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None of the following parameters are included
in the novice version.
With the exception of Atmospheric
Pressure, each of the variables has
shortcuts to commonly used values. For
example, Gamma of Gas in Rocket
can be typed in as any value but by pressing
a letter corresponding to the Gas required (a
for Air ... e
for CO2)
the value will be inserted into the
appropriate variable field.
The Gamma and Density
of Gas in Rocket are linked in that,
if you make the letter you press into an uppercase,
it will insert the values for both Gamma
and Density. So, by pressing
E, the Gamma
and Density for CO2
will be inserted into the appropriate fields.
The valid letters are displayed in the
help panel on the upper right of the model.
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Gamma of Gas
in Rocket This is a
measure of the compressibility of the
gas. The number itself (Gamma) is
derived from the ratio of the
specific heat capacities of the
compressed gas at constant pressure
and constant volume thus . . . Therefore, Gamma
can be measured in the laboratory
using simple equipment that gives
real-life numbers rather than
fiddle-factors. You can look up the
values of Gamma in any useful
physical constants book but just in
case you haven't got one to hand and
you are thinking about trying out
some other gasses in the rocket, here
are some Gammas of common gasses -
remember to be careful with gasses
and familiarise yourself with any
appropriate safety data sheets or
other information.
|
Gamma
of gas in rocket |
Gas |
Gamma |
air |
1.402 |
Ar |
1.667 |
He |
1.66 |
C2H4 |
1.26 |
CO2 |
1.304 |
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Density of
Gas in Rocket (kg/m3)
Each gas has a different density -
proportional to the molecular weight
of the gas or gas mixture in
question. The density has an
effect on the amount of push it can
give the rocket when it is expelled
at the end of the water thrust phase.
On the right are the densities of the
same set of gasses as above.
|
Density
of gas in rocket |
Gas |
Density
(kg/m3) |
air |
1.293 |
Ar |
1.784 |
He |
0.179 |
C2H4 |
1.260 |
CO2 |
1.977 |
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Density of
Liquid in Rocket (kg/m3)
You are not confined to using water
in the rocket although it would make
most sense to limit yourself to
water. The density of the liquid
in the rocket affects the push on the
rocket during this phase of thrust.
The densities of some common liquids
are listed on the right.
|
Density
of liquid in rocket |
Liquid |
Density
(kg/m3) |
Water |
998 |
Sea Water |
1025 |
Hg |
13546 |
Olive oil |
920 |
CCl4 |
1632 |
Br |
3100 |
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Acceleration
due to Gravity (m/s2)
Gravity (g) affects the rocket in
that it provides a fairly constant
force that tries to bring the rocket
back to earth (or whichever planetary
body you decided to launch it from). For
most purposes, g is 9.81m/s2
but if you want to be pedantic,
standard earth gravity is 9.80665m/s2
and, for those who want to be even
more pedantic there is a formula that
works for heights above sea-level
that are reasonable on the Earth's
surface (acceleration due to gravity
is inversely proportional to the
square of the distance from the
centre but with Mt. Everest being
only about 5 miles tall and roughly
4,000 miles from the Earth's centre,
it is proportional for the purposes
of this equation) . . .
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g
/ms-2 |
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= |
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9.80616 -
0.025928cos2L +
0.000069cos²2L -
0.000003h |
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where: |
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h |
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= |
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height above
sea-level in metres; |
and, |
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L |
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= |
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latitude. |
If you wish to
experiment with launches off
different planets/moons and so on,
here are the figures for this solar
system . . .
|
Some
places to launch |
Body |
Acceleration
(m/s2) |
Sun |
274 |
Moon |
1.62 |
Mercury |
3.76 |
Venus |
8.77 |
Earth |
9.81 |
Mars |
3.80 |
Jupiter |
24.9 |
Saturn |
10.4 |
Uranus |
10.4 |
Neptune |
13.8 |
Pluto |
4 |
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Atmospheric
Pressure (mBar) This
affects the pressure along the nozzle
and the amount of drag on the rocket
(see Density of Air below). Standard
air pressure is 101325 Nm-2 or
1013.25 mBar. I have used mBar as the
air pressure unit in the model
because it is a value that is
available to us all in weather
reports
The air pressure is less at
greater altitudes and the air
pressures that you see on weather
maps are all converted to atmospheric
pressure at sea level. If your launch
site is on raised ground, you can
take this into account with the
following table which uses standard
atmospheric pressure at sea level.
Taking into account the fact that
there are plenty of out of control
factors in any launch, a rough
estimate can be made by taking the
pressure from the weather report and
multiplying it by the factor for your
altitude in the table on the right to
give you the pressure at the launch.
eg, weather report says 998 mBar,
you are at 240 metres and the factor
for 250 metres is 0.9707 therefore .
. .
998 x 0.9707 = 969
mBar
(or,
in practical terms, 970 mBar)
Note that a millibar is 1/1,000th
of a Bar and 1 Bar is 100,000 Nm-2
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Pressure
against Height |
Geometric
Height
/m |
Pressure
/mBar |
Factor |
0 |
1013.25 |
1.0 |
250 |
983.58 |
0.9707 |
500 |
954.61 |
0.9421 |
750 |
926.35 |
0.9142 |
1,000 |
898.76 |
0.9768 |
1,500 |
845.60 |
0.8345 |
2,000 |
798.01 |
0.7876 |
2,500 |
749.92 |
0.7401 |
3,000 |
701.21 |
0.6920 |
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Density of
Air at STP (kg/m3)
This is the density of the gas on the
outside of the rocket at Standard
Temperature and Pressure. This
figure affects the amount of drag
experienced by the rocket - the
higher the density, the more force is
required to move the air out of the
way during flight.
If you are launching in a low
pressure atmosphere such as on the
Moon, use the density of the gas (the
solar wind - mainly hydrogen) at STP
(see the table on the right) and put
the lower Atmospheric Pressure in, in
the previous data field. The model
will give the rocket the correct drag
for the reduced pressure.
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Some
common atmospheres |
Atmosphere |
Density
(kg/m3) |
air |
1.293 |
NH3 |
0.771 |
He |
0.179 |
H2 |
0.090 |
CH4 |
0.717 |
SO2 |
2.927 |
CO2 |
1.977 |
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Copyright
©2000 Paul Grosse. All Rights Reserved.
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