In general, the computation of single phase subsonic mass velocity of gas flowing through a pipe requires a computerized iterative analysis. The equations for the friction factor for laminar and turbulent flow are used to obtain explicit equations for the subsonic mass velocity as a function of the pressures at the ends of a pipe. Explicit equations for mass velocity are presented. Included within the equations is a heat transfer ratio, which can vary between 0 for adiabatic flow conditions to 1 for isothermal flow conditions. The use of this heat transfer ratio also enables the formulation of an explicit equation for the gas temperature along the pipe for nonisothermal flow conditions. The explicit equations eliminate the need for an iterative solution. Laboratory data are used to support the accuracy of the model.

1.
Mulley
,
R.
, 2004,
Flow of Industrial Fluids—Theory and Equations, ISA—The Instrumentation, Systems, and Automation Society
,
CRC
,
Boca Raton, FL
, pp.
321
323
.
2.
Cochran
,
T. W.
, 1966, “
Calculate Pipeline Flow of Compressible Fluids
,”
Chemical Engineering
,
103
(
2
), pp.
115
122
. 0002-7820
3.
Hörnell
,
K.
, and
Lotstedt
,
P.
, 2004, “
Adaptive Iteration to Steady State of Flow Problems
,”
J. Sci. Comput.
0885-7474,
20
(
3
), pp.
331
354
.
4.
Abbaspour
,
M.
,
Chapman
,
K. S.
, and
Keshavarz
,
A.
, 2004, “
Dynamic Modeling of Non-Isothermal Gas Pipeline Systems
,”
Proceedings of the International Pipeline Conference, IPC
, Vol.
3
, pp.
2155
2163
.
5.
Moody
,
L. F.
, 1944, “
Friction Factors for Pipe Flow
,”
Trans. ASME
0097-6822,
66
(
8
), pp.
671
684
.
6.
Blasius
,
H.
, 1913, “
Das Ahnlichkeits-Gesetz bei Reibungsvorgangen in Flussigkeiten
,”
Forschungs-Arbeiten des Ver. Deutsch. Ing.
,
131
, pp.
1
12
. 0002-7820
7.
Davis
,
R. L.
, and
Campbell
,
B. T.
, 2007, “
Quasi-One-Dimensional Unsteady-Flow Procedure for Real Fluids
,”
AIAA J.
0001-1452,
45
(
10
), pp.
2422
2428
.
You do not currently have access to this content.