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Research Papers: Other (Seals, Manufacturing)

Theoretical Analysis of the Static Characteristics of the Carbon Segmented Seal

[+] Author and Article Information
Mihai Arghir

PPRIME Institute,
UPR CNRS 3346,
Université de Poitiers,
ENSMA ISAE,
Chasseneuil Futuroscope 86962, France

Antoine Mariot

Centre National d'Etudes Spatiales,
Paris 75001, France;
PPRIME Institute,
UPR CNRS 3346,
Université de Poitiers,
ENSMA ISAE,
Chasseneuil Futuroscope 86962, France

1Present address: SAFRAN Aircraft Engines, Villaroche 92141, France.

Contributed by the Tribology Division of ASME for publication in the JOURNAL OF TRIBOLOGY. Manuscript received October 26, 2016; final manuscript received February 21, 2017; published online June 30, 2017. Assoc. Editor: Min Zou.

J. Tribol 139(6), 062202 (Jun 30, 2017) (11 pages) Paper No: TRIB-16-1340; doi: 10.1115/1.4036272 History: Received October 26, 2016; Revised February 21, 2017

The segmented carbon seal is regularly used for sealing bearing chambers of aeronautical turboengines or as part of a buffer seal in space turbopumps. The seal operates with contaminated air or with an inert gas and is made of many identical carbon segments (generally three or six) with reciprocally overlapping ends. The segments are pressed against the rotor by the pressure difference between the upstream and the downstream chambers and by a circumferential (garter) spring. The pressure difference and an axial spring press the segments also against the stator. The inner cylindrical surface of each segment is provided with pads that create an aerodynamic lift proportional to the rotor speed. Following this lift force, the segments of the seal are pushed away from the rotor and the seal opens. The contact between the rotor and the segments is lost, and an axial leakage path is thus created. Although it was developed since long, a model for calculating the characteristics of the segmented seal is completely absent from the scientific literature. The goal of the present work is to fill this gap at least for the static characteristics (leakage and torque). The analysis is carried out for a single segment of the seal by supposing that all the segments have the same characteristics. Each segment has a planar motion (i.e., three degrees-of-freedom (3DOF)), and therefore the film thickness under each pad is not uniform. Given the stationary operating conditions (pressure difference and rotation speed), the present model calculates the equilibrium position of each segment on the bases of the lift and the friction force acting on the pads, the friction forces acting on the nose of the seal, and the radial and axial springs. Once found the static equilibrium position, the leakage and the torque of the seal are calculated. A parametric study enlightens the importance of the pad waviness, the pocket depth, and the spring forces on the characteristics of the segmented seal.

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References

Figures

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Fig. 1

Exploded view of the segmented seal

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Fig. 2

Enlarged detail of the segmented seal

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Fig. 3

Pressure field from a computational fluid dynamics (CFD) analysis (a) under the pad and (b) under the lip

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Fig. 4

Simplified view of the forces acting on the segment (a) at nominal speed and (b) after coast-down

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Fig. 5

Calculation domain for the pad and the lip

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Fig. 6

Pressure field on a pocketed pad

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Fig. 7

Typical pressure variation under the lip

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Fig. 8

The displacements of the segment

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Fig. 9

Forces acting on a segment

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Fig. 10

Relative displacements of the segments after seal opening

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Fig. 11

The unwrapped geometry of the segment (all dimensions are in mm)

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Fig. 12

Fluid pressures (left) and contact pressures (right) for pads 1 (top) to 3 (bottom); all pressures are in (Pa) and the lengths in (m)

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Fig. 13

The displacements of the segment (left) and of the seal leakage flow and dissipated power (right) versus different parameters: (a) rotation speed, (b) pocket depth, (c) pocket length, (d) pocket width, (e) magnitude of the axial spring force, (f) magnitude of the garter spring force, and (g) amplitude of the waviness errors

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Fig. 14

Representation of the rough surface

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