Can I build a radio telescope out of a parabolic TV satellite dish?

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I have the possibility to buy a very inexpensive 2.4m parabolic satellite dish and I would like to build a radio telescope from it. Originally this dish was designed to be a satellite TV antenna.



Can I replace the TV LNB with radio receiver tuned for 1420MHz (hydrogen lines) and use the dish as radio telescope? Does the focal length of such an antenna depend on the frequency for which it was designed?







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  • 1




    You'll find pictures of a (much smaller!) parabolic dish radioastronomy project on ccera.ca
    – Marcus Müller
    Aug 8 at 11:19










  • FYI, I just searched for radio telescope here. There are many other SE sites that discuss them. Since I pondered building one decades ago, it appears that SDRs enrich the experience.
    – Mike Waters♦
    Aug 8 at 16:57










  • Oh, I just also found out they have moved and installed so much more cool stuff over at CCERA :) gotta take time to check out their website!
    – Marcus Müller
    Aug 9 at 8:25














up vote
17
down vote

favorite
1












I have the possibility to buy a very inexpensive 2.4m parabolic satellite dish and I would like to build a radio telescope from it. Originally this dish was designed to be a satellite TV antenna.



Can I replace the TV LNB with radio receiver tuned for 1420MHz (hydrogen lines) and use the dish as radio telescope? Does the focal length of such an antenna depend on the frequency for which it was designed?







share|improve this question


















  • 1




    You'll find pictures of a (much smaller!) parabolic dish radioastronomy project on ccera.ca
    – Marcus Müller
    Aug 8 at 11:19










  • FYI, I just searched for radio telescope here. There are many other SE sites that discuss them. Since I pondered building one decades ago, it appears that SDRs enrich the experience.
    – Mike Waters♦
    Aug 8 at 16:57










  • Oh, I just also found out they have moved and installed so much more cool stuff over at CCERA :) gotta take time to check out their website!
    – Marcus Müller
    Aug 9 at 8:25












up vote
17
down vote

favorite
1









up vote
17
down vote

favorite
1






1





I have the possibility to buy a very inexpensive 2.4m parabolic satellite dish and I would like to build a radio telescope from it. Originally this dish was designed to be a satellite TV antenna.



Can I replace the TV LNB with radio receiver tuned for 1420MHz (hydrogen lines) and use the dish as radio telescope? Does the focal length of such an antenna depend on the frequency for which it was designed?







share|improve this question














I have the possibility to buy a very inexpensive 2.4m parabolic satellite dish and I would like to build a radio telescope from it. Originally this dish was designed to be a satellite TV antenna.



Can I replace the TV LNB with radio receiver tuned for 1420MHz (hydrogen lines) and use the dish as radio telescope? Does the focal length of such an antenna depend on the frequency for which it was designed?









share|improve this question













share|improve this question




share|improve this question








edited Aug 9 at 16:14









Community♦

1




1










asked Aug 8 at 9:21









crooveck

1886




1886







  • 1




    You'll find pictures of a (much smaller!) parabolic dish radioastronomy project on ccera.ca
    – Marcus Müller
    Aug 8 at 11:19










  • FYI, I just searched for radio telescope here. There are many other SE sites that discuss them. Since I pondered building one decades ago, it appears that SDRs enrich the experience.
    – Mike Waters♦
    Aug 8 at 16:57










  • Oh, I just also found out they have moved and installed so much more cool stuff over at CCERA :) gotta take time to check out their website!
    – Marcus Müller
    Aug 9 at 8:25












  • 1




    You'll find pictures of a (much smaller!) parabolic dish radioastronomy project on ccera.ca
    – Marcus Müller
    Aug 8 at 11:19










  • FYI, I just searched for radio telescope here. There are many other SE sites that discuss them. Since I pondered building one decades ago, it appears that SDRs enrich the experience.
    – Mike Waters♦
    Aug 8 at 16:57










  • Oh, I just also found out they have moved and installed so much more cool stuff over at CCERA :) gotta take time to check out their website!
    – Marcus Müller
    Aug 9 at 8:25







1




1




You'll find pictures of a (much smaller!) parabolic dish radioastronomy project on ccera.ca
– Marcus Müller
Aug 8 at 11:19




You'll find pictures of a (much smaller!) parabolic dish radioastronomy project on ccera.ca
– Marcus Müller
Aug 8 at 11:19












FYI, I just searched for radio telescope here. There are many other SE sites that discuss them. Since I pondered building one decades ago, it appears that SDRs enrich the experience.
– Mike Waters♦
Aug 8 at 16:57




FYI, I just searched for radio telescope here. There are many other SE sites that discuss them. Since I pondered building one decades ago, it appears that SDRs enrich the experience.
– Mike Waters♦
Aug 8 at 16:57












Oh, I just also found out they have moved and installed so much more cool stuff over at CCERA :) gotta take time to check out their website!
– Marcus Müller
Aug 9 at 8:25




Oh, I just also found out they have moved and installed so much more cool stuff over at CCERA :) gotta take time to check out their website!
– Marcus Müller
Aug 9 at 8:25










3 Answers
3






active

oldest

votes

















up vote
15
down vote



accepted










The primary factor to consider is the directivity of the parabolic antenna. It is given as:



$$d=frac(pi D)^2lambda^2 tag 1$$



where D is the diameter of the dish and $lambda$ is the wavelength of operation, both in the same units.



To convert frequency to wavelength in meters, we use:



$$lambda=frac300f tag 2$$



where f is the frequency in megahertz.



Since your frequency of interest is 1420 MHz, we apply formula 2 to convert this to a wavelength of 0.211 meters. With a dish diameter of 2.5 meters, formula 1 give us a directivity of:



$$d=frac(pi D)^2lambda^2=frac(pi 2.5)^20.211^2=1386$$



We now need to convert this directivity to linear gain. Here the standard antenna formula applies:



$$G=d*e tag 3$$



where d is the directivity from formula 1 and e is unitless efficiency with a value of 1 indicating 100% efficiency.



Most parabolic antennas have efficiencies in the 60% to 70% range. For a conservative estimate, if we assume a 50% efficiency, the linear gain of your parabolic antenna is 693. We can convert this to dBi gain using:



$$G_dBi=10log_10(G) tag 4$$



which nets ~28 dBi in this case.



With diligence, you may be able to obtain a 70% efficiency which will raise the gain to ~30 dBi.



The beamwidth of the parabolic antenna is given as:



$$thetaapproxfrac70lambdaD tag 5$$



The 3 dB beamwidth of your parabolic antenna will therefore be ~6°.



The focal point of a parabolic antenna is given as:



$$f=fracD^216c tag 6$$



where c is the depth of the parabolic reflector.



You can see from this formula, that it is not a function of wavelength. So the focal point of the dish remains largely the same regardless of frequency.



You now must consider the sensitivity and noise of your receive system and the expected field strength of a 1420 MHz hydrogen marker to determine if this is sufficient gain for your radio telescope operation. There is hope for success as several university students have used a similar configuration for their projects.






share|improve this answer





























    up vote
    4
    down vote













    It's been done before. The University of Groningen astronomy department runs (ran?) a couple of 2.5 m dishes for radio astronomy exercises. IIRC they mainly observe our Sun (strongest radio source).

    So I'd say yes, that dish could be a good starting point.






    share|improve this answer



























      up vote
      1
      down vote













      Yes, although not a very big one.



      The wavelength at 1420 MHz is 21.11 cm. Thus the aperture of this telescope is roughly:



      $$ 240:mathrmcm over 21.11:mathrmcm = 11.4 textwavelengths $$



      (Probably somewhat less, considering inefficiencies.)



      For comparison, the wavelength of green light is around 500 nm. So in terms of the ability to resolve features, this 2.4 meter radio telescope is roughly equivalent to an optical telescope with an objective of a miniscule:



      $$ 0.00005:mathrmcm cdot 11.4 = 0.00057 :mathrmcm $$



      Alternately, the -3 dB beamwidth of a 2.4 meter dish at 1420 MHz is approximately 6 degrees. Meaning, 3 degrees any direction away from the axis of maximum gain, the sensitivity of the antenna has diminished by half. With such a wide beam, you will be limited to observing only very large astronomical features.






      share|improve this answer




















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        3 Answers
        3






        active

        oldest

        votes








        3 Answers
        3






        active

        oldest

        votes









        active

        oldest

        votes






        active

        oldest

        votes








        up vote
        15
        down vote



        accepted










        The primary factor to consider is the directivity of the parabolic antenna. It is given as:



        $$d=frac(pi D)^2lambda^2 tag 1$$



        where D is the diameter of the dish and $lambda$ is the wavelength of operation, both in the same units.



        To convert frequency to wavelength in meters, we use:



        $$lambda=frac300f tag 2$$



        where f is the frequency in megahertz.



        Since your frequency of interest is 1420 MHz, we apply formula 2 to convert this to a wavelength of 0.211 meters. With a dish diameter of 2.5 meters, formula 1 give us a directivity of:



        $$d=frac(pi D)^2lambda^2=frac(pi 2.5)^20.211^2=1386$$



        We now need to convert this directivity to linear gain. Here the standard antenna formula applies:



        $$G=d*e tag 3$$



        where d is the directivity from formula 1 and e is unitless efficiency with a value of 1 indicating 100% efficiency.



        Most parabolic antennas have efficiencies in the 60% to 70% range. For a conservative estimate, if we assume a 50% efficiency, the linear gain of your parabolic antenna is 693. We can convert this to dBi gain using:



        $$G_dBi=10log_10(G) tag 4$$



        which nets ~28 dBi in this case.



        With diligence, you may be able to obtain a 70% efficiency which will raise the gain to ~30 dBi.



        The beamwidth of the parabolic antenna is given as:



        $$thetaapproxfrac70lambdaD tag 5$$



        The 3 dB beamwidth of your parabolic antenna will therefore be ~6°.



        The focal point of a parabolic antenna is given as:



        $$f=fracD^216c tag 6$$



        where c is the depth of the parabolic reflector.



        You can see from this formula, that it is not a function of wavelength. So the focal point of the dish remains largely the same regardless of frequency.



        You now must consider the sensitivity and noise of your receive system and the expected field strength of a 1420 MHz hydrogen marker to determine if this is sufficient gain for your radio telescope operation. There is hope for success as several university students have used a similar configuration for their projects.






        share|improve this answer


























          up vote
          15
          down vote



          accepted










          The primary factor to consider is the directivity of the parabolic antenna. It is given as:



          $$d=frac(pi D)^2lambda^2 tag 1$$



          where D is the diameter of the dish and $lambda$ is the wavelength of operation, both in the same units.



          To convert frequency to wavelength in meters, we use:



          $$lambda=frac300f tag 2$$



          where f is the frequency in megahertz.



          Since your frequency of interest is 1420 MHz, we apply formula 2 to convert this to a wavelength of 0.211 meters. With a dish diameter of 2.5 meters, formula 1 give us a directivity of:



          $$d=frac(pi D)^2lambda^2=frac(pi 2.5)^20.211^2=1386$$



          We now need to convert this directivity to linear gain. Here the standard antenna formula applies:



          $$G=d*e tag 3$$



          where d is the directivity from formula 1 and e is unitless efficiency with a value of 1 indicating 100% efficiency.



          Most parabolic antennas have efficiencies in the 60% to 70% range. For a conservative estimate, if we assume a 50% efficiency, the linear gain of your parabolic antenna is 693. We can convert this to dBi gain using:



          $$G_dBi=10log_10(G) tag 4$$



          which nets ~28 dBi in this case.



          With diligence, you may be able to obtain a 70% efficiency which will raise the gain to ~30 dBi.



          The beamwidth of the parabolic antenna is given as:



          $$thetaapproxfrac70lambdaD tag 5$$



          The 3 dB beamwidth of your parabolic antenna will therefore be ~6°.



          The focal point of a parabolic antenna is given as:



          $$f=fracD^216c tag 6$$



          where c is the depth of the parabolic reflector.



          You can see from this formula, that it is not a function of wavelength. So the focal point of the dish remains largely the same regardless of frequency.



          You now must consider the sensitivity and noise of your receive system and the expected field strength of a 1420 MHz hydrogen marker to determine if this is sufficient gain for your radio telescope operation. There is hope for success as several university students have used a similar configuration for their projects.






          share|improve this answer
























            up vote
            15
            down vote



            accepted







            up vote
            15
            down vote



            accepted






            The primary factor to consider is the directivity of the parabolic antenna. It is given as:



            $$d=frac(pi D)^2lambda^2 tag 1$$



            where D is the diameter of the dish and $lambda$ is the wavelength of operation, both in the same units.



            To convert frequency to wavelength in meters, we use:



            $$lambda=frac300f tag 2$$



            where f is the frequency in megahertz.



            Since your frequency of interest is 1420 MHz, we apply formula 2 to convert this to a wavelength of 0.211 meters. With a dish diameter of 2.5 meters, formula 1 give us a directivity of:



            $$d=frac(pi D)^2lambda^2=frac(pi 2.5)^20.211^2=1386$$



            We now need to convert this directivity to linear gain. Here the standard antenna formula applies:



            $$G=d*e tag 3$$



            where d is the directivity from formula 1 and e is unitless efficiency with a value of 1 indicating 100% efficiency.



            Most parabolic antennas have efficiencies in the 60% to 70% range. For a conservative estimate, if we assume a 50% efficiency, the linear gain of your parabolic antenna is 693. We can convert this to dBi gain using:



            $$G_dBi=10log_10(G) tag 4$$



            which nets ~28 dBi in this case.



            With diligence, you may be able to obtain a 70% efficiency which will raise the gain to ~30 dBi.



            The beamwidth of the parabolic antenna is given as:



            $$thetaapproxfrac70lambdaD tag 5$$



            The 3 dB beamwidth of your parabolic antenna will therefore be ~6°.



            The focal point of a parabolic antenna is given as:



            $$f=fracD^216c tag 6$$



            where c is the depth of the parabolic reflector.



            You can see from this formula, that it is not a function of wavelength. So the focal point of the dish remains largely the same regardless of frequency.



            You now must consider the sensitivity and noise of your receive system and the expected field strength of a 1420 MHz hydrogen marker to determine if this is sufficient gain for your radio telescope operation. There is hope for success as several university students have used a similar configuration for their projects.






            share|improve this answer














            The primary factor to consider is the directivity of the parabolic antenna. It is given as:



            $$d=frac(pi D)^2lambda^2 tag 1$$



            where D is the diameter of the dish and $lambda$ is the wavelength of operation, both in the same units.



            To convert frequency to wavelength in meters, we use:



            $$lambda=frac300f tag 2$$



            where f is the frequency in megahertz.



            Since your frequency of interest is 1420 MHz, we apply formula 2 to convert this to a wavelength of 0.211 meters. With a dish diameter of 2.5 meters, formula 1 give us a directivity of:



            $$d=frac(pi D)^2lambda^2=frac(pi 2.5)^20.211^2=1386$$



            We now need to convert this directivity to linear gain. Here the standard antenna formula applies:



            $$G=d*e tag 3$$



            where d is the directivity from formula 1 and e is unitless efficiency with a value of 1 indicating 100% efficiency.



            Most parabolic antennas have efficiencies in the 60% to 70% range. For a conservative estimate, if we assume a 50% efficiency, the linear gain of your parabolic antenna is 693. We can convert this to dBi gain using:



            $$G_dBi=10log_10(G) tag 4$$



            which nets ~28 dBi in this case.



            With diligence, you may be able to obtain a 70% efficiency which will raise the gain to ~30 dBi.



            The beamwidth of the parabolic antenna is given as:



            $$thetaapproxfrac70lambdaD tag 5$$



            The 3 dB beamwidth of your parabolic antenna will therefore be ~6°.



            The focal point of a parabolic antenna is given as:



            $$f=fracD^216c tag 6$$



            where c is the depth of the parabolic reflector.



            You can see from this formula, that it is not a function of wavelength. So the focal point of the dish remains largely the same regardless of frequency.



            You now must consider the sensitivity and noise of your receive system and the expected field strength of a 1420 MHz hydrogen marker to determine if this is sufficient gain for your radio telescope operation. There is hope for success as several university students have used a similar configuration for their projects.







            share|improve this answer














            share|improve this answer



            share|improve this answer








            edited Aug 9 at 16:07

























            answered Aug 8 at 10:10









            Glenn W9IQ

            11.4k1738




            11.4k1738




















                up vote
                4
                down vote













                It's been done before. The University of Groningen astronomy department runs (ran?) a couple of 2.5 m dishes for radio astronomy exercises. IIRC they mainly observe our Sun (strongest radio source).

                So I'd say yes, that dish could be a good starting point.






                share|improve this answer
























                  up vote
                  4
                  down vote













                  It's been done before. The University of Groningen astronomy department runs (ran?) a couple of 2.5 m dishes for radio astronomy exercises. IIRC they mainly observe our Sun (strongest radio source).

                  So I'd say yes, that dish could be a good starting point.






                  share|improve this answer






















                    up vote
                    4
                    down vote










                    up vote
                    4
                    down vote









                    It's been done before. The University of Groningen astronomy department runs (ran?) a couple of 2.5 m dishes for radio astronomy exercises. IIRC they mainly observe our Sun (strongest radio source).

                    So I'd say yes, that dish could be a good starting point.






                    share|improve this answer












                    It's been done before. The University of Groningen astronomy department runs (ran?) a couple of 2.5 m dishes for radio astronomy exercises. IIRC they mainly observe our Sun (strongest radio source).

                    So I'd say yes, that dish could be a good starting point.







                    share|improve this answer












                    share|improve this answer



                    share|improve this answer










                    answered Aug 8 at 19:02









                    Hobbes

                    1411




                    1411




















                        up vote
                        1
                        down vote













                        Yes, although not a very big one.



                        The wavelength at 1420 MHz is 21.11 cm. Thus the aperture of this telescope is roughly:



                        $$ 240:mathrmcm over 21.11:mathrmcm = 11.4 textwavelengths $$



                        (Probably somewhat less, considering inefficiencies.)



                        For comparison, the wavelength of green light is around 500 nm. So in terms of the ability to resolve features, this 2.4 meter radio telescope is roughly equivalent to an optical telescope with an objective of a miniscule:



                        $$ 0.00005:mathrmcm cdot 11.4 = 0.00057 :mathrmcm $$



                        Alternately, the -3 dB beamwidth of a 2.4 meter dish at 1420 MHz is approximately 6 degrees. Meaning, 3 degrees any direction away from the axis of maximum gain, the sensitivity of the antenna has diminished by half. With such a wide beam, you will be limited to observing only very large astronomical features.






                        share|improve this answer
























                          up vote
                          1
                          down vote













                          Yes, although not a very big one.



                          The wavelength at 1420 MHz is 21.11 cm. Thus the aperture of this telescope is roughly:



                          $$ 240:mathrmcm over 21.11:mathrmcm = 11.4 textwavelengths $$



                          (Probably somewhat less, considering inefficiencies.)



                          For comparison, the wavelength of green light is around 500 nm. So in terms of the ability to resolve features, this 2.4 meter radio telescope is roughly equivalent to an optical telescope with an objective of a miniscule:



                          $$ 0.00005:mathrmcm cdot 11.4 = 0.00057 :mathrmcm $$



                          Alternately, the -3 dB beamwidth of a 2.4 meter dish at 1420 MHz is approximately 6 degrees. Meaning, 3 degrees any direction away from the axis of maximum gain, the sensitivity of the antenna has diminished by half. With such a wide beam, you will be limited to observing only very large astronomical features.






                          share|improve this answer






















                            up vote
                            1
                            down vote










                            up vote
                            1
                            down vote









                            Yes, although not a very big one.



                            The wavelength at 1420 MHz is 21.11 cm. Thus the aperture of this telescope is roughly:



                            $$ 240:mathrmcm over 21.11:mathrmcm = 11.4 textwavelengths $$



                            (Probably somewhat less, considering inefficiencies.)



                            For comparison, the wavelength of green light is around 500 nm. So in terms of the ability to resolve features, this 2.4 meter radio telescope is roughly equivalent to an optical telescope with an objective of a miniscule:



                            $$ 0.00005:mathrmcm cdot 11.4 = 0.00057 :mathrmcm $$



                            Alternately, the -3 dB beamwidth of a 2.4 meter dish at 1420 MHz is approximately 6 degrees. Meaning, 3 degrees any direction away from the axis of maximum gain, the sensitivity of the antenna has diminished by half. With such a wide beam, you will be limited to observing only very large astronomical features.






                            share|improve this answer












                            Yes, although not a very big one.



                            The wavelength at 1420 MHz is 21.11 cm. Thus the aperture of this telescope is roughly:



                            $$ 240:mathrmcm over 21.11:mathrmcm = 11.4 textwavelengths $$



                            (Probably somewhat less, considering inefficiencies.)



                            For comparison, the wavelength of green light is around 500 nm. So in terms of the ability to resolve features, this 2.4 meter radio telescope is roughly equivalent to an optical telescope with an objective of a miniscule:



                            $$ 0.00005:mathrmcm cdot 11.4 = 0.00057 :mathrmcm $$



                            Alternately, the -3 dB beamwidth of a 2.4 meter dish at 1420 MHz is approximately 6 degrees. Meaning, 3 degrees any direction away from the axis of maximum gain, the sensitivity of the antenna has diminished by half. With such a wide beam, you will be limited to observing only very large astronomical features.







                            share|improve this answer












                            share|improve this answer



                            share|improve this answer










                            answered Aug 9 at 12:52









                            Phil Frost - W8II

                            24.9k140112




                            24.9k140112



























                                 

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