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Annals of Civil Engineering and Management(ACEM)

ISSN: 3065-9779 | DOI: 10.33140/ACEM

Research Article - (2025) Volume 2, Issue 2

Analytical Solution for Fluid Dynamics

Paul T E Cusack *
 
BScE DULE, 23 Park Ave. Saint John, NB E2J 1R2, Canada
 
*Corresponding Author: Paul T E Cusack, BScE DULE, 23 Park Ave. Saint John, NB E2J 1R2, Canada

Received Date: Jun 07, 2025 / Accepted Date: Jul 16, 2025 / Published Date: Jul 24, 2025

Copyright: ©©2025 Paul T E Cusack. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

Citation: Cusack, P. T. E. (2025). Analytical Solution for Fluid Dynamics, Ann Civ Eng Manag, 2(2), 01-06.

Abstract

In this important paper, we put fluid dynamics on a theoretic basis for some basic flows. We also put the Hazen Williams and Manning Equation on a theoretical foundation. Various other flow environments may be subject to similar transformations.

Introduction

Newtonian Fluids Low Viscosity

Teflon Mass = C2F4 = 2(12.011) + 4(18.989) = 99.989 x 6.022 = 602

∫1/2→π Ln t = 1.602

Mt-1 = M

M = t

PE = KE

PE-KE = 0 Conservation of Energy

t² - t - 1 = 0 GMP

F = Mα

(49989) (1/√2)

=35.3≈i


Figure 1: Cusack’s RLC Circuit


Figure 2: Cusack Exponential Mass-Time Plot

1533.5 x 2π/6.693 = 1/0.6946

15335-1.4645 = -0.0695

t = eM = e-0.0695 = 499 = V+

Hookes Law

σ = Yε

F/A = (0.4233) t

8/3 = 0.4233t

t = 1/0.1588 = 1/E

E = hν = ht6.628(1/0.1588)

=417

GMP: E=1/511=1/Me- flow of Electricity

sin² 45°+cos²45°= 1= x²/a²+y²/b²

θ=t=π/4

f 0 (x) = ax + 1-a

= 2x+1-2

= 2t-1 = dE/dt

dy/dx = a = f(x)″ = 2 = G

y = f0 (x) = ax + b = f(x)′

= 2x+b

= 2t-1

b = 1

For Laminar flow

Bernoulli

p + 1/2ρv² + z = 0

mgh + 1/2ρv² + 0 = 0

PE + KE = 0

M = t

E = 1- e -1

-1/t = 1-1/E

-1/t = 1-t

-1 = t -t²

t²- t -1 = 0 ⇒ GMP sheet flow

The GMP reigns for the flow out of a nozzle


Figure: 8 Source[1]

So, we’ve shown that the GMP is key to analyzing fluid dynamics theoretically

Hazen-Willimam for flow under pressure:

Hazen-Willimam for flow under pressure:

Note that turbulent flow is subject to the Fair Coin GMP Eqaution.

References

1.Meyer, RE. Introduction to Mathematical Fluid Dynamis. USA: Dover, 1971.