L^{3} T^{-2}]. Bottom: [ML−1T−1][L]=[MT−1][M L^{-1} T^{-1}][L] = [M T^{-1}].

Ratio: [L3T−1][L^{3} T^{-1}], a volume per second. Here P is the pressure difference along the tube, and the result is the expected flow rate.

Errors that cost marks

  • Writing [MLT⁻¹]. That is momentum. Viscosity has length to the power −1.
  • Treating dv/dx as a velocity. It is [T⁻¹]; skipping the division by distance gives the wrong answer.
  • Mixing up dynamic and kinematic viscosity. η is [ML⁻¹T⁻¹]; ν is [L²T⁻¹].
  • Converting Pa s to poise by 100. The factor is 10, from 10³ g divided by 10² cm.

The viscosity bracket is collected with the other fluid quantities on the dimensional formulas page.

Frequently asked questions

In SI, what unit does η take?

Pa s. Written with base units that is kg m⁻¹ s⁻¹, and it can also appear as N s m⁻².

Is the dimensional formula of viscosity different from that of the coefficient?

No. When a question says viscosity it normally means the coefficient η, so the answer is [M¹ L⁻¹ T⁻¹]. Only kinematic viscosity differs, at [L²T⁻¹].

How many poise make one pascal second?

Ten. One poise is 0.1 Pa s, and one centipoise is 0.001 Pa s.

Is the coefficient of viscosity a scalar?

Yes. For ordinary fluids η is a single number that depends on the fluid and its temperature, with no direction.

Why is the velocity gradient [T⁻¹]?

It is a change in speed, [LT⁻¹], divided by the distance between layers, [L]. The lengths cancel and only one over time remains.