37th Joint Propulsion Conference and Exhibit 2001
DOI: 10.2514/6.2001-3329
|View full text |Cite
|
Sign up to set email alerts
|

A micro-fabricated colloidal thruster array

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
16
0

Year Published

2003
2003
2024
2024

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 22 publications
(16 citation statements)
references
References 4 publications
0
16
0
Order By: Relevance
“…The results were documented in two M.S. Theses, by M. Paine [12] and L.F. Velasquez [13, respectivley. The concept proposed by Paine involved micro-capillary channels oriented perpendicular to the face of a silicon wafer.…”
Section: Ir-a %V-hired (From -mentioning
confidence: 80%
“…The results were documented in two M.S. Theses, by M. Paine [12] and L.F. Velasquez [13, respectivley. The concept proposed by Paine involved micro-capillary channels oriented perpendicular to the face of a silicon wafer.…”
Section: Ir-a %V-hired (From -mentioning
confidence: 80%
“…Following research in micro-ion-propulsion systems for attitude control 2 and the miniaturization of ground-based mobile communications, it is known that the satellite power requirement does not reduce linearly with mass. Many small satellite missions simply use body-mounted photovoltaic cells, severely restricting the total available power (because of the small surface area of the satellite).…”
Section: A Mmentioning
confidence: 99%
“…= constant for tape-spring dynamic solution a = width of undeformed tape spring B m = constant for tape-spring dynamic solution C m = constant for tape-spring dynamic solution D = flexural rigidity E = Young's modulus G = shear modulus I array = inertia of unfolding array I y = inertia of tape spring around y axis J = St. Venant torsional constant L = total tape-spring length l 1 , l 2 = array lengths defined from L and µ l s2 = length of tape-spring segment 2 ( = initial longitudinal and transverse radii of curvature, respectively T = torsional moment of tape sprinḡ T = nondimensional torsional moment t = time from deployment release t ts = thickness of the tape spring α = angle subtended by cross-section of spring β = angle of plane (which contains the tape spring) from the horizontal plane γ = total twist angle γ 2 = twist of tape spring segment 2 ( T HE total satellite mass has always been a key parameter in satellite design, and with advances in microtechnology 1 there is an increasing interest in the space industry to develop very lowmass satellites for a wide variety of applications. Following research in micro-ion-propulsion systems for attitude control 2 and the miniaturization of ground-based mobile communications, it is known that the satellite power requirement does not reduce linearly with mass.…”
Section: A Mmentioning
confidence: 99%
“…Over recent decades there has been growing research and development in the miniaturization of electronic and mechanical technologies [1]. It is now possible to construct very small satellites [2], thereby dramatically reducing the cost of access to space.…”
Section: Introductionmentioning
confidence: 99%