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22-Mec-A6 Fluid Machinery · December 2018

Question 5 of 6: Dimensional Analysis of Missile Lift

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams — December 2018, 16-Mec-A6 Advanced Fluid Mechanics. Open book, 3 hours. Six questions of equal value (20 marks); any five constitute a complete paper. All six are solved here.

Reference texts. J.D. Anderson, Modern Compressible Flow, 3rd ed. (Q1); F.M. White, Fluid Mechanics, 8th ed. and Kundu, Cohen & Dowling, Fluid Mechanics, 6th ed. (Q2, Q5); F.M. White, Viscous Fluid Flow, 3rd ed. (Q3, Q4, Q6); Schlichting & Gersten, Boundary-Layer Theory, 8th ed. (Q6); Fox & McDonald, Introduction to Fluid Mechanics, 10th ed. (general).

Question 5: Dimensional Analysis of Missile Lift (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. The functional statement $F=f(L,V,D,\alpha,\rho,\mu,c)$ with eight variables, one of which ($\alpha$) is already dimensionless.

Variables and MLT dimensions
Variable$M$$L$$T$
$F$ (lift)11−2
$L$ (length)010
$V$ (velocity)01−1
$D$ (diameter)010
$\rho$ (density)1−30
$\mu$ (viscosity)1−1−1
$c$ (sound speed)01−1
$\alpha$ (angle)000

Find. The complete set of independent $\pi$ groups and the reduced functional relation.

Approach. Apply the Buckingham $\pi$ theorem: count variables and independent dimensions to fix the number of groups, choose dimensionally independent repeating variables, and form each remaining variable into a dimensionless product.

  1. Number of groups. There are $n=8$ variables and $k=3$ independent dimensions ($M,L,T$), so the number of independent dimensionless groups is $$n-k = 8-3 = \boxed{5}.$$
  2. Repeating variables. Choose $\rho,\ V,\ D$ — they contain all three dimensions and cannot form a dimensionless group among themselves.
  3. Form the groups. Non-dimensionalising each remaining variable gives $$\pi_1=\frac{F}{\rho V^{2} D^{2}}\ (\text{lift coefficient}),\quad \pi_2=\frac{L}{D}\ (\text{slenderness}),\quad \pi_3=\frac{\rho V D}{\mu}=Re,$$ $$\pi_4=\frac{V}{c}=Ma\ (\text{Mach number}),\quad \pi_5=\alpha\ (\text{already dimensionless}).$$
  4. Reduced relation. The eight-variable law collapses to a five-group relation: $$\boxed{\dfrac{F}{\rho V^{2} D^{2}}=\phi\!\left(\dfrac{L}{D},\ \dfrac{\rho V D}{\mu},\ \dfrac{V}{c},\ \alpha\right).}$$ So the lift coefficient depends on slenderness, Reynolds number, Mach number and angle of attack — all recognizable, named groups.
Question 5 — the five $\pi$ groups
GroupMeaning
$\pi_1=F/(\rho V^2 D^2)$lift (force) coefficient
$\pi_2=L/D$geometric slenderness ratio
$\pi_3=\rho V D/\mu$Reynolds number
$\pi_4=V/c$Mach number
$\pi_5=\alpha$angle of attack