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 #1523
Joined: Sat Jun 07 2008, 02:05PM
Location:
Posts: 97
One day, I was thinking about rail guns.
And I had a quesion, How big does a permanent magnet, and current in a railgun have to be, to have equal force to a rail gun without a permanent magnet?
so, I did some equation derivations. Please bear with me.
I started with
f=qvXb
Where f is the force. q is the charge. v is the velocity (of the charges). X is cross product. And b is the magnetic field.
Can be rewritten to
F=ilXb
Where i is the current. And l is the distance between the rails.
So, in a railgun that is not augmented.
F=ilb.
(assuming a railgun where everything is at 90 degrees)
Where b=ui/2(pi)r
Where u is the permeability of free space. And r is the distance.
In a rail gun, the distance would be in the middle of the two rails. And the equation should be doubled.
So, once simplified
B=2ui/(pi)l
So, for a non-augmented railgun
F=2ui2/(pi)
Now, for a railgun augmented by a permanent magnet.
F=ilb (of course)
Where i (for the sake of my purpose) will be replaced with w. Since, although it is a current, it shouldn’t be confused with the current in the original equation, which is larger.
Also, b, instead of being dependent of current. It is dependent on the permanent magnet.
So, for a augmented railgun. F=wlb.
Now, I will set them equal, to figure out how big the magnetic field and current has to be in an augmented railgun, to equal the force of a non-augmented railgun.
So
Wlb=2ui2/(pi)
So
Wb=2ui2/(pi)l
Yea. So we have a nice equation. But what does it mean?!?!?
Lets plug in some numbers and see what happens.
The common Neodymium magnet is around 1 T.
So, b=1.
U=4(pi)x(10^-7)
And, the common Photo Flash capacitor can put out .4 amps.
It isn’t uncommon to have around ten of these in a small rail gun
So, i=4
Lastly, a good width for a small rail gun is 5 mm. Which is 5x(10^-3)
So, assuming these numbers are good. How big of a current does my augmented rail gun need to be on par with a rail gun powered by 10 photo flash capacitors?
W=4x(10^-7)x42/5x(10^-3)
W=1.28x(10^-3)
So, a small rail gun augmented by one small neodymium magnet. Only requires a current of 1.28 mA to compete with a rail gun powered by ten photo flash capacitors.
So, my question is, why do we bother with high amperages at all? Why don’t we just use some big magnets?
Which I would very much like to know.
Howver, for those who wouldn't mind following some more math. I had anouther quesion. (My curiosity is Unsatiable)
My previous calculation strikes me a a contradiction to the law of conservation of matter an energy.
What if I took that logic a little further, and calculate how big of a magnetic field would be needed to break the law?
So, bear with me as I do some more calculations.
To be a contradiction of the law of conservation of matter and energy, the energy in the projectile must be greater than the energy put into it by the electricity.
Let me start by finding the energy of the projectile.
Assuming no friction. All the energy in the projectile, due to the railgun, is kinetic.
So, we can use, e=.5 m(v^2)
Where e is energy, m is mass. And v is velocity.
And
V=at
Where a is acceleration, and t is time.
So we need to find the acceleration and the time.
Well,
F=ma
And f=ilb
So a=ilb/m
Time is a little harder
If we start with x=a(t^2)
Where x is the distance that the acceleration is applied. (length of the railgun).
To solve for t
T=(x/a)^(1/2)
And we know that
A=ilb/m
So, T=(xm/ilb)^(1/2)
So, to plug this all in
E=.5 m ((ilb/m)^2) (xm/ilb)
To simplify further
E=.5 xilb
That simplified nicely.
Now, for the energy that is put into the rail gun via the current.
Well,
E=pt
Where p is power
And p=(i^2)r
Where r is resistance. (I could use p=iv, but it seems to me that p=(i^2)r better describes what is going on)
So
E=i2rt
And t=(xm/ilb)^(1/2)
So
E=(i^2)r(xm/ilb)(^1/2)
So for the fun part. To decide if these equations break the laws of physics.
First, I will set the energy in the bullet to be greater than the energy in the electricity. Which inherently implies a breakage in the law of conservation of energy
So
.5xilb>(i^2)r(xm/ilb)^(1/2)
now I will solve for b. to see how big of a magnetic field is needed, before the laws of physics no longer apply
Which comes out to be
b>(4m/xl2i)^(1/3)
hmm…so, if I have a permanent magnet, augmenting a railgun, that is bigger than that strange number, I will break the law of conservation of energy.
Lets plug in some numbers.
Say,
M=5 grams. Which is .05 kg.
X= 1 meter
L= 5x(10^-3) meters
And I= 4 amps
once pluged in, you come up with
b>12.6 Tesla.
Which, although is bigger magnetic field then I want to make with my college budget. It is only around 12 small neodymium magnets. Not unreasonable.
So, I guess I am wondering. I trust the laws of conservation of matter and energy more than I do my own math and understanding.
Where did I screw up? And what don’t I understand?
Registered Member #1062
Joined: Tue Oct 16 2007, 02:01AM
Location:
Posts: 1529
I did not follow the math very well, but.... Math can model equations that theoretically can break laws. There is a point where the math continues to model past practical limits, you need to find the limits.
As for your first question, relating to the above, I think there are also limits to that. You need a starting current that can overcome friction, and to maintain the force. Magnets are considered to have neutral energy, so it does not add power. The magnets mearly improve the affect of the current. Also, with larger railgun's, magnet augmentation becomes pointless, as they will operate above the magnet strength. This is where people use electromagnets rather than permanent magnets, in configurations called parallel augmented or series augmented. This essentially increases the number of turns in a railgun.
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.