EP0329524B1 - Dispositif de calcul du pas d'intégration de trajectoire d'obus - Google Patents
Dispositif de calcul du pas d'intégration de trajectoire d'obus Download PDFInfo
- Publication number
- EP0329524B1 EP0329524B1 EP19890400336 EP89400336A EP0329524B1 EP 0329524 B1 EP0329524 B1 EP 0329524B1 EP 19890400336 EP19890400336 EP 19890400336 EP 89400336 A EP89400336 A EP 89400336A EP 0329524 B1 EP0329524 B1 EP 0329524B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- trajectory
- integration step
- shell
- values
- point
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
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Images
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F41—WEAPONS
- F41G—WEAPON SIGHTS; AIMING
- F41G3/00—Aiming or laying means
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F41—WEAPONS
- F41G—WEAPON SIGHTS; AIMING
- F41G3/00—Aiming or laying means
- F41G3/14—Indirect aiming means
- F41G3/142—Indirect aiming means based on observation of a first shoot; using a simulated shoot
Definitions
- the present invention relates to a device for calculating the integration pitch of a shell trajectory.
- the subject of the present invention is a device for calculating such an optimized integration step, that is to say the maximum integration step compatible with the required precision, making it possible to save on the integration time of the trajectories. without losing on the precision of the integration calculation.
- the set of these variables constitutes a point P of the trajectory.
- time limit noted h limit
- firing configurations T each of which is characterized by the following parameters: firing conditions applied to the cannon, geographic and meteorological data, characteristics of the shell (mass, ejection speed).
- This method is relatively costly in calculation time, but it does not have to be implemented in the field, in the calculation means associated with the firing battery; it will advantageously be implemented beforehand, with more efficient calculation means than those associated with the firing battery, the performance of which is obviously limited for reasons of bulk. Since this database cannot be exhaustive, it is necessary, if we want to effectively reduce the time taken to calculate trajectories in the field, using the calculation means associated with the firing battery, to determine a means quick calculation of the h lim value corresponding to any point P, from this database and according to the parameters existing at the point considered and the firing configuration considered.
- explanatory variables that is, variables according to which the variable to be modeled h lim is expressed according to a certain function.
- This geometrically amounts to carrying out a projection of the set of points representing h lim in the space of the different variables "x" of the set (T, X, ⁇ p ), on each plans (h lim , x), then to select those of these variables "x" having the strongest explanatory power.
- h lim is expressed linearly, by domain, of the explanatory variables.
- M denotes the Mach number (ratio of the speed of the shell to the speed of sound)
- P r the local pressure
- m the mass of the shell
- T e temperature
- U o speed of ejection of the shell.
- Each of the eight zones thus defined corresponds to a set of coefficients b i 1, b i 2, b i 3, b i 4, b i 5 (1 ⁇ i ⁇ 8) used in the expression of the above model. These different cases will appear in FIG. 3 which will be described later.
- the model is represented graphically making it possible to approximate h lim in a limited space for greater clarity with the two explanatory variables ⁇ p and M ⁇ 2 and in this space we have only considered the case M> M0 (zone " High Mach ").
- This model is constituted by a succession of planes which each project, as represented on figure 2a, in each of the planes (h lim , ⁇ p ) and (h lim , M ⁇ 2) according to the line segments resulting from the modeling linear.
- the values of the parameters which it is necessary to know at the point considered are the values of the parameters M, U X , U Y , U Z , A0, T e , P r , U o , W X , m.
- the parameters U X , U Y , U Z designate the components of the absolute speed of the shell at the point considered; A0 denotes the rise of the barrel.
- the value of the increase A0 is necessary for the calculation of the tolerable position error by step ⁇ p at the point considered.
- This modeling of ⁇ p is obtained from a database ( ⁇ p , T) which can itself be obtained in the following way.
- the invention makes it possible to significantly reduce the calculation times and to dispense with operators specialized in the calculation means associated with the firing battery; the architecture of these is simplified and their energy consumption reduced, which is fundamental for problems of portability and autonomy.
- the device according to the invention makes it possible to reduce this number to around twenty.
Landscapes
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Management, Administration, Business Operations System, And Electronic Commerce (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR8801857 | 1988-02-17 | ||
FR8801857A FR2627302B1 (fr) | 1988-02-17 | 1988-02-17 | Procede et dispositif de calcul du pas d'integration de trajectoire d'obus |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0329524A1 EP0329524A1 (fr) | 1989-08-23 |
EP0329524B1 true EP0329524B1 (fr) | 1993-05-12 |
Family
ID=9363327
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP19890400336 Expired - Lifetime EP0329524B1 (fr) | 1988-02-17 | 1989-02-07 | Dispositif de calcul du pas d'intégration de trajectoire d'obus |
Country Status (4)
Country | Link |
---|---|
EP (1) | EP0329524B1 (da) |
DE (1) | DE68906418T2 (da) |
DK (1) | DK66489A (da) |
FR (1) | FR2627302B1 (da) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2294133B (en) * | 1994-10-11 | 1999-08-18 | Accuracy Int Ltd | Ballistic calculator |
DE102005023739A1 (de) | 2005-05-17 | 2006-12-07 | Krauss-Maffei Wegmann Gmbh & Co. Kg | Verfahren zur Ermittlung einer Feuerleitlösung |
DE102006036257A1 (de) * | 2006-08-03 | 2008-02-07 | Rheinmetall Defence Electronics Gmbh | Bestimmung der einzustellenden Ausrichtung einer ballistischen Waffe |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2459443A1 (fr) * | 1979-06-15 | 1981-01-09 | Thomson Brandt | Procede et dispositif de determination des elements de tir d'un projectile |
SU860082A1 (ru) * | 1979-10-03 | 1981-08-30 | Таганрогский радиотехнический институт им. В.Д.Калмыкова | Стохастический интегратор |
GB2094950B (en) * | 1981-03-12 | 1984-08-30 | Barr & Stroud Ltd | Gun fire control systems |
GB2098705A (en) * | 1981-05-15 | 1982-11-24 | Marconi Co Ltd | A gun aiming arrangement |
-
1988
- 1988-02-17 FR FR8801857A patent/FR2627302B1/fr not_active Expired - Lifetime
-
1989
- 1989-02-07 EP EP19890400336 patent/EP0329524B1/fr not_active Expired - Lifetime
- 1989-02-07 DE DE1989606418 patent/DE68906418T2/de not_active Expired - Fee Related
- 1989-02-13 DK DK66489A patent/DK66489A/da not_active Application Discontinuation
Also Published As
Publication number | Publication date |
---|---|
DE68906418D1 (de) | 1993-06-17 |
DE68906418T2 (de) | 1993-09-09 |
DK66489D0 (da) | 1989-02-13 |
DK66489A (da) | 1989-08-18 |
EP0329524A1 (fr) | 1989-08-23 |
FR2627302B1 (fr) | 1990-06-08 |
FR2627302A1 (fr) | 1989-08-18 |
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