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Rayleigh's method for orifice discharge

Short answer

Q = √g d⁵/² φ(H/d, μ/(ρ√g d³/²)). The dimensionless groups are head ratio and a Reynolds-type number; standard form is Q = C_d A√(2gH).

In a flow through a small orifice discharging freely into atmosphere under a constant head (H), the flow discharge (Q) depends on diameter of pipe (d), constant head, dynamic viscosity (μ\mu), density of fluid (ρ\rho) and acceleration due to gravity (g). Using Rayleigh's methods develop the relation in terms of non-dimensional terms.

Relation

QQ depends on d,H,μ,ρ,gd, H, \mu, \rho, g. By Rayleigh's method:

Q=K daHbμcρegfQ = K\,d^{a}H^{b}\mu^{c}\rho^{e}g^{f}

Dimensions

Q=L3T−1Q = L^3T^{-1}, d=H=Ld = H = L, μ=ML−1T−1\mu = ML^{-1}T^{-1}, ρ=ML−3\rho = ML^{-3}, g=LT−2g = LT^{-2}.

DimensionEquation
M0=c+e0 = c + e
L3=a+b−c−3e+f3 = a + b - c - 3e + f
T−1=−c−2f-1 = -c - 2f

There are 5 unknowns and 3 equations. Express in terms of bb and cc:

e=−c,f=1−c2,a=52−3c2−be = -c,\qquad f = \frac{1-c}{2},\qquad a = \frac52 - \frac{3c}{2} - b

Substitute

Q=K d 52−3c2−b Hb μc ρ−c g1−c2Q = K\,d^{\,\frac52-\frac{3c}{2}-b}\,H^{b}\,\mu^{c}\,\rho^{-c}\,g^{\frac{1-c}{2}}

Collect terms with the same powers:

Q=K g d5/2(Hd)b(μρ g1/2d3/2)cQ = K\,\sqrt g\,d^{5/2}\left(\frac Hd\right)^{b}\left(\frac{\mu}{\rho\,g^{1/2}d^{3/2}}\right)^{c}

Answer:

Q=g d5/2 ϕ[Hd, μρg d3/2]Q = \sqrt{g}\,d^{5/2}\ \phi\left[\frac Hd,\ \frac{\mu}{\rho\sqrt g\,d^{3/2}}\right]

Equivalently, Q=d2gH ϕ1 ⁣(H/d, Re)Q = d^2\sqrt{gH}\ \phi_1\!\left(H/d,\ Re\right). The dimensionless groups are the head ratio H/dH/d and a Reynolds-type number. For a given orifice, experiments give Q=CdA2gHQ = C_dA\sqrt{2gH}.

✓ Answer checked by Claude Opus 5.5 (high effort)

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