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Library / Dimensional analysis and similarity / DIM-16

Dimensional analysis and similarity

Stanton number

Heat actually transferred to the fluid compared with the heat the stream can carry.

Ref
DIM-16
Rev
v1
Field
Dimensional analysis and similarity
Result
St

Sth = h/(ρcpU) compares the heat transferred to the fluid with the heat the stream can carry, ρcpU per unit area for each kelvin. It equals Nu/(Re Pr), so it can be found from a Nusselt correlation. For Prandtl numbers near 1 it is about half the skin-friction coefficient (the Reynolds analogy). The mass-transfer analogue is Stm = km/U = Sh/(Re Sc).

Heat actually transferred to the fluid compared with the heat the stream can carry. It is the Nusselt number divided by the product of the Reynolds and Prandtl numbers.

Calculator

Solve for
W/(m² K)
110,000
kg/m³
0.12,000
J/(kg K)
5005,000
m/s
0.1400
  • Stream heat-capacity rate per unit area, ρcpU12,000 W/(m² K)
  • Skin-friction coefficient from the Reynolds analogy, 2St (Pr ≈ 1)0.01
  • Stanton number with the speed doubled and h unchanged0.0025
  • Heat flux per kelvin at the surface60 W/(m² K)

What drives the result

Each variable is moved across its typical range while the others stay at the values above. The longest bar is the key driver.

Stanton number () current value 0.005
hConvective heat-transfer coefficientKey driver
8.33e-50.833
UFree-stream or bulk speed
1.25e-40.5
ρFluid density
3e-60.06
cpSpecific heat capacity at constant pressure
0.0010.01
  • St = 0.005 means the surface passes a fraction 0.005 of the stream’s heat-carrying capacity per kelvin: 0.5 % of the maximum possible.
  • Combined with the Reynolds analogy, St ≈ Cf/2 when Pr is near 1, so a skin-friction measurement gives a first estimate of the heat-transfer coefficient.
Chart data as tables

Ranked variables

VariableTypical rangeLowest resultHighest resultSwing ()Local stepChange in result
h Convective heat-transfer coefficient1 to 10,000 W/(m² K)8.333e-50.83330.8333+10%+10 %
U Free-stream or bulk speed0.1 to 400 m/s1.25e-40.50.4999+10%−9.09 %
ρ Fluid density0.1 to 2,000 kg/m³3e-60.060.06+10%−9.09 %
cp Specific heat capacity at constant pressure500 to 5,000 J/(kg K)0.0010.010.009+10%−9.09 %

Sweep of Free-stream or bulk speed

Free-stream or bulk speed (m/s)Stanton number
0.10.5
0.2820.1773
0.79530.06287
2.2430.02229
6.3250.007906
17.840.002803
50.39.941e-4
141.83.525e-4
4001.25e-4

Sweep one variable

Stanton number ()Hover, touch, or use the arrow keys on the chart
00.10.20.30.40.5 0.1110100 Free-stream or bulk speed (m/s), log scale now 0.005

Variables and how each one contributes

St

Stanton number

Result ·

What the equation gives you. Everything else feeds it.

h

Convective heat-transfer coefficient

W/(m² K) · typical 1 to 10,000

The convective heat-transfer coefficient, in W/(m² K). Raises the Stanton number in direct proportion. Raising it by 10 % (to 66) moves the result by +10 %, from 0.005 to 0.0055.

ρ

Fluid density

kg/m³ · typical 0.1 to 2,000

The fluid density, in kg/m³. Lowers the Stanton number in inverse proportion. Raising it by 10 % (to 1.32) moves the result by −9.09 %, from 0.005 to 0.004545.

cp

Specific heat capacity at constant pressure

J/(kg K) · typical 500 to 5,000

The specific heat capacity at constant pressure, in J/(kg K) (air about 1005, water about 4180). Lowers the Stanton number in inverse proportion. Raising it by 10 % (to 1,100) moves the result by −9.09 %, from 0.005 to 0.004545.

U

Free-stream or bulk speed

m/s · typical 0.1 to 400

The free-stream or bulk speed, in m/s. Lowers the Stanton number in inverse proportion: the stream carries more heat at higher speed. Raising it by 10 % (to 11) moves the result by −9.09 %, from 0.005 to 0.004545.

Worked example with the values above

  1. Stream capacity: ρcpU = 1.2 × 1,000 × 10 = 12,000 W/(m² K).
  2. Divide the heat-transfer coefficient by it: 60 / 12,000.
  3. St = 0.005.

Assumptions and limits

  • h is the convective coefficient defined with the same reference temperature difference as in the correlation used.
  • Properties are evaluated at a consistent reference temperature, such as the film temperature.

Common mistakes

  • Using the specific heat at constant volume instead of cp.
  • Mixing U from different positions: free-stream or bulk.
  • Using the mass-transfer form Stm = km/U with a thermal h.

Statistics and uncertainty

The result is a product of powers, so to first order its relative error is the root sum of squares of each input’s relative error multiplied by its exponent (h × 1, ρ × −1, cp × −1, U × −1). The coefficient h usually carries the largest uncertainty, typically 10 to 25 % from a correlation, so St inherits it.

Where it is used

  • Expressing a convective heat-transfer coefficient as a size-independent number for correlations and for scaling.
  • Relating heat transfer to skin friction in boundary layers through the Reynolds analogy.

Maths you need

  • Nusselt number: dimensionless heat-transfer coefficient
  • Specific heat capacity: energy to heat 1 kg by 1 K

Related formulas

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