JPS599744B2 - rocket engine - Google Patents
rocket engineInfo
- Publication number
- JPS599744B2 JPS599744B2 JP2328575A JP2328575A JPS599744B2 JP S599744 B2 JPS599744 B2 JP S599744B2 JP 2328575 A JP2328575 A JP 2328575A JP 2328575 A JP2328575 A JP 2328575A JP S599744 B2 JPS599744 B2 JP S599744B2
- Authority
- JP
- Japan
- Prior art keywords
- combustion
- rocket
- grain
- present
- thrust
- 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
Links
- 238000002485 combustion reaction Methods 0.000 claims description 40
- 239000000463 material Substances 0.000 claims description 10
- 235000015842 Hesperis Nutrition 0.000 description 2
- 235000012633 Iberis amara Nutrition 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000005452 bending Methods 0.000 description 1
- 239000003380 propellant Substances 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 230000001502 supplementing effect Effects 0.000 description 1
Landscapes
- Testing Of Engines (AREA)
Description
【発明の詳細な説明】
本発明は高々度飛翔体として好適なロケットエンジンに
関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a rocket engine suitable for use as a high-altitude flying object.
周知のごとく、高々度に飛翔体を効果的に到達させる様
打上げるにはそのロケットエンジンの推力と推力の作用
時間(通常作動時間という)の最適の組合せがある。As is well known, in order to effectively launch a projectile to a high altitude, there is an optimal combination of the thrust of the rocket engine and the operating time of the thrust (normal operating time).
(特許出願公告昭41−762号、特許出願公告昭41
−6762号)。(Patent Application Publication No. 1976-762, Patent Application Publication No. 1972)
-6762).
従来のロケットは最適な推力X時間の組合せが得られな
い内面燃焼形式が殆どであった。Most conventional rockets were of the internal combustion type, which did not provide the optimal combination of thrust and time.
一部上記特許願による高燃焼速度推進剤等を軸上に埋込
んだ特殊端面燃焼形式もあるが広範囲に使用されていな
い。There is also a special end-combustion type in which a high-burning-rate propellant, etc. is embedded on the shaft, as disclosed in some of the above-mentioned patent applications, but it is not widely used.
本発明者は現在容易に得られる燃焼速度のグレインのみ
を用いて最適な推力と作動時間の組合せを達成し得るロ
ケットエンジンを得るため種々検討の結果、ロケットチ
ャンバー内に内壁から内側に向って交互に突出し相互に
平行に延びる複数個の平板状燃焼制限材を配置してダレ
インを区画し、グレインの燃焼の進行方向を屈折させ稲
妻状にすることによりその目的を達成したものである。In order to obtain a rocket engine that can achieve an optimal combination of thrust and operating time using only grains with a burning rate that can be easily obtained at present, the present inventor has conducted various studies, and found that grains are placed in the rocket chamber alternately inward from the inner wall. This objective is achieved by arranging a plurality of flat combustion restricting materials that protrude from the grain and extend in parallel to each other to divide the dalein and bend the direction of combustion of the grains into a lightning bolt shape.
即ち本発明はロケットチャンバーにグレインが装填され
、該グレインはロケット中心軸方向に相互に平行に延び
る複数個の平板状燃焼制限材で区画されており、これら
の燃焼制限材はロケットの中心軸を通る縦断面仮想面に
対し左右対称に配置され、且つ横断面に於で一端はロケ
ットチャンバーの内周に固着し他端は内周から離隔して
配設され、グレインの燃焼の進行方向が燃焼制限材の上
記他端に於で屈折される様にしたことを特徴とするロケ
ットエンジンを提供するものである。That is, in the present invention, a rocket chamber is loaded with grains, and the grains are partitioned by a plurality of flat combustion restricting materials that extend parallel to each other in the direction of the rocket's central axis. They are arranged symmetrically with respect to the imaginary plane of the longitudinal section through which they pass, and in the cross section, one end is fixed to the inner periphery of the rocket chamber and the other end is arranged away from the inner periphery, so that the direction of grain combustion is symmetrical to the combustion direction. The present invention provides a rocket engine characterized in that the restricting member is bent at the other end thereof.
内面燃焼形式のロケットの場合は、グレインの燃え進む
距離(以下ウエブという)が通常そのグレインの直径の
25〜30%であるのに対し、本発明のロケットエンジ
ンに於では燃焼制限材2個を左右に1個づつ配置してグ
レインの燃焼の進行方向を1回屈折させた場合でもグレ
インの直径の2倍のウエブが実質上得られ、左右に2個
づつ配置し2回屈折させた場合はグレインの直径の4倍
、3回以上屈折させた場合はそれ以上のウエブが得られ
る。In the case of internal combustion type rockets, the distance that the grains burn (hereinafter referred to as the web) is usually 25 to 30% of the diameter of the grains, but in the rocket engine of the present invention, two combustion restriction materials are used. Even if one is placed on each side and the direction of grain combustion is refracted once, a web twice the diameter of the grain is essentially obtained; if two are placed on each side and refracted twice. A web four times the diameter of the grain, or even more if refracted three or more times, can be obtained.
左右に夫々複数個の燃焼制限材が配置される場合それら
は横断面に於で一端がロケットチャンバーの内周の上下
に交互に固着され、内周から離隔した他端に於で燃焼の
進行方向が稲妻状に順次屈折するように配置されること
は勿論である。When multiple combustion restriction materials are arranged on the left and right sides, one end of the material is fixed alternately above and below the inner periphery of the rocket chamber in cross section, and the other end separated from the inner periphery is fixed in the direction of combustion. Of course, they are arranged so that they are sequentially refracted in the shape of a lightning bolt.
以下本発明の一実施例を図面にもとづいて説明する。An embodiment of the present invention will be described below based on the drawings.
本発明の一実施例である第3図の形状のスラストパター
ンを示すと第2図bに示す様になる。A thrust pattern having the shape shown in FIG. 3, which is an embodiment of the present invention, is shown in FIG. 2b.
又、第2図aのスラストパターンは第1図の内面燃焼形
式のものの代表例であるがこれは第3図の実施例のもの
と寸法及びグレイン1の種類並びに燃焼圧力を同じとし
た場合のものである。The thrust pattern shown in Figure 2a is a typical example of the internal combustion type shown in Figure 1, but it is similar to the thrust pattern shown in Figure 3 when the dimensions, type of grain 1, and combustion pressure are the same. It is something.
本実施例の場合は2回屈折型であるので実質のウエブが
約8倍従って推力は約1/8となっている。In the case of this embodiment, since it is of the twice-bending type, the actual web is about 8 times as large, and therefore the thrust is about 1/8.
実施例の内の2回屈折型の燃焼の進行状態は第4図の燃
焼進行面Aに示す様になる。The progress state of combustion in the double refraction type of the embodiment is as shown in the combustion progress plane A in FIG.
この形状のま\では燃焼の進行方向が屈折する近傍では
燃焼面積の急激な増加がみられるがこれを防ぐには別の
実施例である第7図の様にエンジン2の外周レストリク
ター4の内壁等に稍三角柱状の燃焼制限材3を設置する
方法がある。With this shape, there is a sharp increase in the combustion area in the vicinity where the direction of combustion is bent, but in order to prevent this, another embodiment of the outer circumferential restrictor 4 of the engine 2 as shown in FIG. There is a method of installing a combustion restricting material 3 in the shape of a slightly triangular prism on an inner wall or the like.
尚第4図中1aはグレイン燃焼初期面を示す。Note that 1a in FIG. 4 shows the initial surface of grain combustion.
到達高度と推力X時間が一定の場合に於ける作動時間を
パラメターとして計算した例を第5図に示す。FIG. 5 shows an example of calculating the operating time as a parameter when the altitude reached and the thrust x time are constant.
これはロケット直径が110朋φロケットエンジン部の
長さが2400mmで構造重量及び計器重量を一定とし
たもので垂直上昇で計算した。This was calculated using vertical ascent, assuming that the rocket diameter was 110mm, the length of the rocket engine was 2400mm, and the structural weight and instrument weight were constant.
この第5図の横軸のdに作動時間を示すがこの寸法のロ
ケットに対し内面燃焼形式とした場合のグレイン1の必
要燃焼速度をeに、端面燃焼形式とした場合のそれをf
に、本発明の形式とした場合のそれをgに夫々併記した
。The operating time is shown in d on the horizontal axis of Fig. 5. For a rocket of this size, e is the required combustion speed of grain 1 when the internal combustion type is used, and f is the required combustion speed when the end combustion type is used.
, the format of the present invention is also shown in g.
尚、現在容易に達成可能な燃焼速度は約3mm/see
から約15〜16關/secであるのでその範囲をe,
f,g上に斜線で示した。Incidentally, the combustion speed that can be easily achieved at present is approximately 3 mm/see.
Since it is about 15 to 16 degrees/sec, the range is e,
Indicated by diagonal lines above f and g.
これによると、端面燃焼形式は推力不足により全く効率
が悪く、内面燃焼形式では最適設計時到達高度の約60
%が最高である。According to this, the end combustion type is completely inefficient due to the lack of thrust, and the internal combustion type has an altitude of approximately 60%, which is the optimum design altitude.
% is the highest.
然るに本発明の内の2回屈折の形式によれば現存するグ
レイン1により容易に最適設計が可能であることが判る
。However, according to the two-fold refraction method of the present invention, it is found that an optimal design can be easily achieved using the existing grain 1.
別の実施例を示せば第8図の様な1回屈折型、第9図の
様な3回屈折型等があり、それより多い屈折型も容易に
可能である。Other examples include a one-time refraction type as shown in FIG. 8, a three-time refraction type as shown in FIG. 9, and more refraction types are easily possible.
即ち、本発明により従来の内面燃焼形式により得られる
スラストパターンと端面燃焼形式によるスラストパター
ンの中間のスラストパターンを完全に包含する設計が可
能となった。That is, according to the present invention, it has become possible to design a thrust pattern that is intermediate between the thrust pattern obtained by the conventional internal combustion type and the thrust pattern obtained by the end face combustion type.
本発明のロケットエンジン2により打上げを行う場合初
期の推力が充分でない場合には第6図に示す様に内面燃
焼形式のブースタグレイン5と併用する事によりランチ
ャー離脱時の速度を補う事を配慮すれば良い。When launching with the rocket engine 2 of the present invention, if the initial thrust is not sufficient, consideration should be given to supplementing the speed at the time of launcher separation by using it together with an internal combustion type booster grain 5 as shown in Fig. 6. Good.
尚第6図中6はノズルを示す。In addition, 6 in FIG. 6 indicates a nozzle.
第1図及び第2図は本発明に係る従来例を示し、第1図
は従来の内面燃焼形式のロケットの断面図、第2図は推
力F1時間t曲線のグラフ図を示し、aは第1図の形式
のグラフ図、bは第3図の形式のグラフ図、第3図乃至
第6図は、本発明の一実施例を示し、第3図は、第6図
のI−I線に沿うロケットの断面図、第4図は燃焼進行
状況を示す要部拡大図、第5図は、一実施例における作
動時間t1燃焼速度r到達高度Zの関係のグラフ図を示
し、Cはt r r s c曲線のグラフ図、dはt曲
線のグラフ図、eは内面燃焼形式とした場合の必要燃焼
速度r曲線グラフ図、fは端面燃焼形式とした場合のr
曲線グラフ図、gは本発明の内2回屈折型とした場合の
r曲線グラフ図、第6図は、実際のロケットに適用した
場合のロケットエンジンの一実施例の縦断面図、第7図
乃至第9図は本発明の他実施例を示し、第6図のI−I
線に沿うロケットの断面図である。
A・・・・・・燃焼進行面、1・・・・・・グレイン、
1a・・・・・・グレイン燃焼初期面、2・・・・・帽
ケットエンジン、3・・・・・・燃焼制限材、4・・・
・・・外周レストリクター、5・・・・・・ブースター
グレイン、6・・・・・・ノズル。1 and 2 show a conventional example according to the present invention, FIG. 1 is a sectional view of a conventional internal combustion type rocket, FIG. 2 is a graph of the thrust F1 time t curve, and a is a 1, b is a graph in the format of FIG. 3, FIGS. 3 to 6 show an embodiment of the present invention, and FIG. 4 is an enlarged view of main parts showing the progress of combustion, FIG. 5 is a graph showing the relationship between operating time t1 burning speed r reached altitude Z in one embodiment, C is t r r s A graph of the c curve, d is a graph of the t curve, e is a graph of the required burning rate r curve for internal combustion, f is r for end combustion.
A curve graph diagram, g is an r curve graph diagram when the two-fold refraction type of the present invention is used, FIG. 6 is a vertical cross-sectional view of an embodiment of a rocket engine when applied to an actual rocket, and FIG. 7 9 to 9 show other embodiments of the present invention, and I-I in FIG.
FIG. 3 is a cross-sectional view of the rocket along a line. A... Burning progress surface, 1... Grain,
1a... Grain combustion initial surface, 2... Cap engine, 3... Combustion restriction material, 4...
...Perimeter restrictor, 5...Booster grain, 6...Nozzle.
Claims (1)
インはロケット中心軸方向に相互に平行に延びる複数個
の平板状燃焼制限材で区画されており、これらの燃焼制
限材はロケットの中心軸を通る縦断面仮想面に対し左右
対称に配置され、且つ横断面に於で一端はロケットチャ
ンバーの内周に固着し他端は内周から離隔して配設され
、グレインの燃焼の進行方向が燃焼制限材の上記他端に
於で屈折される様にしたことを特徴とするロケットエン
ジン。1 Grain is loaded into the rocket chamber, and the grain is partitioned by a plurality of flat combustion restricting materials that extend parallel to each other in the direction of the rocket's central axis, and these combustion restricting materials have a vertical cross section passing through the rocket's central axis. They are arranged symmetrically with respect to an imaginary plane, and in a cross section, one end is fixed to the inner periphery of the rocket chamber and the other end is arranged away from the inner periphery, so that the direction of combustion of the grains is aligned with the combustion restriction material. A rocket engine characterized by being bent at the other end.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2328575A JPS599744B2 (en) | 1975-02-25 | 1975-02-25 | rocket engine |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2328575A JPS599744B2 (en) | 1975-02-25 | 1975-02-25 | rocket engine |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5198418A JPS5198418A (en) | 1976-08-30 |
| JPS599744B2 true JPS599744B2 (en) | 1984-03-05 |
Family
ID=12106321
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2328575A Expired JPS599744B2 (en) | 1975-02-25 | 1975-02-25 | rocket engine |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS599744B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5752540Y2 (en) * | 1978-03-27 | 1982-11-15 | ||
| JP5187947B2 (en) * | 2008-03-13 | 2013-04-24 | 株式会社Ihiエアロスペース | End face combustion type gas generator |
-
1975
- 1975-02-25 JP JP2328575A patent/JPS599744B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5198418A (en) | 1976-08-30 |
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