We perform gas flow experiments in a shallow microchannel, 1.14±0.02 μm deep, 200 μm wide, etched in glass and covered by an atomically flat silicon wafer. The dimensions of the channel are accurately measured by using profilometry, optical microscopy and interferometric optical microscopy. Flow-rate and pressure drop measurements are performed for helium and nitrogen, in a range of averaged Knudsen numbers extending up to 0.8 for helium and 0.6 for nitrogen. This represents an extension, by a factor of 3 or so, of previous studies. We emphasize the importance of the averaged Knudsen number which is identified as the basic control parameter of the problem. From the measurements, we estimate the accommodation factor for helium to be equal to 0.91±0.03 and that for nitrogen equal to 0.87±0.06. We provide estimates for second-order effects, and compare them with theoretical expectations. We estimate the upper limit of the slip flow regime, in terms of the averaged Knudsen number, to be 0.3±0.1, for the two gases.

1.
J.
Maxwell
, “
On stress in rarefied gases arising from inequalities of temperature
,”
Philos. Trans. R. Soc. London
170
,
231
(
1879
).
2.
S. Schaaf, in Modern Developments in Gas Dynamics, edited by W. Loh (Plenum, New York, 1969), p. 235.
3.
G. Karniadakis and A. Beskok, Micro Flows (Springer-Verlag, Berlin, 2002).
4.
C.
Cercignani
and
A.
Daneri
, “
Flow of a rarefied gas between two parallel plates
,”
J. Appl. Phys.
34
,
3509
(
1963
).
5.
R.
Deissler
, “
An analysis of second-order slip flow and temperature jump boundary conditions for rarefied gases
,”
Int. J. Heat Mass Transfer
7
,
681
(
1964
).
6.
Y. Sone, in Lecture Notes, Department of Aeronautics and Astronautics,Graduate School of Engineering, Kyoto University (1998); this work is accounted for in Ref. 3.
7.
M.
Knudsen
, “
Die gesetze der molekularstromung und der inneren riebungsstromung der gaze durch rohnen
,”
Ann. Phys. (Leipzig)
28
,
75
(
1909
);
M.
Knudsen
,
Ann. Phys. (Leipzig)
28
,
130
(
1909
).
8.
C.
Ho
and
Y.
Tai
, “
Microelectromechanical systems (MEMS) and fluid flows
,”
Annu. Rev. Fluid Mech.
30
,
579
(
1998
).
9.
M.
Gad-El-Hak
, “
The fluid mechanics of microdevices
,”
J. Fluids Eng.
12
(
1
),
5
(
1999
).
10.
S.
Tison
, “
Experimental data and theoretical modeling of gas flows through metal capillary leaks
,”
Vacuum
44
,
1171
(
1993
).
11.
J.
Pfhaler
,
C.
Harley
,
H.
Bau
, and
J.
Zemel
, “
Gas and liquid flows in small channels
,”
J. ASME
32
,
49
(
1991
).
12.
E.
Arkilic
,
K.
Breuer
, and
M.
Schmidt
, “
Mass flow and tangential momentum accomodation in silicon micromachined channels
,”
J. Fluid Mech.
437
,
29
(
2001
).
13.
C.
Aubert
and
S.
Colin
, “
Second-order effects in gas flows through microchannels
,”
Microscale Thermophys. Eng.
5
,
1
,
41
(
2001
).
14.
Y. Zohar, S. Lee, W. Lee, L. Jiang, and P. Tong, “Subsonic gas flow in a straight and uniform microchannel,” J. Fluid. Mech. (to be published).
15.
E.
Piekos
and
K.
Breuer
, “
Numerical modeling of micromechanical devices using the direct simulation Monte Carlo method
,”
J. Fluids Eng.
118
,
464
(
1996
).
16.
H.
Xue
,
A.
Fan
, and
C.
Shu
, “
Prediction of micro-channel flows using direct simulation Monte Carlo
,”
Probab. Eng. Mech.
15
,
213
(
2000
).
17.
F.
Sharipov
and
V.
Seleznev
, “
Data on internal rarefied gas flows
,”
J. Phys. Chem. Ref. Data
27
,
657
(
1998
).
This content is only available via PDF.
You do not currently have access to this content.