The achievable values of specific impulse and structural
mass fraction , encountered in practice are such that it is very difficult for
a single rocket to provide the velocities required for orbiting the Earth and
for escaping from it. An increase in propellant mass, if provided to give
larger value of impulse , makes the rocket unwieldy and heavy and leads to
smaller values of the thrust to mass ratio.
If a series of rockets were put one on top of the other and
operated sequentially In stages one after the other , the total velocity would
correspond to the sum of the ideal velocities provided by the operation of each stage of the rocket.
The above fig. gives a schematic diagram of a two stage rocket with the first
stage rocket taking off from the ground and followed by the operation of 2nd
stage. The 2nd stage gets started when its velocity is equal to the
velocity provided by the 1ststageV1.i.e.
the velocity at the end of the operation of the 1st stage . If V2 is the velocity
contributed by the 2ndstage , the velocity at the end of operation
of the 2nd stage is V1 +
V2.
In general, for a
rocket having n stages , this stage continues with each successive stage
provided an incremental velocity . Denoting the ideal velocity provided by each
stage as V1,V2,…..Vn
respectively , the total ideal velocity of a n stage rocket is:
V=V1+V2+….+Vn
The used rocket stages are discarded once their propellant
is consumed in order to reduce the inert mass and hence improve the mass
fraction of the upper stages . This procedure of operating a series of rockets
sequentially is known as staging of
rockets .
Most of the
rockets used for putting space crafts into orbit have 2 to 4 rocket stages ,
and are referred to as satellite launch vehicles. The first stage rocket of a
satellite launch vehicle , which takes off from ground , is the heaviest and it
carries the upper rocket stages on it . It is known as the Booster stage . The
payload of the initial rocket stage comprises the upper stage rockets in addition to the actual payload . If the
mass ratio of the booster stage is Rm1
and the mass ratios of the upper stages are Rm2,Rm3,…..Rmnfor a rocket with n stages
in series, the net ideal velocity of the rocket is the sum of the individual
velocity increment of each stage .
V =Vj1ln(1/Rm1)+ Vj2ln(1/Rm2)
+ ….+ Vjnln(Rmn)
We get V=Vjln(Mi,1/Mf,n)
Where Vj=V1=V2……..=Vn
V=Vjln (1/Rm)n
=nVjln (1/Rm)
Multiple rocket stages are therefore , used to obtain higher
values of V. As the No.of stages goes up , the
operational complexity and cost of the multi-stage rocket increases. The No.of
stages cannot therefore , be arbitrarily
increased. The main aim has been to enhance the values of Vj and
decrease the structural mass fraction , keeping the No.of stage as small as possible
. The present trend is to work towards a Two stage to orbit (TSTO) launch
vehicle. A single stage to orbit(SSTO) vehicle would perhaps be possible if
very advanced materials of construction are devised to reduce th structural and
inert mass and have energetic
propellants which provide larger values of Vj than
obtainable at present.
The initial mass of a multi
stage rocket is quiet large considering that the mass of all the rocket stages
above booster stage have to be carried by it . The thrust of the booster rocket
should be sufficient for the vehicle to accelerate and take off from ground .
If the thrust of a single booster rocket is is insufficient a No.of rockets are
clustered together and operated simultaneously to generate the large values of
thrust required. Clustering is like parallel staging . Two booster rockets
could be strapped on either side of the core rocket to get sufficient
acceleration for take off. The strapped rockets are known as strap on rockets .
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