If you need assistance, please send an email to forum at 4hv dot org. To ensure your email is not marked as spam, please include the phrase "4hv help" in the subject line. You can also find assistance via IRC, at irc.shadowworld.net, room #hvcomm.
Support 4hv.org!
Donate:
4hv.org is hosted on a dedicated server. Unfortunately, this server costs and we rely on the help of site members to keep 4hv.org running. Please consider donating. We will place your name on the thanks list and you'll be helping to keep 4hv.org alive and free for everyone. Members whose names appear in red bold have donated recently. Green bold denotes those who have recently donated to keep the server carbon neutral.
Special Thanks To:
Aaron Holmes
Aaron Wheeler
Adam Horden
Alan Scrimgeour
Andre
Andrew Haynes
Anonymous000
asabase
Austin Weil
barney
Barry
Bert Hickman
Bill Kukowski
Blitzorn
Brandon Paradelas
Bruce Bowling
BubeeMike
Byong Park
Cesiumsponge
Chris F.
Chris Hooper
Corey Worthington
Derek Woodroffe
Dalus
Dan Strother
Daniel Davis
Daniel Uhrenholt
datasheetarchive
Dave Billington
Dave Marshall
David F.
Dennis Rogers
drelectrix
Dr. John Gudenas
Dr. Spark
E.TexasTesla
eastvoltresearch
Eirik Taylor
Erik Dyakov
Erlend^SE
Finn Hammer
Firebug24k
GalliumMan
Gary Peterson
George Slade
GhostNull
Gordon Mcknight
Graham Armitage
Grant
GreySoul
Henry H
IamSmooth
In memory of Leo Powning
Jacob Cash
James Howells
James Pawson
Jeff Greenfield
Jeff Thomas
Jesse Frost
Jim Mitchell
jlr134
Joe Mastroianni
John Forcina
John Oberg
John Willcutt
Jon Newcomb
klugesmith
Leslie Wright
Lutz Hoffman
Mads Barnkob
Martin King
Mats Karlsson
Matt Gibson
Matthew Guidry
mbd
Michael D'Angelo
Mikkel
mileswaldron
mister_rf
Neil Foster
Nick de Smith
Nick Soroka
nicklenorp
Nik
Norman Stanley
Patrick Coleman
Paul Brodie
Paul Jordan
Paul Montgomery
Ped
Peter Krogen
Peter Terren
PhilGood
Richard Feldman
Robert Bush
Royce Bailey
Scott Fusare
Scott Newman
smiffy
Stella
Steven Busic
Steve Conner
Steve Jones
Steve Ward
Sulaiman
Thomas Coyle
Thomas A. Wallace
Thomas W
Timo
Torch
Ulf Jonsson
vasil
Vaxian
vladi mazzilli
wastehl
Weston
William Kim
William N.
William Stehl
Wesley Venis
The aforementioned have contributed financially to the continuing triumph of 4hv.org. They are deserving of my most heartfelt thanks.
Registered Member #2431
Joined: Tue Oct 13 2009, 09:47PM
Location: Chico, CA. USA
Posts: 5639
Dr. Slack wrote ...
Now for Mk2, if you mounted the motor on a bearing, and resisted the rotation with some means of measuring torque... ....you could measure true torque/power at the prop, and you'd have a motor dynamometer as well.
hell. i should have thought of that.
there is a super dooper important PDF, but i cant get it to save in the attachments section.
hers the link: the velocity and pressure diamgrams are important. i may throw flour into the propeller to visualize the exhaust stream.
Registered Member #3414
Joined: Sun Nov 14 2010, 05:05PM
Location: UK
Posts: 4245
Not only do I have helicopters flying past my windows most days (I live on a hill in a military training area), but recemtly they've been flying around my head. I think if you have a 'Chinook' configuration, but with two pairs of concentric props (four props altogether), you can do it just with VPP, without swashplates 'IF' you drive each prop from a separate motor.....still thinking....and drinking....
EDIT: It's possible to do without VPP as well, if you use electric motors.....four motors, four props, but two concentric pairs, in Chinook configuration.
The first equation is Newtons law of motion. The second one is wrong. The third describes the thrust of e.g. propeller, which accelerates air at the rate dm/dt from velocity vh to ve. Think of the situation of pushing a mass m with the force F for a time t. Then the mass will have accelerated to the velocity v. The involved quantities are related by the equation
F*t = m*v
This equation describes the conservation of momentum. Divide both sides by t and you get:
F = (m/t) * v
This is basically your third equation for the special case, that the entrant air velocity vh is zero.
Registered Member #2529
Joined: Thu Dec 10 2009, 02:43AM
Location:
Posts: 600
The m and the v are related, at high v_e, you are drawing more air through your rotor per second.
i.e.
m ~= rho v_e A
where rho is the air density and A is the disk area
but the reality is more complicated; some of the air is vortexing around in a circuit and not being accelerated as much, so giving less force; you could probably have some sort of fudge factor for that. However, due to viscosity you'll still get advantage from even that.
But the rho v_e A is probably a good start.
Basically:
F = m dv/dt
let's say that every second you're accelerating a mass m of air, from rest above the vehicle to V_e, as a jet of air below the vehicle:
F = m V_e
substitute for 'm'
F = (rho V_e A) V_e
rearrange:
F = rho A V_e^2
(n.b. you have to be a bit careful with those dm/dt terms, mass is conserved, so dm/dt is always technically 0!)
Registered Member #3414
Joined: Sun Nov 14 2010, 05:05PM
Location: UK
Posts: 4245
BigBad wrote ...
but the reality is more complicated; some of the air is vortexing around in a circuit and not being accelerated as much, so giving less force; you could probably have some sort of fudge factor for that. However, due to viscosity you'll still get advantage from even that.
If BigBad is reffering to the peripheral vortex losses, these are much greater for a smaller, faster turning prop than they are for a larger, slower turning prop, assuming both are consuming the same power, for two reasons, firstly, the losses will be greater from the faster moving air, and secondly, the cross sectional area/circumferance ratio means that, for a larger, slower turning prop, a smaller percentage of the moving column is at the periphery, and experiencing losses.
You want to aim to accelerate the largest volume of air possible to a low velocity, as this is far more efficient than accelerating a small volume of air to a high velocity, due to these peripheral losses.
EDIT:The 'trade-off' is manouverability. Dr Spark's drone with 5" blades spinning at 25,000RPM demonstrates this exactly, very manouverable, but short flight times.
This site is powered by e107, which is released under the GNU GPL License. All work on this site, except where otherwise noted, is licensed under a Creative Commons Attribution-ShareAlike 2.5 License. By submitting any information to this site, you agree that anything submitted will be so licensed. Please read our Disclaimer and Policies page for information on your rights and responsibilities regarding this site.