|
query_id,query,relevant_docs_gt_0
|
|
1, |
|
of heated high speed aircraft .","['184', '29', '31', '12', '51', '102', '13', '14', '15', '57', '378', '859', '185', '30', '37', '52', '142', '195', '875', '56', '66', '95', '462', '497', '858', '876', '879', '880']
|
|
2, |
|
of high speed aircraft .","['12', '15', '184', '858', '51', '102', '202', '14', '52', '380', '746', '859', '948', '285', '390', '391', '442', '497', '643', '856', '857', '877', '864', '658']
|
|
4, |
|
far .","['236', '166']
|
|
8, |
|
solutions for chemically reacting gas mixtures based on the simplifying |
|
assumption of instantaneous local chemical equilibrium .","['48', '122', '20', '58', '196', '354', '360', '197', '999', '1112', '1005']
|
|
9, |
|
problems .","['21', '22', '550']
|
|
10, |
|
couette flow behaviour .","['259', '405', '302', '436', '437', '438', '998', '1011']
|
|
12, |
|
ogive forebody at zero angle of attack to the lower surface pressures of |
|
an equivalent ogive forebody at angle of attack .","['86', '194', '650', '649', '652']
|
|
13, |
|
for predicting body pressures at angle of attack.","['64', '265', '65', '311']
|
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15,papers on internal /slip flow/ heat transfer studies .,"['463', '462']"
|
|
18, |
|
enthalpies and densities .","['196', '197', '198']
|
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22, |
|
blast wave problem in the newtonian approximation .
|
|
23, |
|
machines be calculated .","['900', '902', '200', '201', '601', '899', '903', '593', '199', '594', '901', '544', '597', '749', '917', '919', '1333', '634', '687', '698', '1290', '700', '704', '705', '1109', '1112', '1141', '1197', '1256', '1259', '1272', '1289']
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|
26,what is the basic mechanism of the transonic aileron buzz .,"['145', '611', '376', '406', '565', '1076']"
|
|
27,papers on shock-sound wave interaction .,"['224', '278', '428']"
|
|
29,material properties of photoelastic materials .,"['250', '514', '609', '225', '793', '464', '465', '612', '466']"
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31, |
|
calculated efficiently by an electronic computer .
|
|
32, |
|
a body of revolution be reduced to a two-dimensional problem .","['465', '249', '777', '778', '247', '250']
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33, |
|
of attack available .","['252', '431', '141']
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34, |
|
combining consideration of realistic effects with relative simplicity of |
|
results .","['252', '431', '672', '714', '799', '800']
|
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35, |
|
by the induced current, in magnetohydrodynamic free convection flows |
|
under general conditions .","['166', '167', '132']
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39, |
|
speed data for helium and air .","['272', '555', '24', '283', '552', '79', '207', '418', '557', '554', '556', '505', '1257']
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40, |
|
sensitive to the nature of the variation of the viscosity with |
|
temperature .","['24', '283', '552', '272', '85', '976', '557', '558', '553', '554', '555', '556']
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41,what progress has been made in research on unsteady aerodynamics .,"['288', '289', '433']"
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49, |
|
structural matrices .","['320', '478']
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50, |
|
interaction between adjacent blade rows of a supersonic cascade .","['326', '629', '21', '94', '22', '306']
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51, |
|
a laminar boundary layer in compressible flow on a flat plate .","['94', '23', '105', '381', '192', '326', '63', '494', '629', '261']
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52, |
|
by thickness .","['21', '22', '306', '326']
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53,what application has the linear theory design of curved wings .,"['296', '33', '446', '447', '448', '449', '208', '297', '298', '299']"
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|
54, |
|
delta wings with sharp leading edges .","['84', '24', '101', '294', '628', '661', '364', '365', '560']
|
|
55,papers on flow visualization on slender conical wings .,"['16', '375', '460', '378', '255', '271', '376', '377', '562', '502']"
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|
56, |
|
flow conditions over a bluff cylindrical body of finite aspect ratio .","['380', '749', '1339', '14', '705', '779', '780', '379', '643', '686']
|
|
57, |
|
theory .","['380', '593', '746', '914', '14', '379', '705', '779', '780', '704', '12', '15', '857', '859']
|
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58, |
|
using free-flight models) compare with similar measurements made in |
|
a low-blockage wind tunnel .","['788', '785', '786', '787', '23', '381', '382', '784', '789']
|
|
59, |
|
basis .","['788', '785', '786', '787']
|
|
61, |
|
gases .","['565', '566', '564', '1159', '661']
|
|
62, |
|
suddenly heated wall .","['566', '567', '1084', '1078', '1081']
|
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66,are there any theoretical methods for predicting base pressure .,"['664', '629', '180', '659', '660']"
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67,does transition in the hypersonic wake depend on body geometry and size,"['2', '3', '664', '629', '323', '324', '393', '128', '180', '394', '659', '389', '4', '1302']"
|
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68,how can one detect transition phenomena in boundary layers .,"['662', '101', '460', '661', '62']"
|
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69,how can one detect transition phenomena in hypersonic wakes .,"['458', '570', '977', '62', '336']"
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71, |
|
wake behind a cruciform wing .","['569', '571', '1355', '101', '655', '1213', '798', '572']
|
|
72, |
|
round leading edge be validly analyzed by the linearized transonic flow |
|
theory .","['21', '324', '630', '94', '664', '304', '128', '323', '663', '570', '494', '305', '309', '571', '655', '388', '62']
|
|
74, |
|
analysed in a simple approximate way .","['576', '656', '575', '317', '574', '578']
|
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79, |
|
(chapman-enskog theory) .","['597', '598', '688', '708', '713']
|
|
80, |
|
hypersonic viscous interactions .","['594', '597', '596', '598']
|
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81, |
|
hypersonic flow .","['672', '799']
|
|
82, |
|
an insulated flat plate .","['676', '677', '678', '679', '205']
|
|
83,what controls leading-edge attachment at transonic speeds .,"['680', '681', '682', '683']"
|
|
84, |
|
be integrated numerically, using suitable transformations, without |
|
iteration on the boundary conditions .","['606', '406', '608', '142', '294', '354', '522', '962', '1192', '1213', '873']
|
|
85, |
|
characteristics of the boundary layers on slender bodies of revolution .","['608', '406', '606', '710']
|
|
86, |
|
slender bodies of revolution in continuum flow (the ?transverse |
|
curvature effect) .","['594', '790']
|
|
87, |
|
rarefaction on boundary layer flows (the ?slip? effect) .","['606', '611', '562', '50', '236', '609', '612', '406']
|
|
93, |
|
through a rarefied, partially ionized gas in the presence of a magnetic |
|
field .
|
|
94, |
|
by mass transfer at the nose of a blunted cone .","['24', '283', '294', '559', '689', '690', '101', '1393', '354', '1104', '1161', '1395']
|
|
95, |
|
layers be applied to problems involving compressible boundary layers .","['283', '662']
|
|
97, |
|
utilized to predict lifting-surface flutter characteristics .","['699', '700', '701', '698', '1289', '702', '703', '779', '1339', '681']
|
|
98, |
|
which affect the flutter mechanism .","['713', '708', '709', '711', '712']
|
|
99, |
|
from heated cylinders of non-circular cross-section, (the fluid flow |
|
being along the generators) .","['717', '719', '1001', '1379']
|
|
100, |
|
cylinders .","['821', '822', '824', '820', '823', '825', '1122', '1051', '1121']
|
|
101, |
|
of the mixing problem (i.e. the blasius problem with three-point |
|
boundary conditions) .","['817', '818', '819', '820', '825', '824']
|
|
102, |
|
around a yawed cylinder .","['728', '913', '910', '911']
|
|
103, |
|
is the velocity just outside of the boundary layer a linear function of |
|
the distance around the cylinder .","['826', '828']
|
|
104,where can i find pressure data on surfaces of swept cylinders .,"['833', '834', '835', '836', '837']"
|
|
105, |
|
place of vibrational shapes . if so, can we provide a justification by |
|
means of an example .","['848', '844', '845', '846', '847']
|
|
106, |
|
pressure gradient .","['847', '846', '849', '844', '845']
|
|
107, |
|
flow problem be applied when the main stream is a shear flow .","['725', '728', '729', '911', '720', '75', '909']
|
|
108, |
|
a shear flow .","['724', '726', '727', '75', '909', '720', '723']
|
|
109, |
|
distribution corresponding to an isothermal transpiration cooled |
|
hemisphere .","['860', '861', '606', '980', '12']
|
|
110, |
|
equations .","['862', '863', '31', '1174']
|
|
111,previous solutions to the boundary layer similarity equations .,"['15', '391', '864', '914', '392', '627', '658']"
|
|
112,experimental results on hypersonic viscous interaction .,"['731', '730']"
|
|
113, |
|
number flows, particularly at high mach numbers .","['746', '748', '749', '265']
|
|
114, |
|
equilibrium) play in the similitude laws governing hypersonic flows over |
|
slender aerodynamic bodies .","['919', '916', '920', '921']
|
|
116, |
|
with respect to the realization of hypersonic simulation in high |
|
enthalpy wind tunnels .","['922', '360', '605', '927', '492']
|
|
118, |
|
on stagnation-point heat transfer result primarily from the |
|
differences in the viscosity-temperature law assumed .","['923', '924', '925']
|
|
119, |
|
assumed in some of the analyses of hypersonic shock layer at low |
|
reynolds number .
|
|
120, |
|
experiments in the low reynolds number (merged-layer) regime .","['829', '887', '890', '885', '886', '888', '889', '1146', '891']
|
|
121, |
|
axial compressor .","['885', '886', '1146', '887', '888', '890', '891']
|
|
122, |
|
numbers and comparison been made with theoretical work .","['931', '932', '934', '935', '936', '937', '938', '957', '1131']
|
|
123, |
|
could be adopted for use in short running time facilities .","['966', '967']
|
|
126, |
|
mounted off-centre in a tunnel .","['974', '1326', '187', '969', '970', '971', '972', '973']
|
|
128, |
|
distributions on swept wings in subsonic flow compare with each other and with |
|
experiment .","['985', '990']
|
|
130,what is the present state of the theory of quasi-conical flows .,"['766', '858', '859', '1008', '12']"
|
|
131, |
|
aerodynamic heat transfer to conical bodies for both laminar and turbulent |
|
flow .","['1014', '1020', '1013', '1016', '1017', '1012', '1018', '1019']
|
|
132, |
|
from laminar to turbulent flow on a model in a wind tunnel .","['1014', '1013', '1015', '1016', '1012', '1018', '1019', '1017', '951', '1023', '1020', '952', '1024', '1025', '1026']
|
|
133, |
|
oscillatory derivatives on slender sting-mounted models in supersonic |
|
wind tunnels .","['1020', '1018', '1019', '1024', '1012', '1016', '1022']
|
|
135, |
|
behind the shock, neglecting effects of leading edge and corner .","['1018', '1017', '1023', '1024', '1025', '1026', '950', '1016']
|
|
136, |
|
an atmosphere in which the scale height varies with altitude .","['1021', '1022', '1034']
|
|
137, |
|
from that on a closely-related tapered sweptback wing .","['1029', '1034', '951', '1021']
|
|
138,recent data on shock-induced boundary-layer separation .,"['846', '1036']"
|
|
139,what interference effects are likely at transonic speeds .,"['1031', '1032', '1035', '1037']"
|
|
140, |
|
would be used in order to minimize sonic boom intensity, and is there a |
|
limit to the degree of minimizing that can be accomplished .","['1038', '1039', '1041', '1042', '1043', '1044']
|
|
141, |
|
medium and predict, within experimental accuracies, the results |
|
obtained in air .","['1038', '1041', '1043', '1044', '1039', '1042']
|
|
142, |
|
blunt body .
|
|
143,what is the theoretical heat transfer distribution around a hemisphere .,"['1043', '1044']"
|
|
145, |
|
wings in subsonic flow .","['763', '838', '839', '1045', '743', '852', '841']
|
|
146, |
|
gusts or blasts in the subsonic regime .","['840', '1045']
|
|
147, |
|
speeds and how do they compare with conventional trailing-edge |
|
flaps .","['889', '1046', '1048', '1047', '1049', '1051', '1050', '843', '926', '822']
|
|
148, |
|
atmosphere, is it possible to predict when and how it will stop |
|
tumbling and its subsequent motion .","['889', '1048', '1050', '1046', '1049', '843']
|
|
149, |
|
cylindrical shells under axial compression .","['1057', '1058', '1059', '1052', '930', '931', '934', '936', '937', '938', '1131']
|
|
150, |
|
stress-strain relationship differ greatly when applied to stability |
|
problems .","['1074', '1075']
|
|
152,basic dynamic characteristics of structures continuous over many spans .,"['1076', '1077', '569', '572', '687', '655']"
|
|
153,is the information on the buckling of sandwich sphere available .,"['1078', '1083', '1084', '1080', '1081', '1082', '1085']"
|
|
154, |
|
material being inelastic and a non uniform temperature being present .","['1087', '1088']
|
|
155, |
|
vibrations of a cylindrical shell .","['1103', '1100', '983', '1101', '1104', '1099']
|
|
156,experimental techniques in shell vibration .,"['983', '1102', '1097', '1100', '274', '1096', '1098', '1099', '1103', '982', '1104', '553', '1101', '82']"
|
|
157, |
|
typical aircraft structure in a noise environment is it possible to |
|
develop a design procedure .","['273', '1105', '1106', '93', '161', '302', '122', '666', '1107', '556', '25', '1011', '19', '35', '1355', '372', '410', '456', '36', '44', '215', '626', '1151', '354', '369', '370', '421', '557', '605', '655', '657', '689', '1307', '318', '423', '1304', '160', '482', '572']
|
|
158,what data is there on the fatigue of structures under acoustic loading .,"['302', '1011', '552', '998', '1009', '1010', '273', '556']"
|
|
160,panels subjected to aerodynamic heating .,"['1134', '1137', '1138', '1135', '1136']"
|
|
161, |
|
buckling change the buckling mode .","['54', '1386', '562', '336', '55', '996']
|
|
163, |
|
previous papers on panel flutter .","['20', '56', '57']
|
|
164, |
|
of bending, been reduced to two successive membrane boundary value |
|
problems .","['311', '415', '416', '798', '316', '335', '1364', '1367']
|
|
165, |
|
at transonic mach numbers .","['71', '72']
|
|
167, |
|
oscillating in transonic flow can be determined by purely analytical |
|
methods . is it possible to determine the airforces on a single |
|
particular planform, such as the rectangular one by such method .","['274', '82']
|
|
168, |
|
aeroelastic effects in heated flow as intractable as previous investigations |
|
imply .","['217', '774']
|
|
169, |
|
cylindrical portion of a cone-cylinder configuration .","['118', '157', '774', '775']
|
|
170, |
|
the normal force on the body of various angles of incidence .","['139', '238', '239', '904', '906', '672']
|
|
171, |
|
lift of a fin-body combination .","['252', '431', '141']
|
|
173, |
|
on the non linear (large-deflection) load-deflection response of |
|
cylinders under hydrostatic pressure .","['367', '451']
|
|
175, |
|
cylindrical shells unnecessarily involved or even inaccurate due to the |
|
assumed forms of buckling mode .","['351', '966', '967', '964', '965']
|
|
176, |
|
thermal buckling or due to mechanical loading .","['582', '583', '584', '585', '978', '586', '982']
|
|
177, |
|
conical shells . how do the results compare with experiment .","['588', '589', '592', '772', '590']
|
|
181, |
|
viscous flow in a straight channel .","['973', '974', '409', '997', '1061']
|
|
182, |
|
compressible flow in slender channels a problem . |
|
what analytical investigations have been made of the stability of |
|
conical shells . how do the results compare with experiment .","['685', '686']
|
|
183,jet interference with supersonic flow -dash experimental papers .,"['803', '808', '802', '807', '811', '253', '804', '805', '806', '809', '810', '1243', '1247']"
|
|
184,thrust vector control by fluid injection -dash papers .,"['32', '67', '715', '717', '716', '499', '1379']"
|
|
187, |
|
heat equation for an exponential (in time) heat input .","['838', '839', '840', '743', '842', '1045']
|
|
189, |
|
computer .","['395', '866', '869', '865', '868', '870', '867', '872', '873']
|
|
190, |
|
three-dimensional equations for incompressible nonviscous flow .","['15', '391', '285', '390', '864']
|
|
196, |
|
x-15 vertical stabilizer when subjected to aerodynamic heating .","['51', '185', '874', '878', '879', '880', '12', '875', '876', '202', '746', '13']
|
|
200, |
|
times and experimentally measured collapse times for compressed columns |
|
in creep .","['1134', '1137', '1138']
|
|
201,theoretical studies of creep buckling .,"['552', '625', '1296', '93', '1151', '401', '110', '1391', '423', '541', '1295', '318', '1304', '160', '369', '482']"
|
|
202,experimental studies of creep buckling .,"['1303', '1304', '1309', '1306', '1308', '605', '602', '603', '604', '1110', '1305', '1310', '48', '232']"
|
|
203, |
|
different structures within the framework of a single theory .","['58', '1305', '1306', '602', '603', '604', '1307', '1310', '19', '232', '323', '688', '122', '1188']
|
|
204,what are the experimental results for the creep buckling of columns .,"['572', '1311', '63', '540', '602', '603', '604', '1305', '1188', '307', '1213', '655', '1355', '68']"
|
|
205, |
|
external pressure .","['1321', '1322']
|
|
206, |
|
mechanism associated with creep collapse for a long circular cylindrical |
|
shell which exhibits both primary and secondary creep as well as elastic |
|
deformations under various distributed force systems .","['1338', '1341', '1340']
|
|
208, |
|
circular cylindrical shells, been investigated .","['163', '1344', '1345', '164', '1347', '1346']
|
|
209, |
|
the frequencies of vibration of circular cylindrical shells been |
|
investigated .","['1351', '1356', '1350', '187', '487', '45', '55', '316', '1383', '1385', '1106', '1228']
|
|
210, |
|
structures .","['1171', '891', '1172', '1173', '1030', '1174']
|
|
211, |
|
shells of revolution .","['891', '1172', '1173', '1174', '763', '769', '1030', '1031', '1033', '1052', '1068']
|
|
212, |
|
on cylindrical pressure vessels .","['888', '889', '1178', '885', '887', '886', '841', '1176', '1177', '890', '769', '891', '1173', '843']
|
|
213, |
|
revolution are available .","['888', '885', '887', '889', '1178', '769', '1173', '1177', '886', '890', '843']
|
|
214, |
|
but maintaining their shape by virtue of internal pressure provide any |
|
insight into the behaviour of pressurized cylinders with finite wall |
|
stiffness .","['833', '1361', '1362', '1363']
|
|
215, |
|
theory analyses available for pressurized cylinders in bending .","['37', '35']
|
|
216, |
|
membrane cylinders in bending can be predicted .
|
|
217, |
|
corrugated core sandwich cylinders .","['666', '667', '1258', '1394', '668', '670', '1204', '1391', '1395', '1300', '37', '559', '630', '1107', '1213']
|
|
218,papers on small deflection theory for buckling of sandwich cylinders .,"['24', '101', '666', '667', '93', '1258', '1393', '559', '630', '662', '1104', '1107', '1204', '1213', '1300']"
|
|
219, |
|
deflection behaviour of conical shells .","['1391', '666', '667', '1258', '1078', '1080', '1081', '1394', '1395', '1214', '1198', '1204', '1300', '559', '630', '662', '1107', '1213']
|
|
223, |
|
at high supersonic mach number .","['400', '1387', '1392', '1398']
|
|
224, |
|
surface of a wing alone .","['656', '1313', '1317', '1316', '1318', '1319', '1157', '1274']
|
|
225, |
|
and what is its magnitude .","['1379', '1305', '1304', '40', '293', '1309', '161', '421', '1377', '1378', '1381', '225', '1380', '448', '449', '1124', '1280', '433', '923', '924', '1062', '1074', '1075', '1213']
|
|
226,how should the navier-stokes difference equations be solved .,[]
|
|
227, |
|
difference equations is most rapidly convergent .
|
|
230,technical report on measurement of ablation during flight .,[]
|
|
231, |
|
materials research .
|
|
232, |
|
with experiment for a wide range of free stream conditions and body |
|
shapes .
|
|
233,what are the available properties of high-temperature air .,[]
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234, |
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of a slender body of revolution characteristic of launch vehicles .
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241, |
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the possibility of buckling under internal pressure . has anyone |
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investigated for which ranges of shell parameters these stresses are |
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sufficiently large to cause elastic buckling .
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245, |
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method of calculating the laminar separate point for various |
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incompressible and compressible boundary layers with zero heat transfer .
|
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246, |
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various incompressible and compressible boundary layers with zero heat |
|
transfer are available .
|
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247, |
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predicting surface pressures of an ogive forebody at angle of attack .
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250,what determines the onset of shock-induced boundary-layer separation .,[]
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251, |
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moving wave known .
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252, |
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boundary layer induced by a moving wave .
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253, |
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material ablating at high temperatures in a hypersonic flight |
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environment .
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254, |
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flow in the throat of a nozzle, i.e. finding the flow in a given |
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nozzle .
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255, |
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transonic flow in the throat of a nozzle, i.e. finding a nozzle which |
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has a given axial velocity distribution .
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257, |
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calibrations appear to be,. - (a) significantly different from those formerly |
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specified, (b) wildly variable at low reynolds numbers .
|
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259, |
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using free-flight models and similar measurements made in a low-blockage |
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wind tunnel .
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261,solution of the blasius problem with three-point boundary conditions .,[]
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264, |
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differential equations with periodic coefficients .
|
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265, |
|
data .
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266,work on flow in channels at low reynolds numbers .,[]
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267, |
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other than biot's principle .",[]
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268,"what mode of stalling can be expected for each stage of an axial |
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compressor .",[]
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269,"has a criterion been established for determining the axial compressor |
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choking line .",[]
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272,"has a theory of quasi-conical flows been developed, in supersonic |
|
linearised theory, for which the upwash distribution on the lifting |
|
surface, apart from being a homogeneous function in the |
|
co-ordinate, is permitted to have a quite general functional form .",[]
|
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273,how does scale height vary with altitude in an atmosphere .,[]
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274,"jet interference with supersonic flows |
|
theoretical papers .",[]
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275,"effects of leading-edge bluntness on the flutter characteristics of some |
|
square-planform double-wedge airfoils at mach numbers less than 15.4.",[]
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|
277,"what factors have been shown to have a primary influence on sonic boom |
|
strength .",[]
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283,work on small-oscillation re-entry motions .,[]
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284,experimental studies on panel flutter .,[]
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|
285,"how can wing-body, flow field interference effects be approximated |
|
rationally .",[]
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288,"has anyone analytically or experimentally investigated the effects of |
|
internal pressure on the buckling of circular-cylindrical shells under |
|
bending .",[]
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|
291,"what theoretical and experimental work has been done on the excitation |
|
and response of typical structures in a noise environment .",[]
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|
292,"is there a design method for calculating thermal fatigue endurances of |
|
components of various types and sizes in a variety of circumstances .",[]
|
|
293,"will an analysis of panel flutter based on arbitrarily assumed modes of |
|
deformation prove satisfactory, and if so, what is the minimum number |
|
of modes that need be considered .",[]
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294,"what is the criterion for true panel flutter, as opposed to small |
|
amplitude vibration arising from acoustic disturbances .",[]
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295,papers dealing with uniformly loaded sectors .,[]
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296,general methods of solving clamped plate problems .,[]
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297,"how can the analytical solution of the buckling strength of a uniform |
|
circular cylinder loaded in axial compression be refined so as to lower |
|
the buckling load .",[]
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298,"in the problem of the buckling strength of uniform circular cylinders |
|
loaded in axial compression, does the linear solution help with |
|
improving the non-linear one .",[]
|
|
299,"the problem of similarity for representative investigation of |
|
aeroelastic effects in a flow with the absence of heating effects .",[]
|
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300,how is fatigue damage estimated using the normal long-hand method .,[]
|
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301,"is there any information available on the difference in the effects of |
|
various edge conditions on the buckling of cylindrical shells .",[]
|
|
303,"have non-linear large deflection analyses been conducted for shell |
|
shapes other than conical .",[]
|
|
304,"are asymptotic methods sufficiently accurate in the determination of |
|
pre-buckling stresses in torispherical shells, or must we resort to |
|
numerical methods .",[]
|
|
306,"what are the nonequilibrium chemical constituents in the viscous shock |
|
layer ahead of a blunt re-entry vehicle .",[]
|
|
314,"how accurate are existing analytical theories in estimating pressure |
|
distributions on cones at incidence, at hypersonic speeds .",[]
|
|
315,"are simple empirical methods of any use for estimating pressure |
|
distribution in cones .",[]
|
|
316,do viscous effects seriously modify pressure distributions .,[]
|
|
317,"has anyone investigated theoretically whether surface flexibility |
|
can stabilize a laminar boundary layer .",[]
|
|
321,"how do subsonic and transonic flutter data measured in the new langley |
|
transonic dynamics tunnel compare with similar data obtained in other |
|
facilities .",[]
|
|
323,"how do large changes in new mass ratio quantitatively affect |
|
wing-flutter boundaries .",[]
|
|
327,"what is the effect of the shape of the drag polar of a lifting |
|
spacecraft on the amount of reduction in maximum deceleration obtainable by |
|
continuously varying the aerodynamic coefficients during re-entry .",[]
|
|
331,"what are the physical significance and characteristics of separated |
|
laminar and turbulent boundary layer flows .",[]
|
|
332,"has anyone analytically investigated the stabilizing influence of soft |
|
elastic cores on the buckling strength of cylindrical shells subjected |
|
to non-uniform external pressure .",[]
|
|
333,"what papers are available on the buckling of empty cylindrical shells |
|
under non-uniform pressure .",[]
|
|
335,"what effect do thermal stresses have on the compressive buckling |
|
strength of ring-stiffened cylinders .",[]
|
|
336,"what is the effect on cylinder buckling of a circumferential stress |
|
system that varies in the axial direction .",[]
|
|
338,"can non-linear shallow shell analysis be reduced to an engineering |
|
technique by use of the matrix .",[]
|
|
339,"is it possible to predict the shape of a shroud which will allow |
|
simulation of the nose region flow field for a sphere in hypersonic flow .",[]
|
|
340,"what investigations have been made of the wave system created by a |
|
static pressure distribution over a liquid surface .",[]
|
|
347,"has anyone investigated the effect of shock generated vorticity on heat |
|
transfer to a blunt body .",[]
|
|
348,what is the heat transfer to a blunt body in the absence of vorticity .,[]
|
|
349,"what are the general effects on flow fields when the reynolds number is |
|
small .",[]
|
|
352,"find a calculation procedure applicable to all incompressible laminar |
|
boundary layer flow problems having good accuracy and reasonable |
|
computation time .",[]
|
|
353,"papers applicable to this problem (calculation procedures for laminar |
|
incompressible flow with arbitrary pressure gradient) .",[]
|
|
355,has anyone investigated the shear buckling of stiffened plates .,[]
|
|
356,papers on shear buckling of unstiffened rectangular plates under shear .,[]
|
|
360,"in practice, how close to reality are the assumptions that the flow |
|
in a hypersonic shock tube using nitrogen is non-viscous and in |
|
thermodynamic equilibrium .",[]
|
|
365,"what design factors can be used to control lift-drag ratios at mach |
|
numbers above 5 .",[]
|
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