0% found this document useful (0 votes)
16 views15 pages

Slides 3

Uploaded by

Murali Krishna
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
0% found this document useful (0 votes)
16 views15 pages

Slides 3

Uploaded by

Murali Krishna
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
You are on page 1/ 15

Fundamentals: Relevant Terms

….. pushing   change of momentum

 Momentum (kgm/s)  mass (m) x velocity (v)

 Impulse (kgm/s or Ns)  change of momentum

 Force (N)  rate of change of momentum

 Specific Impulse (Ns/kg)  Impulse delivered per unit mass of propellant

Rocket Propulsion AE411 46


Rocket Principle and Rocket Equation

 Principle: Pushing itself forward by constantly ejecting out material stored


within it.

 Ziolkovsky Equation (Rocket Equation) [early 1900’s]

V = Vj ln (Mi/Mf)

where, V, velocity increment


Vj, efflux velocity
Mi, initial mass
Mf, final mass

Rocket Propulsion AE411 47


Mass Ratio Of a Rocket

Mass Ratio Rm = Mf/Mi


where, Mf = final mass after all the propellant has been consumed
and Mi = initial mass before the rocket operation

ie. V = Vj ln (1/ Rm)

We can show that, V = Vj ln [( +  + )/ ( + )]


where,  = payload mass fraction, Mu/Mi
 = structural mass fraction, Ms/Mi and
 = propellant mass fraction, Mp/Mi

Rocket Propulsion AE411 48


Desirable parameters of rocket

V = Vj ln [( +  + )/ ( + )]

or,  = e-(V / Vj) - 

i.e., to achieve higher values of payload mass fraction ,


(i) Vj needs to be large
(ii)  needs to be small

Rocket Propulsion AE411 49


Payload mass fraction,  Vs (V/Vj) and 

Rocket Propulsion AE411 50


Rockets having small propellant mass fraction

i.e., Mp < Mu , Ms

V ~ Vj [ (/ ( + )]
= Vj (Mp/Mf)
~ Vj (Mp/Mi)

Mp = pVp

where, p the density of the propellant,


Vp the volume of the propellant in the rocket

 V  pVj as Vp and Mf are fairly fixed

Rocket Propulsion AE411 51


Performance parameters of a rocket
 Impulse (I)
 change in momentum = mpVj [Ns]

 Specific Impulse (Isp)


 impulse delivered per unit mass of propellant = I/mp = Vj [m/s, Ns/kg, s]

 Density Impulse = Isp * propellant bulk density

 Thrust (F)
 rate of change of impulse = dI/dt = pVj [N]

 Impulse to mass ratio


 ratio of total impulse to the initial mass of rocket = I/Mi

 Thrust to mass ratio


 ratio of the thrust to the initial mass = F/Mi
Rocket Propulsion AE411 52
Propulsive Efficiency

Energy balance
diagram for a
chemical rocket

Propulsive efficiency determines how much of the k.e. of the exhaust jet is
useful for propelling a vehicle

Rocket Propulsion AE411 53


Propulsive Efficiency

Propulsive efficiency (p): ratio of the rate of work done by the rocket to the
rate of energy supplied

Rate of work done = Thrust power = Thrust (F) * Flight velocity (V)
Rate of energy supplied = Thrust power + residual kinetic jet power

i.e.

The propulsive efficiency is maximum when the forward vehicle velocity is


exactly equal to the exhaust velocity

Rocket Propulsion AE411 54


V/Vj

Rocket Propulsion AE411 55


Staging and Clustering of Rockets

liquid prop.
solid prop.

liquid prop.

solid prop (booster rocket).


strap-on rockets
(parallel staging)

Rocket Propulsion AE411 56


Multistaging
Mu Mu

Mu

1/2Mp 1/2Mp

Mp
For eg. for a rocket of 1000 tonnes 1/2Mp
Vj = 2700 m/s, Mu = 1 ton, Ms = 10 tonnes
V single stage = 5959 m/s
For a 2 stage rocket each with half the Mp
and Ms we get, 1/2Ms
V1 = 1590 m/s and
V2 = 5752 m/s
ie. V2-stage = 7342 m/s

Rocket Propulsion AE411 57


Staging and Clustering of Rockets (continued)

 the total velocity at the end of the operation is equal to the sum of the ideal
velocities provided by the operation of each stage
i.e., the total ideal velocity at the end of a n stage rocket
V = V1 + V2 + V3 + V4 …….+ Vn where, V1, V2…… Vn
are the velocity provided by each stage
or V = Vj1 ln (1/ Rm1) + Vj2 ln (1/ Rm2) +……….+ Vjn ln (1/ Rmn)
= Vj ln [(1/ Rm1) (1/ Rm2)… (1/ Rmn)] for equal Vj at the end
of each stages
= Vj ln [(Mi/Mf)1(Mi/Mf)2.... (Mi/Mf)n] in terms of intial and
final masses
= Vj ln [(Mi,1/Mf,n)] with intial mass of the
successive stage equal to
the final mass of previous
stage i.e., Mf,1 = Mi,2, Mf,2
= Mi,3...

Rocket Propulsion AE411 58


Staging and Clustering of Rockets (continued)

 In case of equal mass ratios at all stages,

i.e., V = Vj ln (1/ Rm)n for Rm1 = Rm2 =…Rmn = Rm


= n Vj ln (1/ Rm)

Rocket Propulsion AE411 59


Staging and Clustering of Rockets (continued)

Rocket Propulsion AE411 60

You might also like