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velocity factor???
given that the length of a half wave dipole is calculated by 468 / freq in mhz when velocity factor is 1, ie 468 / 1.9 is about 246 ft. i'm sitting here wondering why folks with small city lots don't use (468 / freq in mhz) * velocity factor, to construct a much shorter antnenna, particularly on 80m & 160m? as an example, rg59 coax typically has a velocity factor of .66, so plugging to the formula, 468 / 1.9 is about 246 ft, * .66 is about 162 ft. why couldn't 162 ft of rg59 be cut in two, attached to a 50 ohm, have the remaining ends of the rg59 shorted together, and hoisted into the air? so what am i missing? there are no free lunches:-) larry kd5foy |
velocity factor???
larry d clark wrote:
why couldn't 162 ft of rg59 be cut in two, attached to a 50 ohm, have the remaining ends of the rg59 shorted together, and hoisted into the air? The velocity factor of the inside of RG-59 is 0.66 when the currents are differential. The inside of RG-59 doesn't radiate when the currents are differential. The outside of RG-59 is used for radiation. The velocity factor of the outside of RG-59 is about 0.95, about the same as ordinary insulated wire. -- 73, Cecil http://www.w5dxp.com |
velocity factor???
larry d clark wrote:
given that the length of a half wave dipole is calculated by 468 / freq in mhz when velocity factor is 1, ie 468 / 1.9 is about 246 ft. i'm sitting here wondering why folks with small city lots don't use (468 / freq in mhz) * velocity factor, to construct a much shorter antnenna, particularly on 80m & 160m? as an example, rg59 coax typically has a velocity factor of .66, so plugging to the formula, 468 / 1.9 is about 246 ft, * .66 is about 162 ft. why couldn't 162 ft of rg59 be cut in two, attached to a 50 ohm, have the remaining ends of the rg59 shorted together, and hoisted into the air? so what am i missing? there are no free lunches:-) larry kd5foy One wavelength in free space in feet is 984/F in feet (300/F in meters); a half-wavelength is 492/F. 468/F assumes a vf of 0.95 of the antenna radiating surface. The vf of coaxial cable is dependent upon the dielectric used. 0.66 is common for solid polyethylene. Foamed PE is typically near 0.80. As with many RG cables, RG59 is available both ways. In your example, the vf of the dielectric would not matter, since the majority of the current flows on the *outside* of the shield due to skin-effect. Thus, the formula for the length would be very close to (only slightly shorter than) 468/F. Since I^2*R losses would be lower, bandwidth would be better than a smaller-diameter wire. Bryan WA7PRC |
velocity factor???
On Feb 11, 5:58 pm, larry d clark wrote:
given that the length of a half wave dipole is calculated by 468 / freq in mhz when velocity factor is 1, ie 468 / 1.9 is about 246 ft. i'm sitting here wondering why folks with small city lots don't use (468 / freq in mhz) * velocity factor, to construct a much shorter antnenna, particularly on 80m & 160m? as an example, rg59 coax typically has a velocity factor of .66, so plugging to the formula, 468 / 1.9 is about 246 ft, * .66 is about 162 ft. why couldn't 162 ft of rg59 be cut in two, attached to a 50 ohm, have the remaining ends of the rg59 shorted together, and hoisted into the air? so what am i missing? there are no free lunches:-) larry kd5foy To achieve resonance in a shorter antenna, you can increase either the capacitance or the inductance--or both, of course. To increase the capacitance, all you have to do is fill the universe with polyethylene, or some similar low-loss dielectric. You don't have to actually fill the whole universe with it; it would work to fill a volume around the antenna. But to get the full effect, it should be a pretty large volume, containing the electric field in the neighborhood of the antenna. Not very practical. In coax, the electric field is between the wires; in the dipole, it's also between the wires, but the volume is very much larger. On the other hand, people have been shortening resonant antennas for a long time by increasing the inductance: thus, loading coils and "slinky" antennas. Similarly, people make "slow" coax by making the center conductor a helix, and thus make delay lines. Cheers, Tom |
delay line? velocity factor???
I.....verse with it; it would work to fill a
volume around the antenna. But to get the full effect, it should be a pretty large volume, containing the electric field in the neighborhood of the antenna. Not very practical. In coax, the electric field is between the wires; in the dipole, it's also between the wires, but the volume is very much larger. On the other hand, people have been shortening resonant antennas for a long time by increasing the inductance: thus, loading coils and "slinky" antennas. Similarly, people make "slow" coax by making the center conductor a helix, and thus make delay lines. Cheers, Tom ok what is a 'delay line'?? i would think that would just increase the surface area and therfore sorta increase performance |
delay line? velocity factor???
On Feb 14, 3:21 pm, ml wrote:
I.....verse with it; it would work to fill a volume around the antenna. But to get the full effect, it should be a pretty large volume, containing the electric field in the neighborhood of the antenna. Not very practical. In coax, the electric field is between the wires; in the dipole, it's also between the wires, but the volume is very much larger. On the other hand, people have been shortening resonant antennas for a long time by increasing the inductance: thus, loading coils and "slinky" antennas. Similarly, people make "slow" coax by making the center conductor a helix, and thus make delay lines. Cheers, Tom ok what is a 'delay line'?? i would think that would just increase the surface area and therfore sorta increase performance Wikipedia gives a definition of delay line; a length of transmission line is technically a delay line, but often for longer delays, a special line is made in which the center conductor is a wire wound around a core (often of the same material as the dielectric between center and outer). The winding should be done with space between the turns, not close-wound, to give more uniform delay versus frequency. For a uniform TEM transmission line, the delay time is the square root of the total capacitance between the conductors times the total net inductance of the length of the conductors: Tau=sqrt(L*C). Many E&M texts go into how to accurately calculate the inductance and capacitance for coaxial line with straight conductors. In an antenna, you can increase the inductance by adding a lumped inductance, commonly called a loading coil, or you can replace the straight wire with a wire formed into a helix. Google "slinky antenna". You'll find lots of info. I'm not making any claims that a slinky antenna is either a good antenna or a poor one; it's just one way to make a shortened dipole or monopole antenna, or even a shortened Yagi. Cheers, Tom |
delay line? velocity factor???
K7ITM wrote:
On Feb 14, 3:21 pm, ml wrote: I.....verse with it; it would work to fill a volume around the antenna. But to get the full effect, it should be a pretty large volume, containing the electric field in the neighborhood of the antenna. Not very practical. In coax, the electric field is between the wires; in the dipole, it's also between the wires, but the volume is very much larger. On the other hand, people have been shortening resonant antennas for a long time by increasing the inductance: thus, loading coils and "slinky" antennas. Similarly, people make "slow" coax by making the center conductor a helix, and thus make delay lines. Cheers, Tom ok what is a 'delay line'?? i would think that would just increase the surface area and therfore sorta increase performance Wikipedia gives a definition of delay line; a length of transmission line is technically a delay line, but often for longer delays, a special line is made in which the center conductor is a wire wound around a core (often of the same material as the dielectric between center and outer). The winding should be done with space between the turns, not close-wound, to give more uniform delay versus frequency. For a uniform TEM transmission line, the delay time is the square root of the total capacitance between the conductors times the total net inductance of the length of the conductors: Tau=sqrt(L*C). Many E&M texts go into how to accurately calculate the inductance and capacitance for coaxial line with straight conductors. In an antenna, you can increase the inductance by adding a lumped inductance, commonly called a loading coil, or you can replace the straight wire with a wire formed into a helix. Google "slinky antenna". You'll find lots of info. I'm not making any claims that a slinky antenna is either a good antenna or a poor one; it's just one way to make a shortened dipole or monopole antenna, or even a shortened Yagi. Cheers, Tom In the early days of computers they used to use a length of wire as temporary memory. At the start of a store cycle a piece of data would be input to the wire, after a period of time the data would come out and be placed into the computation. Admiral Grace Hopper used to give an example of time and delay in her speeches. She would say that one day she called down to the computer department and asked for a micro second. They sent her 1000 feet of wire. She then called down and asked for a nanosecond, they sent her one foot of wire. No point to this just a good story. Dave N |
delay line? velocity factor???
"David G. Nagel" wrote in message ... In the early days of computers they used to use a length of wire as temporary memory. At the start of a store cycle a piece of data would be input to the wire, after a period of time the data would come out and be placed into the computation. Admiral Grace Hopper used to give an example of time and delay in her speeches. She would say that one day she called down to the computer department and asked for a micro second. They sent her 1000 feet of wire. She then called down and asked for a nanosecond, they sent her one foot of wire. No point to this just a good story. Early color TV sets used a coaxial cable delay line for the luminance (B&W signal) component, since the chromanance (color signal) is delayed in the circuits that process it but they both need to arrive at the picture tube simultaneously. Newer sets use various means besides a length of coax. |
delay line? velocity factor???
Adm. Hooper would bring her wires with her
when she was a guest on the Tonight show with Johnny Carson. Adm Grace Murray Hooper, a pioneer in practical computing, and the first woman admiral in the U.S. Navy. In the early days of computers they used to use a length of wire as temporary memory. At the start of a store cycle a piece of data would be input to the wire, after a period of time the data would come out and be placed into the computation. Admiral Grace Hopper used to give an example of time and delay in her speeches. She would say that one day she called down to the computer department and asked for a micro second. They sent her 1000 feet of wire. She then called down and asked for a nanosecond, they sent her one foot of wire. No point to this just a good story. Dave N |
delay line? velocity factor???
In the early days of computers they used to use a length of wire as temporary memory. At the start of a store cycle a piece of data would be input to the wire, after a period of time the data would come out and be placed into the computation. Admiral Grace Hopper used to give an example of time and delay in her speeches. She would say that one day she called down to the computer department and asked for a micro second. They sent her 1000 feet of wire. She then called down and asked for a nanosecond, they sent her one foot of wire. No point to this just a good story. Dave N The delay lines I encountered at IBM that were used for storage were "sonic" delay lines. They were driven in a torsion mode (mechanical) and were very reliable up to about 10 milliseconds(I think!) of data. Above that they began to be temperamental and required constant temperature ovens. The larger ones were used as video storage with a screen of data in each instance. Delay lines running at light speed (about a NS per ft) were used as clock generators by inputting a pulse and tapping the line down stream for a very stable clock sequence. John Ferrell W8CCW |
delay line? velocity factor???
A feature of the '50s-era radars I worked on in the '60s was MTI, or
moving target indication. It was done simply by subtracting the return from the previous pulse from the current one and displaying only things which had changed. This was done to reduce clutter from fixed objects, and it was effective against some jamming techniques. Doing something like that is trivial today, but it wasn't back then. The pulse repetition time of the long-range radars was over 2 ms (round trip time for 400 miles or so), so a delay of that time with a bandwidth of a few MHz was required. The sets I worked on used a large piezoelectric quartz slab with many faces, and transducers on two of the faces. One transducer would convert the electrical signal to a mechanical wave which would enter the slab, bounce around from one face to another, until at the right time it would hit a face below the critical angle and exit. And that face was, of course, where the other transducer was. To keep the timing precise, the slab was used to control the radar pulse interval. Not long before I was involved, a mercury delay line was used. This was a tube of mercury with a transducer at each end, and a mechanical wave was sent from one end to the other. I never saw one, but heard many stories about how fussy they were and that it would take hours or days for waves to settle if it was bumped or jiggled. Folks who had dealt with them considered the quartz delay line to be a big improvement. Roy Lewallen, W7EL |
delay line? velocity factor???
Roy Lewallen wrote in news:12tkkh6n7us4v19
@corp.supernews.com: A feature of the '50s-era radars I worked on in the '60s was MTI, or moving target indication. It was done simply by subtracting the return from the previous pulse from the current one and displaying only things which had changed. This was done to reduce clutter from fixed objects, and it was effective against some jamming techniques. Doing something like that is trivial today, but it wasn't back then. The pulse repetition time of the long-range radars was over 2 ms (round trip time for 400 miles or so), so a delay of that time with a bandwidth of a few MHz was required. My recollection was that LC delay lines were also used, and MTI radar was very useful for close in to the airport where structures (the built environment) created the greatest clutter problem distinguishing low flying aircraft, so shorter delay times (hundreds of us) were adequate. Other techniques I have come across for various delay applications, including circulating memories included various forms of semi-distributed LC elements, coils of piano wire with magnetostrictive transducers, and early dynamic shift registers that were a kind of charge shuffling arrangement. Owen |
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