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首页> 外文期刊>Acta astronautica >Velocity corrections in generalized coplanar coaxial Hohmann and bi-elliptic impulsive transfer orbits
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Velocity corrections in generalized coplanar coaxial Hohmann and bi-elliptic impulsive transfer orbits

机译:广义共面同轴Hohmann和双椭圆脉冲传输轨道的速度校正

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摘要

We shall investigate the problem of the differential corrections of the orbital elements a, e of the final elliptic orbit, in order that we might obtain the required very precise one. This will be achieved by the application of differential motor thrust impulses △v_A, △v_B at peri-apse A and apo-apse B, to induce correctional △a, △e increments. We apply differential thrusts at peri-apse and apo-apse of the generalized Hohmann and bi-elliptic transfer impulsive systems of orbits. Our purpose is to find the differential corrections in major axes and eccentricities of the two considered transfer systems. Thus we can obtain a very precise final elliptic orbit, throughout differential velocity increments perpendicular to the coaxial major axes and tangential to peri-apse and apo-apse of the elliptical terminal orbits. We find out the four relationships between △a_1, △a_T, △e_1, △e_T and △v_A, △v_B the velocity increments at the points A and B , for the four cases of the Hohmann type trajectories . We notice that △a_1 and △e_1 are related to △v_A whilst △a_T and △e_T are combined with , △v_B. This occurs for the four Hohmann configurations. Referring to the bi-elliptic type of impulsive transfer we have: △v_A = f(△a_1); △v_C = f(△v_A) = ψ(△a_1); △v_B = f(△v_A) = ψ(△a_1), △a_T = f(a_1, a_2, e_1, e_2) for all four feasible cases. △a_(T') = f(△v_a) = ψ(△a_1) for all four bi-elliptic cases. In addition for all feasible bi-elliptic cases we have Ae = /(Ava).
机译:我们将研究最终椭圆轨道的轨道元素a,e的微分校正问题,以便获得所需的非常精确的轨道。这将通过在近端A和近端近端B处施加差分电动机推力脉冲△v_A,△v_B来实现,以产生校正的△a,△e增量。我们在广义的Hohmann和双椭圆转移脉冲轨道系统的近点和近点上施加不同的推力。我们的目的是找到两个考虑的传递系统的主轴和偏心距的微分校正。因此,我们可以得到一个非常精确的最终椭圆轨道,其垂直于同轴主轴线且与椭圆终轨道的近周点和近端点切线成正比的速度差增量。对于Hohmann型轨迹的四种情况,我们找出了△a_1,△a_T,△e_1,△e_T和△v_A,△v_B之间的四个关系。我们注意到,△a_1和△e_1与△v_A有关,而△a_T和△e_T与△v_B​​相结合。对于四种霍曼配置,都会发生这种情况。关于脉冲转移的双椭圆类型,我们有:△v_A = f(△a_1); △v_C = f(△v_A)=ψ(△a_1);对于所有四个可行情况,△v_B = f(△v_A)=ψ(△a_1),△a_T = f(a_1,a_2,e_1,e_2)。对于所有四个双椭圆形情况,△a_(T')= f(△v_a)=ψ(△a_1)。另外,对于所有可行的双椭圆形情况,我们都有Ae = /(Ava)。

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