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Yagi efficiency
Does anyone know why the efficiency of the Stanford Big Dish (150 feet) is only 35% on 1420MHz, compared to 55% on 150 and 400MHz? http://www-star.stanford.edu/rsg/bigdish.php --Zack Lau W1VT More than likely, mesh in the reflector is too big and parabolic perfection is poorer at the higher frequency W4ZCB |
Yagi efficiency
Harold E. Johnson wrote: Does anyone know why the efficiency of the Stanford Big Dish (150 feet) is only 35% on 1420MHz, compared to 55% on 150 and 400MHz? http://www-star.stanford.edu/rsg/bigdish.php --Zack Lau W1VT More than likely, mesh in the reflector is too big and parabolic perfection is poorer at the higher frequency According to my interpretation of material written by Dick Knadle, K2RIW published in the ARRL Antenna Book, a reflector error on the order of 1 inch peak to peak results in a gain deterioration of 0.3 dB on 1420MHz. I doubt the mesh adds more than another 0.2 dB of loss. There is still another 1.5 dB of loss to account for the lower efficiency. Could the dish be optimized for receiving, sacrificing some gain for a better gain to temperature ratio? Zack Lau W1VT W4ZCB |
Yagi efficiency
Harold E. Johnson wrote: Does anyone know why the efficiency of the Stanford Big Dish (150 feet) is only 35% on 1420MHz, compared to 55% on 150 and 400MHz? http://www-star.stanford.edu/rsg/bigdish.php --Zack Lau W1VT More than likely, mesh in the reflector is too big and parabolic perfection is poorer at the higher frequency According to my interpretation of material written by Dick Knadle, K2RIW published in the ARRL Antenna Book, a reflector error on the order of 1 inch peak to peak results in a gain deterioration of 0.3 dB on 1420MHz. I doubt the mesh adds more than another 0.2 dB of loss. There is still another 1.5 dB of loss to account for the lower efficiency. Could the dish be optimized for receiving, sacrificing some gain for a better gain to temperature ratio? Zack Lau W1VT W4ZCB |
Yagi efficiency
"Zack" wrote in message ups.com... Harold E. Johnson wrote: Does anyone know why the efficiency of the Stanford Big Dish (150 feet) is only 35% on 1420MHz, compared to 55% on 150 and 400MHz? http://www-star.stanford.edu/rsg/bigdish.php --Zack Lau W1VT More than likely, mesh in the reflector is too big and parabolic perfection is poorer at the higher frequency According to my interpretation of material written by Dick Knadle, K2RIW published in the ARRL Antenna Book, a reflector error on the order of 1 inch peak to peak results in a gain deterioration of 0.3 dB on 1420MHz. I doubt the mesh adds more than another 0.2 dB of loss. There is still another 1.5 dB of loss to account for the lower efficiency. Could the dish be optimized for receiving, sacrificing some gain for a better gain to temperature ratio? Zack Lau W1VT W4ZCB Please be a bit more careful where you plan your responses Zack, I wasn't the one that posed that question above. I suppose that they could be under-illuminating the dish in order to suppress the "hot" ground behind it. For a dish that size though, one inch is awfully tight. Why don't you ask them? W4ZCB |
Yagi efficiency
Art Unwin wrote:
"When one looks at a radiating array pattern one can see that the yagi is very inefficient." Efficiency is output over input. Antennas can be made very efficient. When radiation resistance is large in comparison with waste (ohmic loss resistance), efficiency is high. Directivity is something else. Often, Terman answers antenna questions simply. This is such an occasion. Terman writes on page 907 of his 1955 edition of "Electronic and Radio Engineering": "The Yagi antenna of Fig. 23-39, and the corner reflector, represent about the best that can be achieved with respect to edirective gain in a compact array." Pity the fool who argues with Terman or Kraus. Best regards, Richard Harrison, KB5WZI |
Yagi efficiency
"art" wrote in message oups.com... Dan, you know quite well what the post that started this thread asked for. I only added the TOA comments to fill in some body where I was coming from not for advice on what antenna to build. People are quibling over the word "efficiency" which I find rather wierd especially since I am supposed to be in the company of fellow engineers. The subject was antenna radiation patterns and ascertaining the relative volume of the main lobe which is the reason for an antenna and comparing it to the total volume of the array which one accepts to obtain the desirable primary lobe. Oh yes, when we talk of efficiency one must multiply the ratio by 100 Some may have forgotten that! Obviously this group comprises of a swarm of tadpoles with a few little goldfish in a small pond none of which are qualified to be termed faculty. Now you have something to get your teeth into since you deign to respond to the initial post This term "I don't understand" is usually used by student who enter class after late night partying and it didn't work then either. A dull brain is a dull brain unless one activates it. Carry on with a thread of your own choice and quibble amongst yourselves about what "is" is really meant by use of the word "is" For what was a very short question this thread has gone amok and is way to long Art wrote: The moral of inventing meanings for words is that those meanings have a short shelf life. This kind of thing doesn't even last out a week in the white house press room. True, true. If only all this word-twisting energy could be harnessed as valid antenna design... the chipster seems to have relegated himself these days to fairly innocuous posts elsewhere regarding staying on the good side of your neighbors' graces by putting up visually low profile antennas... Certainly a change from the f-word antenna wars of old. I was a regular reader of r.r.a.a. in those days... not much of a poster back then, though. I wonder if a thousand-mile long, five mile high stack of rhombics might meet Art's requirements... of course, at that point you could just run open wire line to any distant receiver. That would be quite efficient, from Art's standpoint. 73, Dan Your definition of efficencency was accepted and then a very good answer within the boundaries of your definition was given which you rejected. The fact is if you could recover all the energy that goes into the sidelobes or radiates from the rear of the antenna and place it in the main beam you would increase power in that direction precious little. Apparently what you are seeking is a LASER beam performing in the HF spectrum. Even this would not be very "efficent" for communicating from one point on the surface of the earth to another point below the horizon that is to say you cant send a signal through the Earth. Communication through the air via radio is inherently inefficent if you look at it from the standpoint of thousands to millions of watts at the transmitter with only microwatts being received. In the futre we may learn to transmit nearly all of the power to a distant point. If this happenes the most efficent method of getting an HF signal across the ocean will be a moot point. By then will will be doing matter/energy/matter conversion so that we will be able to transmit ourselves over long distances if this is at all possible. In the mean time hams will continue to make do with a very inefficent medium even by todays standards It is true that in the past we have accepted many thing that were true which was not, many of these errors have been corrected at what seems to be an expotential rate over the past couple of hundred years. Much of this was accomplished by people viewing the world with a degree of open-mindedness that had never existed in the past and this is a very good thing. Being totally opened minded has it fallicies in making us not being able to recognize when we have the correct answer. My mother as I am sure a lot of other mothers have said this best. "I am open minded, just not so much as to let my brains fall out." It is our closed mindedness that keeps of from running off accepting every BS explantion that comes along It has been your choice to deem anything someone says to you that you do not agree with as RUDENESS. Perhaps we should all be POLITE to you and let you go ahead with your fools errand. I doubt if most of us could be that cruel. Actually most people are very polite to you in the truest snese of the word carefully trying to explain things to you that you clearly do not understand, trying to explain to you a reality you refuse to accept. |
Yagi efficiency
Harold E. Johnson wrote: Please be a bit more careful where you plan your responses Zack, I wasn't the one that posed that question above. My apologies--I didn't mean to make it look like you asked that question. 73--Zack Lau W1VT |
Yagi efficiency
Zack wrote:
My apologies--I didn't mean to make it look like you asked that question. The newsreader nested attributions indicated that he did not write the posting immediately following his name so you didn't really mis-attribute anything. -- 73, Cecil, http://www.qsl.net/w5dxp |
Yagi efficiency
"art" wrote in message ups.com... Dave wrote: "art" wrote in message ups.com... Richard Clark wrote: On 21 Sep 2006 19:09:38 -0700, "art" wrote: Notwithstanding that the upper half of the major lobe serves no usefull purpose to what the antenna is required for there is a mass of radiation in many directions and levels that have no connection to the required purpose of the antenna, thus we have a lot of wasted radiation that if we harness it so that it is used for the antennas primary use the efficiency of the antenna would increase immensly. Hi Art, The classic solution is to stack yagis vertically. This draws down the higher radiation lobes and puts their gain in the forward direction. Well you are getting closer to the question at hand. You have now doubled the power input but only slightly gained directionality(2db) efficiency I would also suspect that you have flattened the lower lobe only into a pancake shape. But again I go back to the desirable radiation which can be said in this case to be the lower half of the major lobes half power envelope which for a directional radiated array is very small compared to the total radiated field.True propagation can play games but the ARRL give the average arrival angles over a 11 year period so it is not a hopeless task to get a ball park figure regarding usefull radiation knowing where the target is I suppose I could make a model and slice out the half power lobe portion and compare the two volumes for myself, I just thought that it had already been looked at Oh well back to the drawing board Art what you are missing is the variability in that arrival angle. if you are interested in a specific path you must be able to receive all the possible arrival angles, which with yagi's requires mounting several of them at different heights. for instance consider a path from w1 to western europe at the sunspot peak on 10m... it is not uncommon for the band to open at a very low angle, say where a single yagi at 120' is the best antenna, then as the day progresses the angle increases so much that the 120' antenna is almost worthless but one at only 30' is working great. if you put everything into getting that 10-12 degree angle you lose out by mid morning when the arrival angle is up to 30 degrees or more... David that is not absolutely correct, we are talking about a single point to point communication where the arrival angle is below 10 degrees. If the angle of arrival is above that then it is created by unusual propagation or deflection of radiation path. For a given distance one can say that the communication energy level is comensurate with the number of skips taken where a point is reached when the number of skips controls the amount of energy left at the communication distance. Thus the east may hear the west coast talking to Europe where they cannot hear the transmitting station because of the excessive number of hops. Remember, I am talking about point to point communication which largely defined by the number of skips taken which is why dipole to dipole transmissions are pushed aside for those desiring DX contacts tho I am sure you are not advocating dipoles for DX. but at the same time that top antenna may be working great into siberia! what you are looking for is not normally called 'efficiency', but 'directivity'. unfortunately horizontally polarized yagi's vertical radiation pattern is very dependent on height do you really mean "vertical: radiation pattern? and the terrain so increasing the directivity is seen mostly in the width of the pattern. and as noted above, controlling the vertical pattern is normally done by changing the antenna height, usually by stacking multiple antennas on the tower and selecting them one at a time or in combinations to give the desired vertical coverage. No... stacking is used purely to provide a vector to combat the earths magnetic field which affects all radiation directional patterns not only a vertical pattern There have been some experiments with variable phasing of stacked yagis, but it is not a common capability in amateur installations. Exactly since these methods provide a vectoir to counteract the terrains magnetic field unfortunately this requires extra power supply points where the desire is for just one. Art you have some big misconceptions that i can't begin to address here.. but just a couple of points for you to go study on. 1. the arrival angle is not a fixed value for a point to point circuit. the angle changes with the height of the ionosphere and also with which layers are supporting the path at the time. the angle can change minute by minute, or it can be fairly constant for hours depending on the state of the ionosphere. but it will not be constant for all time. 2. also, it is not like the pretty single ray that some people draw when showing reflections off the ionosphere. the ionosphere is not a mirror, it is a gradient in a layer of ionization. the signals that are 'reflected' are actually refracted and do not arrive perfectly focused as they went up. in addition the polarization is changed which affects the efficiency of the path, this is very evident on 160m and 80m where the prefered polarization can change hour by hour over night. 3. i have no idea where you are going with this idea of stacking is to combat the earths magnetic field. the only effect the earths magnetic field has is on the ionosphere, not on how your antenna works. it is well known that changing the height of a yagi changes the vertical radiation pattern and hence the arrival angles that it favors. stacking yagis at different heights and selecting them separately or in combinations lets you adjust the elevaion pattern to compensate for the changes in the arrival angle. in most cases all the yagis in a stack are fed in phase so their signals combine at the horizon, but there have been some experiments where the phasing is changed to intentionally raise the pattern higher to cover different arrival angles more efficiently. |
Yagi efficiency
"art" wrote in message oups.com... Wow Yuri has arrived I remember that long discusting arguement he had with Tom Rauch that brought words to the fore that brought shame to amateur radio I'm gone, I want no part of what is now on the near horizon Have a great year fellars I enjoyed the short visit while it lasted Art You should rattle your head to get your memory straight. Who brought "shame" to amateur radio? W8JI for claiming nonsense that current along the antenna loading coil is constant and Art for patenting Yagi Reflector being shorter than driven element, or those who objected to fallacies being propagated on the waves of the RRAA? Looks like your logic is a little "converted" or inverted or deflected. Keep it up, you are way ahead of us :-) 73 |
Yagi efficiency
a yagi reflector CAN be shorter than the driven element, if the driven
element is longer than 1/2 wavelength... not common, but it is possible. "Yuri, K3BU" wrote in message ... "art" wrote in message oups.com... Wow Yuri has arrived I remember that long discusting arguement he had with Tom Rauch that brought words to the fore that brought shame to amateur radio I'm gone, I want no part of what is now on the near horizon Have a great year fellars I enjoyed the short visit while it lasted Art You should rattle your head to get your memory straight. Who brought "shame" to amateur radio? W8JI for claiming nonsense that current along the antenna loading coil is constant and Art for patenting Yagi Reflector being shorter than driven element, or those who objected to fallacies being propagated on the waves of the RRAA? Looks like your logic is a little "converted" or inverted or deflected. Keep it up, you are way ahead of us :-) 73 |
Yagi efficiency
Dave wrote:
a yagi reflector CAN be shorter than the driven element, if the driven element is longer than 1/2 wavelength... not common, but it is possible. We already know how much Yuri doesn't. ;) tom |
Yagi efficiency
Cecil, efficiency depends on what your objectives are
The yagi antennas objective is to obtain a radiation beam of gain compared to radiation else where. What is wanted is a radiation lobe that one can use to direct communication. ..rThe yagi achieves the object of producing a lobe which has a higher gain than other lobes that the yagi produces.( A higher ratio) The yagi achieves its object by producing this main lobe but at what cost? If we look at pattern volume as reflecting as energy applied to the yagi we must compare that volume with the whole pattern volume. This means comparing the volume of the upper lobes, the side lobes, the rear lobe and of course the vertical lobe to the main lobe. Any cursury look at a three D radiation pattern will immediately see that the main lobe is less than 50 % of the total radiation pattern Let us look at a common dipole with a reflector, the planar view of radiation which ignores radiation outside the plane is a figure 8 where the addition of a reflector does nothing to enhance increased forward radiation so immidiately we can say that the forward lobe achieves what is termed a major lobe plus other forward lobes outside of the main lobe where as the radiation to the rear achieves nothing that enhances the forward main lobe. So just comparing the forward and the rear lobe we have only achieved 50 per cent of our object and this is not counting other losses. Now you may disagree with the objective of a yagi beam and I understand that may be the case. Hopefully the above answers your request to define efficiency as I was with respect to the yagi antenna. I think the above pretty much explains what I stated in the initial post tho it appears that some read inbetween the lines to read what they wanted to read as a diversionary tactic and there is not much anybody can do about that. One really has to ask themselves the question that if an antenna came on the market with only one main lobe would they buy it Art. Cecil Moore wrote: art wrote: When one looks at a.radiating array pattern one can see that the yagi is very inefficient. Please define "efficiency". -- 73, Cecil, http://www.w5dxp.com |
Yagi efficiency
Cecil, efficiency depends on what your objectives are
The yagi antennas objective is to obtain a radiation beam of gain compared to radiation else where. What is wanted is a radiation lobe that one can use to direct communication. ..rThe yagi achieves the object of producing a lobe which has a higher gain than other lobes that the yagi produces.( A higher ratio) The yagi achieves its object by producing this main lobe but at what cost? If we look at pattern volume as reflecting as energy applied to the yagi we must compare that volume with the whole pattern volume. This means comparing the volume of the upper lobes, the side lobes, the rear lobe and of course the vertical lobe to the main lobe. Any cursury look at a three D radiation pattern will immediately see that the main lobe is less than 50 % of the total radiation pattern Let us look at a common dipole with a reflector, the planar view of radiation which ignores radiation outside the plane is a figure 8 where the addition of a reflector does nothing to enhance increased forward radiation so immidiately we can say that the forward lobe achieves what is termed a major lobe plus other forward lobes outside of the main lobe where as the radiation to the rear achieves nothing that enhances the forward main lobe. So just comparing the forward and the rear lobe we have only achieved 50 per cent of our object and this is not counting other losses. Now you may disagree with the objective of a yagi beam and I understand that may be the case. Hopefully the above answers your request to define efficiency as I was with respect to the yagi antenna. I think the above pretty much explains what I stated in the initial post tho it appears that some read inbetween the lines to read what they wanted to read as a diversionary tactic and there is not much anybody can do about that. One really has to ask themselves the question that if an antenna came on the market with only one main lobe would they buy it Art. Cecil Moore wrote: art wrote: When one looks at a.radiating array pattern one can see that the yagi is very inefficient. Please define "efficiency". -- 73, Cecil, http://www.w5dxp.com |
Yagi efficiency
art wrote:
. . . Any cursury look at a three D radiation pattern will immediately see that the main lobe is less than 50 % of the total radiation pattern . . . Out of curiosity, did you a) not read b) not understand, or c) not believe what I posted about the fraction of power in a Yagi's minor lobes? A cursory look at a 3D pattern is probably one of the least reliable ways to determine anything quantitative about an antenna pattern. By choosing the scale (e.g., field strength, power density, linear dB, ARRL-scale dB), you can make the relative sizes of the lobes just about anything you'd like and lead the casual observer to the conclusion of your choice(*). But why bother trying to divine a value from a 3D pattern, when it's so simple to numerically show that the power in the lobes is insignificant? (*) One of the slides in the "Antenna Basics" talk I've given at many hamfests shows several very different directional patterns, and I ask the audience which one is the most desirable. After the votes are in, I reveal that they're all the same antenna, just drawn to different common and legitimate scales. Roy Lewallen, W7EL |
Yagi efficiency
Roy Lewallen wrote: art wrote: . . . Any cursury look at a three D radiation pattern will immediately see that the main lobe is less than 50 % of the total radiation pattern . . . Out of curiosity, did you a) not read b) not understand, or snip I did not understand your logic. Front to back means nothing in terms of energy containment The measerment is a ratio not a quantity It also is a ratio only for a given plane and does not account for anything outside that plane. Have I stated anything wrong there? Point out the error of my ways starting with a simple dipole. Does any additional element to the array revert the radiation from the rear direction so that it is additive to the forward directive radiation of the main lobe? If so what percentage of the rearward radiation in the rear hemisphere,,(ot a planar amount) ? The question is to you Roy to answer for a one on one,It would help if you gave an actual percentage instead of a "major fraction" which you stated before And if you don't understand then just drop the thread as it has gone on way to long with relatively little specifics with respect to the original post Art c) not believe what I posted about the fraction of power in a Yagi's minor lobes? A cursory look at a 3D pattern is probably one of the least reliable ways to determine anything quantitative about an antenna pattern. By choosing the scale (e.g., field strength, power density, linear dB, ARRL-scale dB), you can make the relative sizes of the lobes just about anything you'd like and lead the casual observer to the conclusion of your choice(*). But why bother trying to divine a value from a 3D pattern, when it's so simple to numerically show that the power in the lobes is insignificant? I do not remember seeing any numerical answer ,was it specific and relative to the contained energy in the primary lobe because that is what I was looking for ? What was the actual percentage that you arrived at? (*) One of the slides in the "Antenna Basics" talk I've given at many Roy the actual scale doesn't matter one iota on a given pattern with respect to my question ! To compare different patterns one must have a common denominator such as scale, to do otherwise is an attempt to deceive. You also use the word "desirable"and my connoctation of that is a major lobe and nothing else whereas some may look for other characteristics. Did the group come to a consensus as to what was desirable? Some may want to hear what is said behind their backs! erns, and I ask the audience which one is the most desirable. After the votes are in, I reveal that they're all the same antenna, just drawn to different common and legitimate scales. Roy Lewallen, W7EL |
Yagi efficiency
art wrote:
I did not understand your logic. Front to back means nothing in terms of energy containment The measerment is a ratio not a quantity It also is a ratio only for a given plane and does not account for anything outside that plane. Have I stated anything wrong there? I thought your interest was in the amount of power contained in lobes other than the main lobe of a Yagi. My posting showed a simple way to relate front to back ratio, which is commonly known for many Yagis, to the fraction of power in secondary lobes, which is not. Point out the error of my ways starting with a simple dipole. Does any additional element to the array revert the radiation from the rear direction so that it is additive to the forward directive radiation of the main lobe? Of course. If so what percentage of the rearward radiation in the rear hemisphere,,(ot a planar amount) ? The question is to you Roy to answer for a one on one,It would help if you gave an actual percentage instead of a "major fraction" which you stated before In my earlier posting I apparently overestimated your ability to do what I thought was a simple calculation. So I'll do it for you so you can have a number. Since there's no "typical" Yagi, I presented one which most people would consider to be worse than average -- one having only a 6 dB front/back ratio. I also assumed for a starting point that the shape of the rear lobe (that is, beamwidth and height) is the same as the front lobe. The first calculation is to determine just what the ratio is of the powers in the front and rear lobe. The answer is 4:1. That is, the front lobe contains four times the power of the rear lobe. Since you seem to be interested in energy rather than power, simply consider the amount of energy each radiates in some amount of time: each second or other unit of time, the forward lobe radiates four times the energy of the rear lobe. What this says is that if you manage to get all the reverse-lobe power (or energy, if you prefer) into the front lobe, without any change in the front lobe's shape, you'd increase the gain just about exactly 1 dB. If you end up fattening it, you'll lose some or all of that gain. So there are some numbers for you. You'll have to do a bit of estimating if the rear lobe is fatter or skinnier than the front lobe, but now you have a number to start from. Or let's say that the front/back is 10 dB instead of 6, a more typical number for a Yagi. With the same criterion of similar lobe shapes, the power ratio for the front and rear lobes is 10:1. So if you got all that rear lobe power or energy into the front lobe without changing its shape, you'd gain a whopping 0.4 dB. If you had two equal rear lobes, both 10 dB below the front lobe, and both of the same shape as the front lobe, the power ratio of the front to all rear lobes would be 5:1, and you'd be able to increase your forward gain by 0.8 dB if you got all that rear power into the front lobe without changing its shape. So there's your actual percentage -- around 25% for a very poor Yagi, and around 10 - 20% for a fair-to-middlin' one. From which you could gain about a dB by very hard work in getting all that rear lobe power into the front lobe(*). If you question any of the calculations, I'll be glad to show how I converted ratios to dB and vice-versa, although you should be able to find this in many publications, as well as on the web. Or you can continue drawing your conclusions from cursory looks at 3D plots. Your choice. And if you don't understand then just drop the thread as it has gone on way to long with relatively little specifics with respect to the original post I'm afraid I do understand, but it's a good idea anyway. (*) Being an engineer, I didn't include placebo effect gain in the calculations. After a lot of hard work squeezing every last bit of power into that front lobe, the signals are going to *seem* a lot stronger, and the reports sure to be better. Roy Lewallen, W7EL |
Yagi efficiency
art wrote:
Cecil, efficiency depends on what your objectives are ... I guess that is why there are 20 definitions for "efficiency" in the IEEE Dictionary. One needs to state one's definition of "efficiency" at the beginning of the discussion to avoid confusion with all the other possible definitions. For instance, Power Company EEs have a different definition of "power" than do physicists, politicians, and priests. -- 73, Cecil http://www.w5dxp.com |
Yagi efficiency
Roy Lewallen wrote: art wrote: I did not understand your logic. Front to back means nothing in terms of energy containment The measerment is a ratio not a quantity It also is a ratio only for a given plane and does not account for anything outside that plane. Have I stated anything wrong there? I thought your interest was in the amount of power contained in lobes other than the main lobe of a Yagi. My posting showed a simple way to relate front to back ratio, which is commonly known for many Yagis, to the fraction of power in secondary lobes, which is not. Point out the error of my ways starting with a simple dipole. Does any additional element to the array revert the radiation from the rear direction so that it is additive to the forward directive radiation of the main lobe? Of course. If so what percentage of the rearward radiation in the rear hemisphere,,(ot a planar amount) ? The question is to you Roy to answer for a one on one,It would help if you gave an actual percentage instead of a "major fraction" which you stated before In my earlier posting I apparently overestimated your ability to do what I thought was a simple calculation. So I'll do it for you so you can have a number. Since there's no "typical" Yagi, I presented one which most people would consider to be worse than average -- one having only a 6 dB front/back ratio. I also assumed for a starting point that the shape of the rear lobe (that is, beamwidth and height) is the same as the front lobe. The first calculation is to determine just what the ratio is of the powers in the front and rear lobe. The answer is 4:1. That is, the front lobe contains four times the power of the rear lobe. I am not interested in front to back for what I am looking for but this 4:1 has my interest What does it represent and how did you get it? The rear usually has more than one lobe and the reflector ndestructs or deflects the energy to 90 degrees of impact. But that 4:1 figure where does it come from? Art Since you seem to be interested in energy rather than power, simply consider the amount of energy each radiates in some amount of time: each second or other unit of time, the forward lobe radiates four times the energy of the rear lobe. What this says is that if you manage to get all the reverse-lobe power (or energy, if you prefer) into the front lobe, without any change in the front lobe's shape, you'd increase the gain just about exactly 1 dB. If you end up fattening it, you'll lose some or all of that gain. So there are some numbers for you. You'll have to do a bit of estimating if the rear lobe is fatter or skinnier than the front lobe, but now you have a number to start from. Or let's say that the front/back is 10 dB instead of 6, a more typical number for a Yagi. With the same criterion of similar lobe shapes, the power ratio for the front and rear lobes is 10:1. So if you got all that rear lobe power or energy into the front lobe without changing its shape, you'd gain a whopping 0.4 dB. If you had two equal rear lobes, both 10 dB below the front lobe, and both of the same shape as the front lobe, the power ratio of the front to all rear lobes would be 5:1, and you'd be able to increase your forward gain by 0.8 dB if you got all that rear power into the front lobe without changing its shape. So there's your actual percentage -- around 25% for a very poor Yagi, and around 10 - 20% for a fair-to-middlin' one. From which you could gain about a dB by very hard work in getting all that rear lobe power into the front lobe(*). If you question any of the calculations, I'll be glad to show how I converted ratios to dB and vice-versa, although you should be able to find this in many publications, as well as on the web. Or you can continue drawing your conclusions from cursory looks at 3D plots. Your choice. And if you don't understand then just drop the thread as it has gone on way to long with relatively little specifics with respect to the original post I'm afraid I do understand, but it's a good idea anyway. (*) Being an engineer, I didn't include placebo effect gain in the calculations. After a lot of hard work squeezing every last bit of power into that front lobe, the signals are going to *seem* a lot stronger, and the reports sure to be better. Roy Lewallen, W7EL |
Yagi efficiency
"art" wrote in message oups.com... Cecil, efficiency depends on what your objectives are The yagi antennas objective is to obtain a radiation beam of gain compared to radiation else where. What is wanted is a radiation lobe that one can use to direct communication. ..rThe yagi achieves the object of producing a lobe which has a higher gain than other lobes that the yagi produces.( A higher ratio) The yagi achieves its object by producing this main lobe but at what cost? If we look at pattern volume as reflecting as energy applied to the yagi we must compare that volume with the whole pattern volume. This means comparing the volume of the upper lobes, the side lobes, the rear lobe and of course the vertical lobe to the main lobe. Any cursury look at a three D radiation pattern will immediately see that the main lobe is less than 50 % of the total radiation pattern Let us look at a common dipole with a reflector, the planar view of radiation which ignores radiation outside the plane is a figure 8 where the addition of a reflector does nothing to enhance increased forward radiation so immidiately we can say that the forward lobe achieves what is termed a major lobe plus other forward lobes outside of the main lobe where as the radiation to the rear achieves nothing that enhances the forward main lobe. So just comparing the forward and the rear lobe we have only achieved 50 per cent of our object and this is not counting other losses. Now you may disagree with the objective of a yagi beam and I understand that may be the case. Hopefully the above answers your request to define efficiency as I was with respect to the yagi antenna. I think the above pretty much explains what I stated in the initial post tho it appears that some read inbetween the lines to read what they wanted to read as a diversionary tactic and there is not much anybody can do about that. One really has to ask themselves the question that if an antenna came on the market with only one main lobe would they buy it Art. Cecil Moore wrote: art wrote: When one looks at a.radiating array pattern one can see that the yagi is very inefficient. Please define "efficiency". -- 73, Cecil, http://www.w5dxp.com There are already words defined to mean the antenna parameters you are talking about. I suggest you use these instead of defining yur own so people will know what you are talking about. Antenna patterns are expressed in db. This means they are logarthmicly compressed. IF they were displayed linearly the sidelobes would would be invisible on the graph. Again. ad nauseum, there is no significant power in a sidelobe of any reasonably designed yagi antenna.. |
Yagi efficiency
On 29 Sep 2006 05:47:14 -0700, "art" wrote:
one having only a 6 dB front/back ratio. But that 4:1 figure where does it come from? Hi Art, Do you know how to work a calculator using logarithms? 73's Richard Clark, KB7QHC |
Yagi efficiency
Art wrote:
"So just comparing the forward and rear lobe we have only achieved 50 per cent of our objective and this is not counting other losses." Adding a director or reflector in the plane of a dipole can make it nearly unidirectional. It will have forward gain over the dipole alone. Adding more directors can increase forward gain. Losses of the radiator and parasitic ellements to heat in them can be made small and antenna efficiency high. Best regards, Richard Harrison, KB5WZI |
Yagi efficiency
art wrote:
Roy Lewallen wrote: Since there's no "typical" Yagi, I presented one which most people would consider to be worse than average -- one having only a 6 dB front/back ratio. I also assumed for a starting point that the shape of the rear lobe (that is, beamwidth and height) is the same as the front lobe. The first calculation is to determine just what the ratio is of the powers in the front and rear lobe. The answer is 4:1. That is, the front lobe contains four times the power of the rear lobe. I am not interested in front to back for what I am looking for but this 4:1 has my interest What does it represent I can't think how I can state it any more clearly than I did in the last sentence of the text just above which you quoted. and how did you get it? When dealing with a power ratio, dB = 10 * log(ratio). Solving for ratio: ratio = 10^(dB/10) Here's where you'll probably need to get out that pocket calculator. dB is 6 (see above text), so ratio = 10^(0.6) ~ 4. Conversion between ratios and dB is a skill that anyone interested in antennas should develop. I had assumed that it was part of the knowledge required to pass a general class amateur exam, but apparently I was mistaken. If the calculator operations are too complex for you, get a chart of conversion factors which have already been calculated. The rear usually has more than one lobe True. See the remainder of my previous posting for a discussion of this. and the reflector ndestructs or deflects the energy to 90 degrees of impact. That's more nonsense. You'd develop a much better understanding of antennas (or any physical system) by developing and learning to apply some basic math skills than by dreaming up alternate explanations for well-known physical phenomena. I don't believe I can help you any more -- if indeed I've helped you at all --, and think (or at least hope) that most other readers have understood what I'm saying. So I'll bow out here. Roy Lewallen, W7EL |
Yagi efficiency
Terman treats decibels on page 8 of the 1955 third edition of
"Electronic and Radio Engineering". The value of the decibel is 10 log of the power ratio. When the ratio of the powers is 4, the decibel value is 6. This 6 dB value applies among other things to doubling the distance between a transmitting and receiving antenna. Half as many volts will be induced in the receiver and will result in half as many amps. This is 1/4 the power induced at half the distance between antennas..This may be expressed as a positive power ratio of 4 to 1, or 6 dB. Best regards, Richard Harrison, KB5WZI |
Yagi efficiency
I had to ask rather than assume. My inclination where it came from
which you didn't say was that since the field produced by an actual antenna is twice as great as the field produced by the isotropic antenna the gain RATIO is two and the power gain is 2 squared which is 4. this means that to produce the same field strength at the same distance, four times as much power would have to be supplied to an isotropic radiator as to the actual antenna under consideration. But as I stated many times RATIO as you are using it has not interest to me as it is not relevant. What you are doing is based on a RATIO at a given plane and that RATIO changes with the plane examined. That is why the yagi is termed a planar array In other words a reflector is used to affect a single plane of radiation it is not all encompassing of the total rear radiation. On top of all that the plane chosen is along the plane of the main lobe only and does not in anyway include the ratio of the second lobe to the rear or any nulls that are made. The rear radiation fields is no way a mirror image of the forward radiated field. You are supplying a conventional answer to a convential question which revolves around a single plane where I am speaking of the total radiation field. You can't keep trotting out the conventional answer to the question that you want to be posed. I am sure glad I didn't guess where you were getting the figure 4 from otherwise the thread would have been 200 posts long plus a lot of accusations as to who said what.Get back to basics and stop trying to section the field of a dipole to make it easier to simplify for newcomers, it does not represent factually everything. it is just a means to an end. without involvement in the toital "wave and fields" subject As I have oft times stated I am looking at the whole pattern in three dimensional form and you keep trotting out answers based on a two dimensional format Art , Roy Lewallen wrote: art wrote: Roy Lewallen wrote: Since there's no "typical" Yagi, I presented one which most people would consider to be worse than average -- one having only a 6 dB front/back ratio. I also assumed for a starting point that the shape of the rear lobe (that is, beamwidth and height) is the same as the front lobe. See, you are building a house on the basis of an assumption such that instead of a rock that you guessed was there it really was just sand. The first calculation is to determine just what the ratio is of the powers in the front and rear lobe. The answer is 4:1. That is, the front lobe contains four times the power of the rear lobe. I am not interested in front to back for what I am looking for but this 4:1 has my interest What does it represent I can't think how I can state it any more clearly than I did in the last sentence of the text just above which you quoted. and how did you get it? When dealing with a power ratio, dB = 10 * log(ratio). Solving for ratio: ratio = 10^(dB/10) Here's where you'll probably need to get out that pocket calculator. dB is 6 (see above text), so ratio = 10^(0.6) ~ 4. Conversion between ratios and dB is a skill that anyone interested in antennas should develop. I had assumed that it was part of the knowledge required to pass a general class amateur exam, but apparently I was mistaken. If the calculator operations are too complex for you, get a chart of conversion factors which have already been calculated. The rear usually has more than one lobe True. See the remainder of my previous posting for a discussion of this. and the reflector ndestructs or deflects the energy to 90 degrees of impact. That's more nonsense. You'd develop a much better understanding of antennas (or any physical system) by developing and learning to apply some basic math skills than by dreaming up alternate explanations for well-known physical phenomena. I don't believe I can help you any more -- if indeed I've helped you at all --, and think (or at least hope) that most other readers have understood what I'm saying. So I'll bow out here. Roy Lewallen, W7EL |
Yagi efficiency
"art" wrote in message ups.com... I had to ask rather than assume. My inclination where it came from which you didn't say was that since the field produced by an actual antenna is twice as great as the field produced by the isotropic antenna the gain RATIO is two and the power gain is 2 squared which is 4. this means that to produce the same field strength at the same distance, four times as much power would have to be supplied to an isotropic radiator as to the actual antenna under consideration. But as I stated many times RATIO as you are using it has not interest to me as it is not relevant. What you are doing is based on a RATIO at a given plane and that RATIO changes with the plane examined. That is why the yagi is termed a planar array In other words a reflector is used to affect a single plane of radiation it is not all encompassing of the total rear radiation. On top of all that the plane chosen is along the plane of the main lobe only and does not in anyway include the ratio of the second lobe to the rear or any nulls that are made. The rear radiation fields is no way a mirror image of the forward radiated field. You are supplying a conventional answer to a convential question which revolves around a single plane where I am speaking of the total radiation field. You can't keep trotting out the conventional answer to the question that you want to be posed. I am sure glad I didn't guess where you were getting the figure 4 from otherwise the thread would have been 200 posts long plus a lot of accusations as to who said what.Get back to basics and stop trying to section the field of a dipole to make it easier to simplify for newcomers, it does not represent factually everything. it is just a means to an end. without involvement in the toital "wave and fields" subject As I have oft times stated I am looking at the whole pattern in three dimensional form and you keep trotting out answers based on a two dimensional format Art then i would suggest learning some of the nitty gritty details of a program like nec and figure out how to integrate it's field values over the 3d surface and sort out the values you are interested in. no one here will do that for you since it is normally not of interest in amateur antenna design. we all understand how to evaluate the performance of antennas for our 'normal' uses in terms of gain and f/b ratio and how to read those 2d slices to evaluate side lobes for our 'normal' uses. as you have stated it your desire is not a normal one, you have special requirements which will require a special solution that is not readily available for amateur antennas.... maybe that data is available for large satellite or deep space dishes where they worry about extreme details of side lobe power and noise temperatures, but not for hf ham use with normal antennas. |
Yagi efficiency
On 29 Sep 2006 12:55:37 -0700, "art" wrote:
As I have oft times stated I am looking at the whole pattern in three dimensional form and you keep trotting out answers based on a two dimensional format Art, The same process in any plane reveals the same net result: you are not going to achieve any more "efficiency" than that already offered by a Yagi. In fact, your design probably suffers extensively with regard to "efficiency." But no one knows this mystery design, do they? Sorry, but Fritz has already cornered the market on flim-flam. He has probably been more efficient about it too (if measured in sucker deposits). 73's Richard Clark, KB7QHC |
Yagi efficiency
On 29 Sep 2006 12:55:37 -0700, "art" wrote:
As I have oft times stated I am looking at the whole pattern in three dimensional form and you keep trotting out answers based on a two dimensional format Art, As I re-consider this statement, I don't believe you at all. The earliest solutions to your "problem" were satisfied by stacked yagis. They also answer what you complain of above as well. Bay arrangements of yagis go even further. As they are skeletal versions of a massive dipole array against a screen, all are solutions that are merely the natural consequence of massive duplication and constructive phase shift. This stuff has been around for half a century or more and you have yet to reveal anything new, much less a method that transcends existing knowledge. If you had more experience in using modelers, and examining the history of antenna design, then you could confidently make the statement above. However, nothing in your correspondence even reveals you understand the fundamentals beyond parroting phrases cut and paste from other sources. 73's Richard Clark, KB7qHC |
Yagi efficiency
"art" wrote in 1159495614.320553.169910
@i42g2000cwa.googlegroups.com: Let us look at a common dipole with a reflector, the planar view of radiation which ignores radiation outside the plane is a figure 8 For the sake of the arguement, let's say we're feeding the antenna with 100W, so 50W goes one way, and 50W goes the other way. Correct? where the addition of a reflector does nothing to enhance increased forward radiation Now the 50W going towards the reflector... What happens to it? Heat? Reflected back down the feed line? (Sorry...) so immidiately we can say that the forward lobe achieves what is termed a major lobe plus other forward lobes outside of the main lobe where as the radiation to the rear achieves nothing that enhances the forward main lobe. So the most efficient antenna is the isotropic, because its radiating volume is a sphere. Next would be a dipole, then a vertical, and then a yagi with just 1 parasitic element, and getting worse as you add elements, because each element is shaving a bit off the volume. Correct? -- David Hatch KR7DH |
Yagi efficiency
David Hatch wrote: "art" wrote in 1159495614.320553.169910 @i42g2000cwa.googlegroups.com: Let us look at a common dipole with a reflector, the planar view of radiation which ignores radiation outside the plane is a figure 8 For the sake of the arguement, let's say we're feeding the antenna with 100W, so 50W goes one way, and 50W goes the other way. Correct? where the addition of a reflector does nothing to enhance increased forward radiation Now the 50W going towards the reflector... What happens to it? Heat? Reflected back down the feed line? (Sorry...) so immidiately we can say that the forward lobe achieves what is termed a major lobe plus other forward lobes outside of the main lobe where as the radiation to the rear achieves nothing that enhances the forward main lobe. So the most efficient antenna is the isotropic, because its radiating volume is a sphere. Next would be a dipole, then a vertical, and then a yagi with just 1 parasitic element, and getting worse as you add elements, because each element is shaving a bit off the volume. Correct? -- David Hatch KR7DH It is true that a vertical monopole antenna will have a larger total footprint of coverage than a yagi. If the earth was evenly coated with ham radio operators I could probably make more contacts using a vertical monopole than I could a yagi that could not be rotated. |
Yagi efficiency
I believe you are correct.
If you understand the question posted over a 100 posts ago why is it that others are stumbling. I could not figure out how to determine the volume mathematically so I took the model making route which confirms the poor efficiency of the yagi. What blows my mind is the assertion that the major lobe is a large fraction of the total volume whatever a large fraction really means ( no hints given by the poster) plus the idea that volume outside the main lobe is miniscule,.Seems like memorisation of required answers is the way to go with amateur radio at the moment. Thinking from first principles obviously not required just give an answer that you want to give regardless what the question was and then blame the poster because he didn't pose the correct question for which the answer was well suited. If you can't provide an answer then change the subject and then discuss that Well I am glad somebody read that first post for what it said not for what most wanted to read. I feel a lot better now Art Dave wrote: "art" wrote in message ups.com... I had to ask rather than assume. My inclination where it came from which you didn't say was that since the field produced by an actual antenna is twice as great as the field produced by the isotropic antenna the gain RATIO is two and the power gain is 2 squared which is 4. this means that to produce the same field strength at the same distance, four times as much power would have to be supplied to an isotropic radiator as to the actual antenna under consideration. But as I stated many times RATIO as you are using it has not interest to me as it is not relevant. What you are doing is based on a RATIO at a given plane and that RATIO changes with the plane examined. That is why the yagi is termed a planar array In other words a reflector is used to affect a single plane of radiation it is not all encompassing of the total rear radiation. On top of all that the plane chosen is along the plane of the main lobe only and does not in anyway include the ratio of the second lobe to the rear or any nulls that are made. The rear radiation fields is no way a mirror image of the forward radiated field. You are supplying a conventional answer to a convential question which revolves around a single plane where I am speaking of the total radiation field. You can't keep trotting out the conventional answer to the question that you want to be posed. I am sure glad I didn't guess where you were getting the figure 4 from otherwise the thread would have been 200 posts long plus a lot of accusations as to who said what.Get back to basics and stop trying to section the field of a dipole to make it easier to simplify for newcomers, it does not represent factually everything. it is just a means to an end. without involvement in the toital "wave and fields" subject As I have oft times stated I am looking at the whole pattern in three dimensional form and you keep trotting out answers based on a two dimensional format Art then i would suggest learning some of the nitty gritty details of a program like nec and figure out how to integrate it's field values over the 3d surface and sort out the values you are interested in. no one here will do that for you since it is normally not of interest in amateur antenna design. we all understand how to evaluate the performance of antennas for our 'normal' uses in terms of gain and f/b ratio and how to read those 2d slices to evaluate side lobes for our 'normal' uses. as you have stated it your desire is not a normal one, you have special requirements which will require a special solution that is not readily available for amateur antennas.... maybe that data is available for large satellite or deep space dishes where they worry about extreme details of side lobe power and noise temperatures, but not for hf ham use with normal antennas. |
Yagi efficiency
art wrote: I believe you are correct. If you understand the question posted over a 100 posts ago why is it that others are stumbling. I could not figure out how to determine the volume mathematically so I took the model making route which confirms the poor efficiency of the yagi. What blows my mind is the assertion that the major lobe is a large fraction of the total volume whatever a large fraction really means ( no hints given by the poster) plus the idea that volume outside the main lobe is miniscule,.Seems like memorisation of required answers is the way to go with amateur radio at the moment. Thinking from first principles obviously not required just give an answer that you want to give regardless what the question was and then blame the poster because he didn't pose the correct question for which the answer was well suited. If you can't provide an answer then change the subject and then discuss that Well I am glad somebody read that first post for what it said not for what most wanted to read. I feel a lot better now Art Dave wrote: "art" wrote in message ups.com... I had to ask rather than assume. My inclination where it came from which you didn't say was that since the field produced by an actual antenna is twice as great as the field produced by the isotropic antenna the gain RATIO is two and the power gain is 2 squared which is 4. this means that to produce the same field strength at the same distance, four times as much power would have to be supplied to an isotropic radiator as to the actual antenna under consideration. But as I stated many times RATIO as you are using it has not interest to me as it is not relevant. What you are doing is based on a RATIO at a given plane and that RATIO changes with the plane examined. That is why the yagi is termed a planar array In other words a reflector is used to affect a single plane of radiation it is not all encompassing of the total rear radiation. On top of all that the plane chosen is along the plane of the main lobe only and does not in anyway include the ratio of the second lobe to the rear or any nulls that are made. The rear radiation fields is no way a mirror image of the forward radiated field. You are supplying a conventional answer to a convential question which revolves around a single plane where I am speaking of the total radiation field. You can't keep trotting out the conventional answer to the question that you want to be posed. I am sure glad I didn't guess where you were getting the figure 4 from otherwise the thread would have been 200 posts long plus a lot of accusations as to who said what.Get back to basics and stop trying to section the field of a dipole to make it easier to simplify for newcomers, it does not represent factually everything. it is just a means to an end. without involvement in the toital "wave and fields" subject As I have oft times stated I am looking at the whole pattern in three dimensional form and you keep trotting out answers based on a two dimensional format Art then i would suggest learning some of the nitty gritty details of a program like nec and figure out how to integrate it's field values over the 3d surface and sort out the values you are interested in. no one here will do that for you since it is normally not of interest in amateur antenna design. we all understand how to evaluate the performance of antennas for our 'normal' uses in terms of gain and f/b ratio and how to read those 2d slices to evaluate side lobes for our 'normal' uses. as you have stated it your desire is not a normal one, you have special requirements which will require a special solution that is not readily available for amateur antennas.... maybe that data is available for large satellite or deep space dishes where they worry about extreme details of side lobe power and noise temperatures, but not for hf ham use with normal antennas. The major lobe is a very large portion of the total power, it has been figured out but I doubt if anyone wants to figure it out again for any particular yagi. I know I could care less, but it is obvious from looking at the plotted radiation patterns that sidelobe power is very small amount easily in the 2% ball park of the total amount. Of course some yagis will be better at concentratining the power in the main lobe than others. By the way ther is 3d yagi antenna pattern information available. Just find plots for the antenna mounted horizontally and vertically. This is something almost any antenna simulation program can provide. |
Yagi efficiency
JIMMIE wrote: art wrote: I believe you are correct. If you understand the question posted over a 100 posts ago why is it that others are stumbling. I could not figure out how to determine the volume mathematically so I took the model making route which confirms the poor efficiency of the yagi. What blows my mind is the assertion that the major lobe is a large fraction of the total volume whatever a large fraction really means ( no hints given by the poster) plus the idea that volume outside the main lobe is miniscule,.Seems like memorisation of required answers is the way to go with amateur radio at the moment. Thinking from first principles obviously not required just give an answer that you want to give regardless what the question was and then blame the poster because he didn't pose the correct question for which the answer was well suited. If you can't provide an answer then change the subject and then discuss that Well I am glad somebody read that first post for what it said not for what most wanted to read. I feel a lot better now Art Dave wrote: "art" wrote in message ups.com... I had to ask rather than assume. My inclination where it came from which you didn't say was that since the field produced by an actual antenna is twice as great as the field produced by the isotropic antenna the gain RATIO is two and the power gain is 2 squared which is 4. this means that to produce the same field strength at the same distance, four times as much power would have to be supplied to an isotropic radiator as to the actual antenna under consideration. But as I stated many times RATIO as you are using it has not interest to me as it is not relevant. What you are doing is based on a RATIO at a given plane and that RATIO changes with the plane examined. That is why the yagi is termed a planar array In other words a reflector is used to affect a single plane of radiation it is not all encompassing of the total rear radiation. On top of all that the plane chosen is along the plane of the main lobe only and does not in anyway include the ratio of the second lobe to the rear or any nulls that are made. The rear radiation fields is no way a mirror image of the forward radiated field. You are supplying a conventional answer to a convential question which revolves around a single plane where I am speaking of the total radiation field. You can't keep trotting out the conventional answer to the question that you want to be posed. I am sure glad I didn't guess where you were getting the figure 4 from otherwise the thread would have been 200 posts long plus a lot of accusations as to who said what.Get back to basics and stop trying to section the field of a dipole to make it easier to simplify for newcomers, it does not represent factually everything. it is just a means to an end. without involvement in the toital "wave and fields" subject As I have oft times stated I am looking at the whole pattern in three dimensional form and you keep trotting out answers based on a two dimensional format Art then i would suggest learning some of the nitty gritty details of a program like nec and figure out how to integrate it's field values over the 3d surface and sort out the values you are interested in. no one here will do that for you since it is normally not of interest in amateur antenna design. we all understand how to evaluate the performance of antennas for our 'normal' uses in terms of gain and f/b ratio and how to read those 2d slices to evaluate side lobes for our 'normal' uses. as you have stated it your desire is not a normal one, you have special requirements which will require a special solution that is not readily available for amateur antennas.... maybe that data is available for large satellite or deep space dishes where they worry about extreme details of side lobe power and noise temperatures, but not for hf ham use with normal antennas. The major lobe is a very large portion of the total power, it has been figured out but I doubt if anyone wants to figure it out again for any particular yagi. I know I could care less, but it is obvious from looking at the plotted radiation patterns that sidelobe power is very small amount easily in the 2% ball park of the total amount. Of course some yagis will be better at concentratining the power in the main lobe than others. By the way ther is 3d yagi antenna pattern information available. Just find plots for the antenna mounted horizontally and vertically. This is something almost any antenna simulation program can provide. Like other I didnt understand the equestion as origionally posted either. This was probably due to your false statement requardinding the efficency or lack there of as you define efficentcy of a yagi antenna. AS you say that you can take a look at an antenna plot see that it is obviously inefficent without showing the mathmatics I can look at one and tell you it is very efficent per your own definition without giving the numbers. I can only assume you are confused by the fact the plots are drawn with a LOG scale as opposed to a linear scale. If drawn using a linear scale the side lobes would be 1/100 to 1/1000 the size of the main beam. If you dont want to take my word for simply take any yagi antenna plot and redraw it to a linear scale. |
Yagi efficiency
art wrote:
Cecil, efficiency depends on what your objectives are snip bull**** Art. Art You are obviously much smarter than every one here combined. So I will leave it up to you to design the antenna(s) that no one has been able to come up with before this miracle antenna you envision. The tens of millions of man hours we have put into antenna developement cannot possibly equal your intelligence. Prove everyone wrong. Go ahead. We're waiting. tom K0TAR |
Yagi efficiency
Richard Clark wrote:
On 29 Sep 2006 05:47:14 -0700, "art" wrote: one having only a 6 dB front/back ratio. But that 4:1 figure where does it come from? Hi Art, Do you know how to work a calculator using logarithms? 73's Richard Clark, KB7QHC |
Yagi efficiency
Richard Clark wrote:
On 29 Sep 2006 05:47:14 -0700, "art" wrote: one having only a 6 dB front/back ratio. But that 4:1 figure where does it come from? Hi Art, Do you know how to work a calculator using logarithms? 73's Richard Clark, KB7QHC Which reminds me, I wanted to start a thread on calculators. tom K0TAR |
Yagi efficiency
Tom Ring wrote:
SNIPPED Which reminds me, I wanted to start a thread on calculators. tom K0TAR Calculator: definition - One person with one brain, one pencil, one piece of paper, and knowledge of math [Oh my gosh! I'll have to spend time learning something. Does that mean I'll have to study to get a license?] |
Yagi efficiency
art wrote:
Dan, you know quite well what the post that started this thread asked for. I only added the TOA comments to fill in some body where I was coming from not for advice on what antenna to build. People are quibling over the word "efficiency" which I find rather wierd especially since I am supposed to be in the company of fellow engineers. Interesting Art, you find that weird, and I find it as an explanation! 8^) - 73 de Mike KB3EIA - |
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