| Home | Research | For Teachers | HISTORY Level 1 Level 2 Level 3 |
PRINCIPLES Level 1 Level 2 Level 3 |
CAREER Level 1 Level 2 Level 3 |
| Search | Hot Links | What's New! | |||
| Gallery | Feedback | Admin/Tools | |||
Please let me remind all of you--this
material is copyrighted. Though partially funded by NASA, it is still a private
site. Therefore, before using our materials in any form, electronic or otherwise, you need
to ask permission.
There are two ways to browse the site: (1) use the search
button above to find specific materials using keywords; or,
(2) go to specific headings like history,
principles or careers at specific levels above and click on the
button.
Teachers may go directly to the Teachers' Guide from the For
Teachers button above or site browse as in (1) and (2).
![]()
In this section, we deal with one of the forces acting on an aircraft, namely, the thrust produced by the aircraft's engine. In the first part of this section we will look at propellers and their efficiency. In the second part of this section, we will provide the formula for the thrust of a jet engine.
Propellers are used to drive many lightweight aircraft and
were the principal means of propulsion for military aircraft
until the advent of the jet engine. As such, it is
important to know how propellers work and how efficient they
are. The propeller efficiency can never reach the ideal
efficiency of 100 %. This is because in the development of the
propeller efficiency several concepts are ignored,
1. The friction drag of the blades.
2. The kinetic energy of the rotation of the slipstream.
3. The fact that the thrust is not uniformly distributed over the
blades.
The maximun propeller efficiency is about 90 %. This is due to
the combined effects of drag from the nacelle and wings upon the
propeller. This combined effect drops propeller efficiency to
about 87 %. From there the thrust horsepower provided by the
propeller is
![]()
where:
= thrust
(lb)
= velocity
(ft/s)
= engine
brake horsepower
550 = conversion factor from ft-lbs to horsepower
=
propeller efficiency
The thrust equation for a turbojet can be derived from the
general form of Newton's second law (i.e., force equals the time
rate of change of momentum),
![]()
The figure below shows the inlet and exhaust flows of the
turbojet. The negative thrust due to bringing the freestream air
almost to rest just ahead of the engine is called momentum drag
or ram drag. The resulting thrust is given by following equation,

Schematic of a turbojet engine.
where:
= is weight flow rate of the air passing through the engine.
= jet
stream velocity
= static
pressure across propelling nozzle
=
atmospheric pressure
=
propelling nozzle area
= aircraft
speed
The information in this section has been extracted from several sources. Those sources have been contacted and permission to use their material on our site is pending. However, the format in which this material has been presented is copyrighted by the ALLSTAR network.
Send all comments to
allstar@fiu.edu
© 1995-2012 ALLSTAR Network. All rights reserved worldwide.
Updated: March 12, 2004