23.12.2012 Views

FIRST STEPS TOWARD SPACE - Smithsonian Institution Libraries

FIRST STEPS TOWARD SPACE - Smithsonian Institution Libraries

FIRST STEPS TOWARD SPACE - Smithsonian Institution Libraries

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

0 it 20 SO 40 90 60 10 BO 90 lot 110 Of 130 140 15V<br />

FIGURE 1.—Correlation of time and acceleration.<br />

tween propulsion force and initial weight of the<br />

rocket.<br />

The time T corresponding to the end of combustion<br />

is given by<br />

,= v (l MA<br />

The rocket velocity Vt at the end of combustion<br />

is given by<br />

„ r M0 i/. MtY<br />

Vt—v \n— — ( 1 — -r-jT-]<br />

f Mt n\ M0/_<br />

The altitude h reached at the end of combustion<br />

is given by<br />

ht= "go<br />

[MJ. Mt , \ . 1 1 /, Mt\<br />

(5)<br />

(6)<br />

(V)<br />

SMITHSONIAN ANNALS OF FLIGHT<br />

The initial velocity V necessary to climb by force<br />

of inertia from height h to height H, the latter<br />

reached with zero velocity speed is given by<br />

V* = 2g0r (_} LA<br />

\h + r H+r H+r)'<br />

where r is the radius of the earth considered as<br />

spherical.<br />

From the above formula we can obtain the value<br />

of ratio M0 necessary for reaching a previously<br />

established altitude H with zero resulting velocity.<br />

The rocket reaches this altitude by coasting from<br />

altitude h where, at the end of the combustion, it<br />

had velocity V. For this calculation a graph has<br />

been prepared, shown in Figure 2, for a prompt<br />

solution of the problems regarding the rocket's<br />

vertical ascension without taking into account the<br />

resistance of the air.<br />

Regarding the resistance of the air, not considered<br />

until now, and expressed by the above formula (8),<br />

this can be expressed in function of ratio M0jm<br />

where m is the value of the mass at any given time.<br />

In Figure 3 are shown a diagram of function<br />

F(V)'d of the resistance of the air; a diagram of the<br />

relative retarding acceleration WA; and a diagram,<br />

with a linear variation, of the rocket's acceleration<br />

in the absence of air.<br />

NOTES<br />

1. Aldo Bartocci, "Le Escursioni in altezza col motore a<br />

reazione," L'Aerotecnica, vol. 13, no. 12 (December 1933),<br />

pp. 1646-66; and "II Razzo," L'Aerotecnica, vol. 14, no. 3<br />

(March 1934), pp. 255-66.<br />

2. In a letter to the author, dated 5 July 1949, General<br />

G. A. Crocco said:<br />

I have indeed been pleased that Professor Eula has informed<br />

me that you are the author of the interesting articles published<br />

in 1933, 34, and 38; and I was very glad to have this<br />

confirmation authenticated in writing. .<br />

I am glad then to tell you that the rate of retardation (drag)<br />

introduced by the air in the vertical movement of the rocket,<br />

and which today is published by an English Review, the subject<br />

of which is the rocket "Neptune" of the U.S. Navy,<br />

coincides exactly with that which you designated certainly<br />

for the first time, in 1934.<br />

The article to which he refers may have been that by C. H.<br />

Smith, M. W. Rosen, and J. M. Bridger, "Super Altitude<br />

Research Rocket Revealed by Navy," Aviation, June 1947,<br />

pp. 40-43.—Ed.<br />

(8)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!