To meet the demand for the accurate measurements of the dynamic pressure of a shock wave, a composite dynamic pressure sensor design method is proposed based on the formation mechanism, propagation characteristics, special testing environment of the dynamic pressure, and Pitot tube structure. The dynamic pressure of the shock wave is evaluated by the total pressure and static pressure units installed in the composite sensor. FLUENT simulation software was used to analyze the aerodynamic characteristics of the dynamic pressure sensor, and parameters such as the structural size and inlet position of the sensor were determined. In response to the special experimental environment of the shock wave, the requirements for the dynamic pressure measurements under damage conditions were analyzed, and a dynamic pressure testing system was established. Dynamic pressure tests with four 2,4,6-trinitrotoluene [C7H5(NO2)3] equivalents of 1, 2, 15, and 20 kg were carried out. The experimental results show that the proposed sensor design method can accurately and effectively measure the dynamic pressure signal, and the dynamic pressure gain multiple decreases with an increase in the proportional distance. This provides an effective testing method for evaluating the dynamic pressure damage effect of ammunition systems.

1.
L.
Ehrhardt
,
J.
Boutillier
,
P.
Magnan
,
C.
Deck
,
S.
De Mezzo
,
R.
Willinger
, and
S.
Cheinet
, “
Evaluation of overpressure prediction models for air blast above the triple point
,”
J. Hazard. Mater.
311
,
176
185
(
2016
).
2.
S. A.
Formby
and
R. K.
Wharton
, “
Blast characteristics and TNT equivalence values for some commercial explosives detonated at ground level
,”
J. Hazard. Mater.
50
,
183
198
(
1996
).
3.
X. S.
Kong
,
W. G.
Wu
,
J.
Li
,
X. B.
Li
, and
S. X.
Xu
, “
Experimental investigation on characteristics of blast load in partially confined cabin structure
,”
J. Shanghai Jiaotong Univ.
18
(
5
),
583
589
(
2013
).
4.
P. E.
Sauvan
,
I.
Sochet
, and
S.
Trélat
, “
Analysis of reflected blast wave pressure profiles in a confined room
,”
Shock Waves
22
,
253
264
(
2012
).
5.
F.
Bai
,
Y.
Liu
,
J. B.
Yan
,
Y. L.
Xu
,
Z. Q.
Shi
, and
F. L.
Huang
, “
Study on the characteristics of blast loads due to two simultaneous detonated charges in real air
,”
Int. J. Non-Linear Mech.
146
,
104108
(
2022
).
6.
Y.
Huang
,
S. J.
Zhu
, and
S.
Chen
, “
Deep learning-driven super-resolution reconstruction of two-dimensional explosion pressure fields
,”
J. Build. Eng.
78
,
107620
(
2023
).
7.
X. L.
Li
,
X.
Wang
,
Z. H.
Lu
,
M.
Li
,
W.
Cao
,
K. Q.
Chen
,
P. Y.
Xue
,
H. J.
Huang
,
C.
Hua
, and
D. Y.
Gao
, “
Numerical simulations of trajectories of shock wave triple points in near-ground explosions of TNT charges
,”
Energ. Mater. Front.
3
,
61
67
(
2022
).
8.
X.
Zhang
,
Y.
Ding
, and
Y.
Shi
, “
Numerical simulation of far-field blast loads arising from large TNT equivalent explosives
,”
J. Loss Prev. Process Ind.
70
,
104432
(
2021
).
9.
W. F.
Xiao
,
M.
Andrae
, and
N.
Gebbeken
, “
Air blast TNT equivalence factors of high explosive material PETN for bare charges
,”
J. Hazard. Mater.
377
,
152
162
(
2019
).
10.
J.
Boutillier
,
L.
Ehrhardt
,
S.
De Mezzo
,
C.
Deck
,
P.
Magnan
,
P.
Naz
, and
R.
Willinger
, “
Evaluation of the existing triple point path models with new experimental data: Proposal of an original empirical formulation
,”
Shock Waves
28
,
243
252
(
2018
).
11.
S.
Pochwała
and
J.
Pospolita
, “
Analysis of applicability of flow averaging Pitot tubes in the areas of flow disturbance
,”
Metrol. Meas. Syst.
23
,
71
84
(
2016
).
12.
J.
Kutin
and
A.
Svete
, “
On the theory of the frequency response of gas and liquid pressure measurement systems with connecting tubes
,”
Meas. Sci. Technol.
29
,
125108
(
2018
).
13.
A.
Svete
and
J.
Kutin
, “
Experimental validation of an improved mathematical model for pneumatic pressure measurement systems with connecting tubes
,”
Meas. Sci. Technol.
31
,
015101
(
2020
).
14.
S.
Sediva
and
M.
Uher
, “
Analysis of the effect of body shape of multiport averaging Pitot tube on permanent pressure loss using ANSYS/FLUENT
,”
IFAC Proc. Vol.
45
,
322
326
(
2012
).
15.
E. D.
Esparza
, “
Blast measurements and equivalency for spherical charges at small scaled distances
,”
Int. J. Impact Eng.
4
,
23
40
(
1986
).
16.
S.
Hank
,
R.
Saurel
,
O.
Le Métayer
, and
E.
Lapébie
, “
Modeling blast waves, gas and particles dispersion in urban and hilly ground areas
,”
J. Hazard. Mater.
280
,
436
449
(
2014
).
17.
A.
Svete
,
F. J.
Hernández Castro
, and
J.
Kutin
, “
Effect of the dynamic response of a side-wall pressure measurement system on determining the pressure step signal in a shock tube using a time-of-flight method
,”
Sensors
22
(
6
),
2103
(
2022
).
18.
Z. Q.
Xue
,
S. P.
Li
,
C. L.
Xin
,
L. P.
Shi
, and
H. B.
Wu
, “
Modeling of the whole process of shock wave overpressure of free-field air explosion
,”
Defence Technol.
15
(
5
),
815
820
(
2019
).
19.
F.
Yin
,
X. D.
Zhi
,
F.
Fan
,
W. C.
Wei
, and
D. S.
Zheng
, “
Blast loads and variability on cylindrical shells under different charge orientations
,”
Sci. Rep.
13
,
6719
(
2023
).
20.
Y.
Li
,
W.
Wang
, and
Z.
Chen
, “
An innovative failure criterion for metal cylindrical shells under explosive loads
,”
Materials
15
,
4376
(
2022
).
21.
P. W.
Sielicki
and
T.
Gajewski
, “
Numerical assessment of the human body response to a ground-level explosion
,”
Comput. Methods Biomech. Biomed. Eng.
22
,
180
205
(
2019
).
22.
T. C. J.
Hu
and
I. I.
Glass
, “
Blast wave reflection trajectories from a height of burst
,”
AIAA J.
24
,
607
(
2012
).
23.
N. W.
Mohottige
,
C.
Wu
, and
H.
Hao
, “
Characteristics of free air blast loading due to simultaneously detonated multiple charges
,”
Int. J. Struct. Stab. Dyn.
14
,
1450002
(
2014
).
24.
Y.
Li
and
H.
Aoude
, “
Blast response of beams built with high-strength concrete and high-strength ASTM A1035 bars
,”
Int. J. Impact Eng.
130
,
41
67
(
2019
).
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