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Dimensional analysis of forced convection

Short answer

With variables h, D, V, rho, mu, k, cp, dimensional analysis using repeating variables D, V, mu, k yields three pi groups: Nu = hD/k, Re = rho V D/mu, Pr = cp mu/k. Thus Nu = f(Re, Pr). Nu represents dimensionless temperature gradient, Re inertia/viscous forces, Pr momentum/thermal diffusivity ratio.

Using Buckingham's pi theorem, show that for forced convection inside a tube the Nusselt number is a function of the Reynolds and Prandtl numbers only. The heat transfer coefficient h depends on the tube diameter D, fluid velocity V, density rho, viscosity mu, thermal conductivity k and specific heat cp. Also state the physical meaning of each dimensionless group.

Variables and dimensions

Fundamental dimensions: mass M, length L, time T, temperature θ\theta (heat is expressed in mechanical units, so there are 4).

VariableSymbolDimensions
Heat transfer coefficienthhMT−3θ−1M T^{-3}\theta^{-1}
DiameterDDLL
VelocityVVLT−1L T^{-1}
Densityρ\rhoML−3M L^{-3}
Viscosityμ\muML−1T−1M L^{-1}T^{-1}
ConductivitykkMLT−3θ−1M L T^{-3}\theta^{-1}
Specific heatcpc_pL2T−2θ−1L^2T^{-2}\theta^{-1}

n=7n = 7 variables, m=4m = 4 fundamental dimensions, so the number of π\pi groups is n−m=3n - m = 3.

Repeating variables

Choose DD, VV, μ\mu, kk (together they contain L,T,M,θL, T, M, \theta and are independent). Each non-repeating variable (hh, ρ\rho, cpc_p) forms one group.

Group 1 with hh: π1=h DaVbμckd\pi_1 = h\,D^aV^b\mu^ck^d. Equating exponents to zero:

  • MM: 1+c+d=01 + c + d = 0
  • LL: a+b−c+d=0a + b - c + d = 0
  • TT: −3−b−c−3d=0-3 - b - c - 3d = 0
  • θ\theta: −1−d=0⇒d=−1-1 - d = 0 \Rightarrow d = -1

Then c=0c = 0, b=0b = 0 and a=1a = 1, so π1=hDk=Nu\pi_1 = \dfrac{hD}{k} = Nu.

Group 2 with ρ\rho: the same procedure gives π2=ρVDμ=Re\pi_2 = \dfrac{\rho V D}{\mu} = Re.

Group 3 with cpc_p: π3=cpμk=Pr\pi_3 = \dfrac{c_p\mu}{k} = Pr.

Result

π1=f(π2,π3)  ⇒  Nu=f(Re,Pr)\pi_1 = f(\pi_2,\pi_3)\;\Rightarrow\; Nu = f(Re, Pr)

Experiments give the form Nu=C RemPrnNu = C\,Re^m Pr^n, for example Dittus-Boelter Nu=0.023 Re0.8PrnNu = 0.023\,Re^{0.8}Pr^{n}.

Physical meaning

GroupMeaning
Nusselt, hD/khD/kRatio of convective to conductive heat transfer in the fluid layer; dimensionless temperature gradient at wall
Reynolds, ρVD/μ\rho VD/\muRatio of inertia to viscous forces; decides laminar or turbulent flow
Prandtl, μcp/k\mu c_p/kRatio of momentum diffusivity to thermal diffusivity; a fluid property

✓ Answer checked by Claude Sonnet 5.5

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