Why do lower pitched string instruments have a larger body?











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I know that increasing the length of the string will decrease the pitch, but that doesn't explain why the body of a cello is larger than a violin, only longer.



What would be the "problem" with having a violin with a really long neck so it's the length of cello, and putting cello strings on it.



Is there some physical issue with trying to achieve a low pitch in a small resonating body (or visa versa)?










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    up vote
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    down vote

    favorite












    I know that increasing the length of the string will decrease the pitch, but that doesn't explain why the body of a cello is larger than a violin, only longer.



    What would be the "problem" with having a violin with a really long neck so it's the length of cello, and putting cello strings on it.



    Is there some physical issue with trying to achieve a low pitch in a small resonating body (or visa versa)?










    share|improve this question







    New contributor




    nanotek is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
    Check out our Code of Conduct.






















      up vote
      13
      down vote

      favorite









      up vote
      13
      down vote

      favorite











      I know that increasing the length of the string will decrease the pitch, but that doesn't explain why the body of a cello is larger than a violin, only longer.



      What would be the "problem" with having a violin with a really long neck so it's the length of cello, and putting cello strings on it.



      Is there some physical issue with trying to achieve a low pitch in a small resonating body (or visa versa)?










      share|improve this question







      New contributor




      nanotek is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
      Check out our Code of Conduct.











      I know that increasing the length of the string will decrease the pitch, but that doesn't explain why the body of a cello is larger than a violin, only longer.



      What would be the "problem" with having a violin with a really long neck so it's the length of cello, and putting cello strings on it.



      Is there some physical issue with trying to achieve a low pitch in a small resonating body (or visa versa)?







      theory learning strings instruments string-instruments






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      nanotek is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
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      nanotek

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          Some of the answers seem to be saying that you want the body to resonate at the frequency of the sound so as to produce the maximum amplitude of sound. That's not quite right. The graph below shows a measurement of the resonance curve of a 1713 Stradivarius violin (redrawn by me from a figure by Carleen Hutchins). There are a number of different resonance peaks, some strong and some weak; the ones near 200 and 400 Hz are vibrations of the wood, and the one near 300 Hz is a resonance of the air moving in and out through the f-holes. The white lines show the fundamental frequencies of the four strings.



          resonance curve of a Stradivarius violin



          So you can see that there certainly are peaks, which indicate resonances, but they're rather narrow and there are a lot of them. From what little I understand of violin acoustics, the effect on the sound is complicated, and has to do with the way the different harmonics coincide with the many different resonances. When you play with vibrato, you're sliding the harmonics back and forth over these resonance peaks. In any case, this is definitely not a situation where the fundamental frequency of the note simply matches the resonance frequency of the body and/or air cavity.



          The OP specifically asks:




          Why do lower pitched string instruments have a larger body?




          In other words, why can't we have a double bass with a soundboard the size of a violin? The answer really has less to do with resonance of the body than with the size of the body in relation to the size of the sound waves. Each of the resonance peaks in the graph above corresponds to some pattern of vibration of the soundboard. Below are some diagrams from WP of the patterns of vibration of a guitar's soundboard.



          Chladni figures for a guitar



          The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling. That is, different parts of the soundboard have different phases. Now the lowest note you can play on a double bass is 41 Hz, which corresponds to a wavelength of 800 cm. Suppose you tried to produce this sound using a soundboard the size of a violin, where the different vibrating patches were only 5-10 cm in size. Then for any patch that was vibrating outward, trying to produce an overpressure in the air, there would be another patch right nearby that was simultaneously vibrating inward, trying to produce an underpressure. They not cooperating. They will come very close to canceling out.



          Let's refer to the patch that's trying to produce an overpressure as +, and the other as -. Ideally you would like the the + patch and the - patch to be 400 cm apart. This would be half a wavelength, and then the + and - would actually be cooperating on producing the same 800 cm sine wave: one would be producing the crest, while the other produced the trough.



          In reality, the size of a double bass's soundboard is somewhere in between these two extremes. Because it's pretty small compared to most of the wavelengths it plays, there is a lot of cancellation going on, and not much cooperation. However, the cancellation is not perfect, so you do get some sound. The instrument could be made louder by making it bigger, but that would be impractical.






          share|improve this answer























          • “The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling” – I'd agree for a guitar, but in the bowed string instruments, the lowest body mode is indeed when most of the top moves consistently in phase with the side of the bridge under which the bass bar sits. What moves with the opposite phase is the bottom of the body, because it's coupled to the other side of the bridge via the sound post. The figures you're showing, whilst interesting, are at any rate not very relevant (though the basic principle you're discussing is).
            – leftaroundabout
            3 hours ago












          • @leftaroundabout: Interesting, thanks. It's clear that you know a lot more about violin acoustics than I do. I'm not totally succeeding in visualizing what you're describing, but if you think you could improve this answer with some edits, that would be great.
            – Ben Crowell
            2 hours ago


















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          The lower the sound the instrument is producing, the larger the vibrating plate needs to be to produce that sound. The vibrations from the strings are being transferred to to the face of the instrument by the bridge, and the face of the instrument vibrates in response, making the air move, producing the waves that we hear as sound.



          The larger face plate also increases the volume of the lower sound. If you had a cello with a violin sized body, you wouldn't hear the instrument very well, and the low notes would sound very "weak" and "thin".



          EDIT:



          Scott's comment has enough votes to stay visible, but I'm quoting it in the answer to make sure:



          QUOTE: "Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz. – Scott Wallace " :QUOTE



          As another example, an imperfect analogy would be the game of skip-rope, where two people swing a rope between them so someone may jump the rope. A very long rope requires more energy to swing and makes a slower and larger rotation, where a short rope can be swung more quickly.



          The depth of the instrument body also helps reinforce the reproduction of lower frequencies due to resonance. Low frequency resonance occurs with the coupled motion of the top plate, the back plate and the enclosed air, so for good low frequency resonance, the cello body needs to be deep as well as large.






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          • 8




            Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz.
            – Scott Wallace
            14 hours ago






          • 2




            You should incorporate @ScottWallace comment into your answer. As it stands, you have pretty much written a tautology. The whole point is that you can't produce a note of X wavelength with a body less than (at best) X/2 dimension.
            – Carl Witthoft
            14 hours ago










          • @CarlWitthoft Yes, this was my late-at-night-just-before-bed answer, and I was looking for a good link to the physics of vibrating plates. I'll edit to include more info.
            – Alphonso Balvenie
            6 hours ago


















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          Just to complement Alphonso's answer: the lower the pitch, the lower the frequency. The lower the frequency, the larger the wavelength. Surfaces respond better to waves, when their wavelength is close to the size of the surface.



          Imagine you try to shake a sheet of paper, by holding it vertically. There is a minimum frequency you need to apply to make it undulate. Now, if you try to apply this same frequency to a post-it, it won't shake, just move along with your hand. To make it undulate you would need to shake it much faster (higher frequency, smaller wavelength), because the post-it is smaller then a sheet of paper. Also, if you take a meter long sheet of paper and shake it that fast, it won't undulate a lot too. You would probably see the waves fading out through the paper, while it's other end barely moves. There is of course a lower frequency that would make it undulate entirely.



          Instruments function in a similar way. The string has to shake the body, to produce a louder sound, and therefore the body size must minimally match the wavelength of the sound waves you want to produce.






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          • 3




            +1 Love the sheet of paper visual!
            – David K
            10 hours ago


















          up vote
          3
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          While each answer explains the physical properties and their relationship to the pitches being produced by the instrument, I'm inclined to add the aspect of the volume of air contained inside the instrument that resonates to amplify the sound the strings are producing. Larger volumes of air will resonate at lower pitches and increase the level of the sound being produced by the strings. The notes on a violin only require a sound box internal volume to resonate at a relatively high pitch, whereas a cello or bass needs a considerably larger sound box that will resonate at lower pitches in order to effectively amplify the sound being produced.






          share|improve this answer




























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            You are only partly correct. For a given tension a string's fundamental resonant frequency scales with length. However, to within mechanical and material limits, you can increase or decrease tension on a fixed-length string to achieve any resonant frequency desired.



            The string on a musical instrument is analogous to the oscillator in an electronic audio generator: it produces the source frequency(ies). The bridge and body of the instrument are analogous to the amplifier, transferring the energy from the string to the atmosphere with (one hopes!) minimal impedance mismatch (and yes, there is such a thing as acoustic impedance in air) so as to maximize the sound volume.






            share|improve this answer

















            • 1




              It may be good to amplify "within mechanical and material limits" to note that for a cello-length string to reach the pitch of a violin's (high) E string would require that it be thinner and/or tighter than practical, and for a violin-length string to reach the pitch of a cello's (low) C string would require that it be thicker and/or looser than practical.
              – supercat
              8 hours ago






            • 1




              @supercat I'm a physicist. I make my strings out of unobtanium.
              – Carl Witthoft
              7 hours ago











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            5 Answers
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            up vote
            3
            down vote



            accepted










            Some of the answers seem to be saying that you want the body to resonate at the frequency of the sound so as to produce the maximum amplitude of sound. That's not quite right. The graph below shows a measurement of the resonance curve of a 1713 Stradivarius violin (redrawn by me from a figure by Carleen Hutchins). There are a number of different resonance peaks, some strong and some weak; the ones near 200 and 400 Hz are vibrations of the wood, and the one near 300 Hz is a resonance of the air moving in and out through the f-holes. The white lines show the fundamental frequencies of the four strings.



            resonance curve of a Stradivarius violin



            So you can see that there certainly are peaks, which indicate resonances, but they're rather narrow and there are a lot of them. From what little I understand of violin acoustics, the effect on the sound is complicated, and has to do with the way the different harmonics coincide with the many different resonances. When you play with vibrato, you're sliding the harmonics back and forth over these resonance peaks. In any case, this is definitely not a situation where the fundamental frequency of the note simply matches the resonance frequency of the body and/or air cavity.



            The OP specifically asks:




            Why do lower pitched string instruments have a larger body?




            In other words, why can't we have a double bass with a soundboard the size of a violin? The answer really has less to do with resonance of the body than with the size of the body in relation to the size of the sound waves. Each of the resonance peaks in the graph above corresponds to some pattern of vibration of the soundboard. Below are some diagrams from WP of the patterns of vibration of a guitar's soundboard.



            Chladni figures for a guitar



            The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling. That is, different parts of the soundboard have different phases. Now the lowest note you can play on a double bass is 41 Hz, which corresponds to a wavelength of 800 cm. Suppose you tried to produce this sound using a soundboard the size of a violin, where the different vibrating patches were only 5-10 cm in size. Then for any patch that was vibrating outward, trying to produce an overpressure in the air, there would be another patch right nearby that was simultaneously vibrating inward, trying to produce an underpressure. They not cooperating. They will come very close to canceling out.



            Let's refer to the patch that's trying to produce an overpressure as +, and the other as -. Ideally you would like the the + patch and the - patch to be 400 cm apart. This would be half a wavelength, and then the + and - would actually be cooperating on producing the same 800 cm sine wave: one would be producing the crest, while the other produced the trough.



            In reality, the size of a double bass's soundboard is somewhere in between these two extremes. Because it's pretty small compared to most of the wavelengths it plays, there is a lot of cancellation going on, and not much cooperation. However, the cancellation is not perfect, so you do get some sound. The instrument could be made louder by making it bigger, but that would be impractical.






            share|improve this answer























            • “The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling” – I'd agree for a guitar, but in the bowed string instruments, the lowest body mode is indeed when most of the top moves consistently in phase with the side of the bridge under which the bass bar sits. What moves with the opposite phase is the bottom of the body, because it's coupled to the other side of the bridge via the sound post. The figures you're showing, whilst interesting, are at any rate not very relevant (though the basic principle you're discussing is).
              – leftaroundabout
              3 hours ago












            • @leftaroundabout: Interesting, thanks. It's clear that you know a lot more about violin acoustics than I do. I'm not totally succeeding in visualizing what you're describing, but if you think you could improve this answer with some edits, that would be great.
              – Ben Crowell
              2 hours ago















            up vote
            3
            down vote



            accepted










            Some of the answers seem to be saying that you want the body to resonate at the frequency of the sound so as to produce the maximum amplitude of sound. That's not quite right. The graph below shows a measurement of the resonance curve of a 1713 Stradivarius violin (redrawn by me from a figure by Carleen Hutchins). There are a number of different resonance peaks, some strong and some weak; the ones near 200 and 400 Hz are vibrations of the wood, and the one near 300 Hz is a resonance of the air moving in and out through the f-holes. The white lines show the fundamental frequencies of the four strings.



            resonance curve of a Stradivarius violin



            So you can see that there certainly are peaks, which indicate resonances, but they're rather narrow and there are a lot of them. From what little I understand of violin acoustics, the effect on the sound is complicated, and has to do with the way the different harmonics coincide with the many different resonances. When you play with vibrato, you're sliding the harmonics back and forth over these resonance peaks. In any case, this is definitely not a situation where the fundamental frequency of the note simply matches the resonance frequency of the body and/or air cavity.



            The OP specifically asks:




            Why do lower pitched string instruments have a larger body?




            In other words, why can't we have a double bass with a soundboard the size of a violin? The answer really has less to do with resonance of the body than with the size of the body in relation to the size of the sound waves. Each of the resonance peaks in the graph above corresponds to some pattern of vibration of the soundboard. Below are some diagrams from WP of the patterns of vibration of a guitar's soundboard.



            Chladni figures for a guitar



            The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling. That is, different parts of the soundboard have different phases. Now the lowest note you can play on a double bass is 41 Hz, which corresponds to a wavelength of 800 cm. Suppose you tried to produce this sound using a soundboard the size of a violin, where the different vibrating patches were only 5-10 cm in size. Then for any patch that was vibrating outward, trying to produce an overpressure in the air, there would be another patch right nearby that was simultaneously vibrating inward, trying to produce an underpressure. They not cooperating. They will come very close to canceling out.



            Let's refer to the patch that's trying to produce an overpressure as +, and the other as -. Ideally you would like the the + patch and the - patch to be 400 cm apart. This would be half a wavelength, and then the + and - would actually be cooperating on producing the same 800 cm sine wave: one would be producing the crest, while the other produced the trough.



            In reality, the size of a double bass's soundboard is somewhere in between these two extremes. Because it's pretty small compared to most of the wavelengths it plays, there is a lot of cancellation going on, and not much cooperation. However, the cancellation is not perfect, so you do get some sound. The instrument could be made louder by making it bigger, but that would be impractical.






            share|improve this answer























            • “The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling” – I'd agree for a guitar, but in the bowed string instruments, the lowest body mode is indeed when most of the top moves consistently in phase with the side of the bridge under which the bass bar sits. What moves with the opposite phase is the bottom of the body, because it's coupled to the other side of the bridge via the sound post. The figures you're showing, whilst interesting, are at any rate not very relevant (though the basic principle you're discussing is).
              – leftaroundabout
              3 hours ago












            • @leftaroundabout: Interesting, thanks. It's clear that you know a lot more about violin acoustics than I do. I'm not totally succeeding in visualizing what you're describing, but if you think you could improve this answer with some edits, that would be great.
              – Ben Crowell
              2 hours ago













            up vote
            3
            down vote



            accepted







            up vote
            3
            down vote



            accepted






            Some of the answers seem to be saying that you want the body to resonate at the frequency of the sound so as to produce the maximum amplitude of sound. That's not quite right. The graph below shows a measurement of the resonance curve of a 1713 Stradivarius violin (redrawn by me from a figure by Carleen Hutchins). There are a number of different resonance peaks, some strong and some weak; the ones near 200 and 400 Hz are vibrations of the wood, and the one near 300 Hz is a resonance of the air moving in and out through the f-holes. The white lines show the fundamental frequencies of the four strings.



            resonance curve of a Stradivarius violin



            So you can see that there certainly are peaks, which indicate resonances, but they're rather narrow and there are a lot of them. From what little I understand of violin acoustics, the effect on the sound is complicated, and has to do with the way the different harmonics coincide with the many different resonances. When you play with vibrato, you're sliding the harmonics back and forth over these resonance peaks. In any case, this is definitely not a situation where the fundamental frequency of the note simply matches the resonance frequency of the body and/or air cavity.



            The OP specifically asks:




            Why do lower pitched string instruments have a larger body?




            In other words, why can't we have a double bass with a soundboard the size of a violin? The answer really has less to do with resonance of the body than with the size of the body in relation to the size of the sound waves. Each of the resonance peaks in the graph above corresponds to some pattern of vibration of the soundboard. Below are some diagrams from WP of the patterns of vibration of a guitar's soundboard.



            Chladni figures for a guitar



            The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling. That is, different parts of the soundboard have different phases. Now the lowest note you can play on a double bass is 41 Hz, which corresponds to a wavelength of 800 cm. Suppose you tried to produce this sound using a soundboard the size of a violin, where the different vibrating patches were only 5-10 cm in size. Then for any patch that was vibrating outward, trying to produce an overpressure in the air, there would be another patch right nearby that was simultaneously vibrating inward, trying to produce an underpressure. They not cooperating. They will come very close to canceling out.



            Let's refer to the patch that's trying to produce an overpressure as +, and the other as -. Ideally you would like the the + patch and the - patch to be 400 cm apart. This would be half a wavelength, and then the + and - would actually be cooperating on producing the same 800 cm sine wave: one would be producing the crest, while the other produced the trough.



            In reality, the size of a double bass's soundboard is somewhere in between these two extremes. Because it's pretty small compared to most of the wavelengths it plays, there is a lot of cancellation going on, and not much cooperation. However, the cancellation is not perfect, so you do get some sound. The instrument could be made louder by making it bigger, but that would be impractical.






            share|improve this answer














            Some of the answers seem to be saying that you want the body to resonate at the frequency of the sound so as to produce the maximum amplitude of sound. That's not quite right. The graph below shows a measurement of the resonance curve of a 1713 Stradivarius violin (redrawn by me from a figure by Carleen Hutchins). There are a number of different resonance peaks, some strong and some weak; the ones near 200 and 400 Hz are vibrations of the wood, and the one near 300 Hz is a resonance of the air moving in and out through the f-holes. The white lines show the fundamental frequencies of the four strings.



            resonance curve of a Stradivarius violin



            So you can see that there certainly are peaks, which indicate resonances, but they're rather narrow and there are a lot of them. From what little I understand of violin acoustics, the effect on the sound is complicated, and has to do with the way the different harmonics coincide with the many different resonances. When you play with vibrato, you're sliding the harmonics back and forth over these resonance peaks. In any case, this is definitely not a situation where the fundamental frequency of the note simply matches the resonance frequency of the body and/or air cavity.



            The OP specifically asks:




            Why do lower pitched string instruments have a larger body?




            In other words, why can't we have a double bass with a soundboard the size of a violin? The answer really has less to do with resonance of the body than with the size of the body in relation to the size of the sound waves. Each of the resonance peaks in the graph above corresponds to some pattern of vibration of the soundboard. Below are some diagrams from WP of the patterns of vibration of a guitar's soundboard.



            Chladni figures for a guitar



            The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling. That is, different parts of the soundboard have different phases. Now the lowest note you can play on a double bass is 41 Hz, which corresponds to a wavelength of 800 cm. Suppose you tried to produce this sound using a soundboard the size of a violin, where the different vibrating patches were only 5-10 cm in size. Then for any patch that was vibrating outward, trying to produce an overpressure in the air, there would be another patch right nearby that was simultaneously vibrating inward, trying to produce an underpressure. They not cooperating. They will come very close to canceling out.



            Let's refer to the patch that's trying to produce an overpressure as +, and the other as -. Ideally you would like the the + patch and the - patch to be 400 cm apart. This would be half a wavelength, and then the + and - would actually be cooperating on producing the same 800 cm sine wave: one would be producing the crest, while the other produced the trough.



            In reality, the size of a double bass's soundboard is somewhere in between these two extremes. Because it's pretty small compared to most of the wavelengths it plays, there is a lot of cancellation going on, and not much cooperation. However, the cancellation is not perfect, so you do get some sound. The instrument could be made louder by making it bigger, but that would be impractical.







            share|improve this answer














            share|improve this answer



            share|improve this answer








            edited 6 hours ago

























            answered 6 hours ago









            Ben Crowell

            44028




            44028












            • “The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling” – I'd agree for a guitar, but in the bowed string instruments, the lowest body mode is indeed when most of the top moves consistently in phase with the side of the bridge under which the bass bar sits. What moves with the opposite phase is the bottom of the body, because it's coupled to the other side of the bridge via the sound post. The figures you're showing, whilst interesting, are at any rate not very relevant (though the basic principle you're discussing is).
              – leftaroundabout
              3 hours ago












            • @leftaroundabout: Interesting, thanks. It's clear that you know a lot more about violin acoustics than I do. I'm not totally succeeding in visualizing what you're describing, but if you think you could improve this answer with some edits, that would be great.
              – Ben Crowell
              2 hours ago


















            • “The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling” – I'd agree for a guitar, but in the bowed string instruments, the lowest body mode is indeed when most of the top moves consistently in phase with the side of the bridge under which the bass bar sits. What moves with the opposite phase is the bottom of the body, because it's coupled to the other side of the bridge via the sound post. The figures you're showing, whilst interesting, are at any rate not very relevant (though the basic principle you're discussing is).
              – leftaroundabout
              3 hours ago












            • @leftaroundabout: Interesting, thanks. It's clear that you know a lot more about violin acoustics than I do. I'm not totally succeeding in visualizing what you're describing, but if you think you could improve this answer with some edits, that would be great.
              – Ben Crowell
              2 hours ago
















            “The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling” – I'd agree for a guitar, but in the bowed string instruments, the lowest body mode is indeed when most of the top moves consistently in phase with the side of the bridge under which the bass bar sits. What moves with the opposite phase is the bottom of the body, because it's coupled to the other side of the bridge via the sound post. The figures you're showing, whilst interesting, are at any rate not very relevant (though the basic principle you're discussing is).
            – leftaroundabout
            3 hours ago






            “The crucial point here is that in all of these patterns, there are some areas that are rising while others are falling” – I'd agree for a guitar, but in the bowed string instruments, the lowest body mode is indeed when most of the top moves consistently in phase with the side of the bridge under which the bass bar sits. What moves with the opposite phase is the bottom of the body, because it's coupled to the other side of the bridge via the sound post. The figures you're showing, whilst interesting, are at any rate not very relevant (though the basic principle you're discussing is).
            – leftaroundabout
            3 hours ago














            @leftaroundabout: Interesting, thanks. It's clear that you know a lot more about violin acoustics than I do. I'm not totally succeeding in visualizing what you're describing, but if you think you could improve this answer with some edits, that would be great.
            – Ben Crowell
            2 hours ago




            @leftaroundabout: Interesting, thanks. It's clear that you know a lot more about violin acoustics than I do. I'm not totally succeeding in visualizing what you're describing, but if you think you could improve this answer with some edits, that would be great.
            – Ben Crowell
            2 hours ago










            up vote
            11
            down vote













            The lower the sound the instrument is producing, the larger the vibrating plate needs to be to produce that sound. The vibrations from the strings are being transferred to to the face of the instrument by the bridge, and the face of the instrument vibrates in response, making the air move, producing the waves that we hear as sound.



            The larger face plate also increases the volume of the lower sound. If you had a cello with a violin sized body, you wouldn't hear the instrument very well, and the low notes would sound very "weak" and "thin".



            EDIT:



            Scott's comment has enough votes to stay visible, but I'm quoting it in the answer to make sure:



            QUOTE: "Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz. – Scott Wallace " :QUOTE



            As another example, an imperfect analogy would be the game of skip-rope, where two people swing a rope between them so someone may jump the rope. A very long rope requires more energy to swing and makes a slower and larger rotation, where a short rope can be swung more quickly.



            The depth of the instrument body also helps reinforce the reproduction of lower frequencies due to resonance. Low frequency resonance occurs with the coupled motion of the top plate, the back plate and the enclosed air, so for good low frequency resonance, the cello body needs to be deep as well as large.






            share|improve this answer



















            • 8




              Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz.
              – Scott Wallace
              14 hours ago






            • 2




              You should incorporate @ScottWallace comment into your answer. As it stands, you have pretty much written a tautology. The whole point is that you can't produce a note of X wavelength with a body less than (at best) X/2 dimension.
              – Carl Witthoft
              14 hours ago










            • @CarlWitthoft Yes, this was my late-at-night-just-before-bed answer, and I was looking for a good link to the physics of vibrating plates. I'll edit to include more info.
              – Alphonso Balvenie
              6 hours ago















            up vote
            11
            down vote













            The lower the sound the instrument is producing, the larger the vibrating plate needs to be to produce that sound. The vibrations from the strings are being transferred to to the face of the instrument by the bridge, and the face of the instrument vibrates in response, making the air move, producing the waves that we hear as sound.



            The larger face plate also increases the volume of the lower sound. If you had a cello with a violin sized body, you wouldn't hear the instrument very well, and the low notes would sound very "weak" and "thin".



            EDIT:



            Scott's comment has enough votes to stay visible, but I'm quoting it in the answer to make sure:



            QUOTE: "Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz. – Scott Wallace " :QUOTE



            As another example, an imperfect analogy would be the game of skip-rope, where two people swing a rope between them so someone may jump the rope. A very long rope requires more energy to swing and makes a slower and larger rotation, where a short rope can be swung more quickly.



            The depth of the instrument body also helps reinforce the reproduction of lower frequencies due to resonance. Low frequency resonance occurs with the coupled motion of the top plate, the back plate and the enclosed air, so for good low frequency resonance, the cello body needs to be deep as well as large.






            share|improve this answer



















            • 8




              Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz.
              – Scott Wallace
              14 hours ago






            • 2




              You should incorporate @ScottWallace comment into your answer. As it stands, you have pretty much written a tautology. The whole point is that you can't produce a note of X wavelength with a body less than (at best) X/2 dimension.
              – Carl Witthoft
              14 hours ago










            • @CarlWitthoft Yes, this was my late-at-night-just-before-bed answer, and I was looking for a good link to the physics of vibrating plates. I'll edit to include more info.
              – Alphonso Balvenie
              6 hours ago













            up vote
            11
            down vote










            up vote
            11
            down vote









            The lower the sound the instrument is producing, the larger the vibrating plate needs to be to produce that sound. The vibrations from the strings are being transferred to to the face of the instrument by the bridge, and the face of the instrument vibrates in response, making the air move, producing the waves that we hear as sound.



            The larger face plate also increases the volume of the lower sound. If you had a cello with a violin sized body, you wouldn't hear the instrument very well, and the low notes would sound very "weak" and "thin".



            EDIT:



            Scott's comment has enough votes to stay visible, but I'm quoting it in the answer to make sure:



            QUOTE: "Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz. – Scott Wallace " :QUOTE



            As another example, an imperfect analogy would be the game of skip-rope, where two people swing a rope between them so someone may jump the rope. A very long rope requires more energy to swing and makes a slower and larger rotation, where a short rope can be swung more quickly.



            The depth of the instrument body also helps reinforce the reproduction of lower frequencies due to resonance. Low frequency resonance occurs with the coupled motion of the top plate, the back plate and the enclosed air, so for good low frequency resonance, the cello body needs to be deep as well as large.






            share|improve this answer














            The lower the sound the instrument is producing, the larger the vibrating plate needs to be to produce that sound. The vibrations from the strings are being transferred to to the face of the instrument by the bridge, and the face of the instrument vibrates in response, making the air move, producing the waves that we hear as sound.



            The larger face plate also increases the volume of the lower sound. If you had a cello with a violin sized body, you wouldn't hear the instrument very well, and the low notes would sound very "weak" and "thin".



            EDIT:



            Scott's comment has enough votes to stay visible, but I'm quoting it in the answer to make sure:



            QUOTE: "Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz. – Scott Wallace " :QUOTE



            As another example, an imperfect analogy would be the game of skip-rope, where two people swing a rope between them so someone may jump the rope. A very long rope requires more energy to swing and makes a slower and larger rotation, where a short rope can be swung more quickly.



            The depth of the instrument body also helps reinforce the reproduction of lower frequencies due to resonance. Low frequency resonance occurs with the coupled motion of the top plate, the back plate and the enclosed air, so for good low frequency resonance, the cello body needs to be deep as well as large.







            share|improve this answer














            share|improve this answer



            share|improve this answer








            edited 6 hours ago

























            answered 20 hours ago









            Alphonso Balvenie

            4,326617




            4,326617








            • 8




              Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz.
              – Scott Wallace
              14 hours ago






            • 2




              You should incorporate @ScottWallace comment into your answer. As it stands, you have pretty much written a tautology. The whole point is that you can't produce a note of X wavelength with a body less than (at best) X/2 dimension.
              – Carl Witthoft
              14 hours ago










            • @CarlWitthoft Yes, this was my late-at-night-just-before-bed answer, and I was looking for a good link to the physics of vibrating plates. I'll edit to include more info.
              – Alphonso Balvenie
              6 hours ago














            • 8




              Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz.
              – Scott Wallace
              14 hours ago






            • 2




              You should incorporate @ScottWallace comment into your answer. As it stands, you have pretty much written a tautology. The whole point is that you can't produce a note of X wavelength with a body less than (at best) X/2 dimension.
              – Carl Witthoft
              14 hours ago










            • @CarlWitthoft Yes, this was my late-at-night-just-before-bed answer, and I was looking for a good link to the physics of vibrating plates. I'll edit to include more info.
              – Alphonso Balvenie
              6 hours ago








            8




            8




            Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz.
            – Scott Wallace
            14 hours ago




            Yep. I'd just add that as a rule of thumb, to most efficiently get air moving for a particular frequency, the vibrating plate should be at least 1/4 of the wavelength of sound to be produced long. That makes a cello plate about right for viola c = 128 Hz, but only half the desired length for the bottom C at 64 Hz. A violin is way too short to get air moving efficiently at 64 Hz.
            – Scott Wallace
            14 hours ago




            2




            2




            You should incorporate @ScottWallace comment into your answer. As it stands, you have pretty much written a tautology. The whole point is that you can't produce a note of X wavelength with a body less than (at best) X/2 dimension.
            – Carl Witthoft
            14 hours ago




            You should incorporate @ScottWallace comment into your answer. As it stands, you have pretty much written a tautology. The whole point is that you can't produce a note of X wavelength with a body less than (at best) X/2 dimension.
            – Carl Witthoft
            14 hours ago












            @CarlWitthoft Yes, this was my late-at-night-just-before-bed answer, and I was looking for a good link to the physics of vibrating plates. I'll edit to include more info.
            – Alphonso Balvenie
            6 hours ago




            @CarlWitthoft Yes, this was my late-at-night-just-before-bed answer, and I was looking for a good link to the physics of vibrating plates. I'll edit to include more info.
            – Alphonso Balvenie
            6 hours ago










            up vote
            10
            down vote













            Just to complement Alphonso's answer: the lower the pitch, the lower the frequency. The lower the frequency, the larger the wavelength. Surfaces respond better to waves, when their wavelength is close to the size of the surface.



            Imagine you try to shake a sheet of paper, by holding it vertically. There is a minimum frequency you need to apply to make it undulate. Now, if you try to apply this same frequency to a post-it, it won't shake, just move along with your hand. To make it undulate you would need to shake it much faster (higher frequency, smaller wavelength), because the post-it is smaller then a sheet of paper. Also, if you take a meter long sheet of paper and shake it that fast, it won't undulate a lot too. You would probably see the waves fading out through the paper, while it's other end barely moves. There is of course a lower frequency that would make it undulate entirely.



            Instruments function in a similar way. The string has to shake the body, to produce a louder sound, and therefore the body size must minimally match the wavelength of the sound waves you want to produce.






            share|improve this answer

















            • 3




              +1 Love the sheet of paper visual!
              – David K
              10 hours ago















            up vote
            10
            down vote













            Just to complement Alphonso's answer: the lower the pitch, the lower the frequency. The lower the frequency, the larger the wavelength. Surfaces respond better to waves, when their wavelength is close to the size of the surface.



            Imagine you try to shake a sheet of paper, by holding it vertically. There is a minimum frequency you need to apply to make it undulate. Now, if you try to apply this same frequency to a post-it, it won't shake, just move along with your hand. To make it undulate you would need to shake it much faster (higher frequency, smaller wavelength), because the post-it is smaller then a sheet of paper. Also, if you take a meter long sheet of paper and shake it that fast, it won't undulate a lot too. You would probably see the waves fading out through the paper, while it's other end barely moves. There is of course a lower frequency that would make it undulate entirely.



            Instruments function in a similar way. The string has to shake the body, to produce a louder sound, and therefore the body size must minimally match the wavelength of the sound waves you want to produce.






            share|improve this answer

















            • 3




              +1 Love the sheet of paper visual!
              – David K
              10 hours ago













            up vote
            10
            down vote










            up vote
            10
            down vote









            Just to complement Alphonso's answer: the lower the pitch, the lower the frequency. The lower the frequency, the larger the wavelength. Surfaces respond better to waves, when their wavelength is close to the size of the surface.



            Imagine you try to shake a sheet of paper, by holding it vertically. There is a minimum frequency you need to apply to make it undulate. Now, if you try to apply this same frequency to a post-it, it won't shake, just move along with your hand. To make it undulate you would need to shake it much faster (higher frequency, smaller wavelength), because the post-it is smaller then a sheet of paper. Also, if you take a meter long sheet of paper and shake it that fast, it won't undulate a lot too. You would probably see the waves fading out through the paper, while it's other end barely moves. There is of course a lower frequency that would make it undulate entirely.



            Instruments function in a similar way. The string has to shake the body, to produce a louder sound, and therefore the body size must minimally match the wavelength of the sound waves you want to produce.






            share|improve this answer












            Just to complement Alphonso's answer: the lower the pitch, the lower the frequency. The lower the frequency, the larger the wavelength. Surfaces respond better to waves, when their wavelength is close to the size of the surface.



            Imagine you try to shake a sheet of paper, by holding it vertically. There is a minimum frequency you need to apply to make it undulate. Now, if you try to apply this same frequency to a post-it, it won't shake, just move along with your hand. To make it undulate you would need to shake it much faster (higher frequency, smaller wavelength), because the post-it is smaller then a sheet of paper. Also, if you take a meter long sheet of paper and shake it that fast, it won't undulate a lot too. You would probably see the waves fading out through the paper, while it's other end barely moves. There is of course a lower frequency that would make it undulate entirely.



            Instruments function in a similar way. The string has to shake the body, to produce a louder sound, and therefore the body size must minimally match the wavelength of the sound waves you want to produce.







            share|improve this answer












            share|improve this answer



            share|improve this answer










            answered 14 hours ago









            coconochao

            1,24117




            1,24117








            • 3




              +1 Love the sheet of paper visual!
              – David K
              10 hours ago














            • 3




              +1 Love the sheet of paper visual!
              – David K
              10 hours ago








            3




            3




            +1 Love the sheet of paper visual!
            – David K
            10 hours ago




            +1 Love the sheet of paper visual!
            – David K
            10 hours ago










            up vote
            3
            down vote













            While each answer explains the physical properties and their relationship to the pitches being produced by the instrument, I'm inclined to add the aspect of the volume of air contained inside the instrument that resonates to amplify the sound the strings are producing. Larger volumes of air will resonate at lower pitches and increase the level of the sound being produced by the strings. The notes on a violin only require a sound box internal volume to resonate at a relatively high pitch, whereas a cello or bass needs a considerably larger sound box that will resonate at lower pitches in order to effectively amplify the sound being produced.






            share|improve this answer

























              up vote
              3
              down vote













              While each answer explains the physical properties and their relationship to the pitches being produced by the instrument, I'm inclined to add the aspect of the volume of air contained inside the instrument that resonates to amplify the sound the strings are producing. Larger volumes of air will resonate at lower pitches and increase the level of the sound being produced by the strings. The notes on a violin only require a sound box internal volume to resonate at a relatively high pitch, whereas a cello or bass needs a considerably larger sound box that will resonate at lower pitches in order to effectively amplify the sound being produced.






              share|improve this answer























                up vote
                3
                down vote










                up vote
                3
                down vote









                While each answer explains the physical properties and their relationship to the pitches being produced by the instrument, I'm inclined to add the aspect of the volume of air contained inside the instrument that resonates to amplify the sound the strings are producing. Larger volumes of air will resonate at lower pitches and increase the level of the sound being produced by the strings. The notes on a violin only require a sound box internal volume to resonate at a relatively high pitch, whereas a cello or bass needs a considerably larger sound box that will resonate at lower pitches in order to effectively amplify the sound being produced.






                share|improve this answer












                While each answer explains the physical properties and their relationship to the pitches being produced by the instrument, I'm inclined to add the aspect of the volume of air contained inside the instrument that resonates to amplify the sound the strings are producing. Larger volumes of air will resonate at lower pitches and increase the level of the sound being produced by the strings. The notes on a violin only require a sound box internal volume to resonate at a relatively high pitch, whereas a cello or bass needs a considerably larger sound box that will resonate at lower pitches in order to effectively amplify the sound being produced.







                share|improve this answer












                share|improve this answer



                share|improve this answer










                answered 7 hours ago









                skinny peacock

                1,9152321




                1,9152321






















                    up vote
                    2
                    down vote













                    You are only partly correct. For a given tension a string's fundamental resonant frequency scales with length. However, to within mechanical and material limits, you can increase or decrease tension on a fixed-length string to achieve any resonant frequency desired.



                    The string on a musical instrument is analogous to the oscillator in an electronic audio generator: it produces the source frequency(ies). The bridge and body of the instrument are analogous to the amplifier, transferring the energy from the string to the atmosphere with (one hopes!) minimal impedance mismatch (and yes, there is such a thing as acoustic impedance in air) so as to maximize the sound volume.






                    share|improve this answer

















                    • 1




                      It may be good to amplify "within mechanical and material limits" to note that for a cello-length string to reach the pitch of a violin's (high) E string would require that it be thinner and/or tighter than practical, and for a violin-length string to reach the pitch of a cello's (low) C string would require that it be thicker and/or looser than practical.
                      – supercat
                      8 hours ago






                    • 1




                      @supercat I'm a physicist. I make my strings out of unobtanium.
                      – Carl Witthoft
                      7 hours ago















                    up vote
                    2
                    down vote













                    You are only partly correct. For a given tension a string's fundamental resonant frequency scales with length. However, to within mechanical and material limits, you can increase or decrease tension on a fixed-length string to achieve any resonant frequency desired.



                    The string on a musical instrument is analogous to the oscillator in an electronic audio generator: it produces the source frequency(ies). The bridge and body of the instrument are analogous to the amplifier, transferring the energy from the string to the atmosphere with (one hopes!) minimal impedance mismatch (and yes, there is such a thing as acoustic impedance in air) so as to maximize the sound volume.






                    share|improve this answer

















                    • 1




                      It may be good to amplify "within mechanical and material limits" to note that for a cello-length string to reach the pitch of a violin's (high) E string would require that it be thinner and/or tighter than practical, and for a violin-length string to reach the pitch of a cello's (low) C string would require that it be thicker and/or looser than practical.
                      – supercat
                      8 hours ago






                    • 1




                      @supercat I'm a physicist. I make my strings out of unobtanium.
                      – Carl Witthoft
                      7 hours ago













                    up vote
                    2
                    down vote










                    up vote
                    2
                    down vote









                    You are only partly correct. For a given tension a string's fundamental resonant frequency scales with length. However, to within mechanical and material limits, you can increase or decrease tension on a fixed-length string to achieve any resonant frequency desired.



                    The string on a musical instrument is analogous to the oscillator in an electronic audio generator: it produces the source frequency(ies). The bridge and body of the instrument are analogous to the amplifier, transferring the energy from the string to the atmosphere with (one hopes!) minimal impedance mismatch (and yes, there is such a thing as acoustic impedance in air) so as to maximize the sound volume.






                    share|improve this answer












                    You are only partly correct. For a given tension a string's fundamental resonant frequency scales with length. However, to within mechanical and material limits, you can increase or decrease tension on a fixed-length string to achieve any resonant frequency desired.



                    The string on a musical instrument is analogous to the oscillator in an electronic audio generator: it produces the source frequency(ies). The bridge and body of the instrument are analogous to the amplifier, transferring the energy from the string to the atmosphere with (one hopes!) minimal impedance mismatch (and yes, there is such a thing as acoustic impedance in air) so as to maximize the sound volume.







                    share|improve this answer












                    share|improve this answer



                    share|improve this answer










                    answered 14 hours ago









                    Carl Witthoft

                    8,04811229




                    8,04811229








                    • 1




                      It may be good to amplify "within mechanical and material limits" to note that for a cello-length string to reach the pitch of a violin's (high) E string would require that it be thinner and/or tighter than practical, and for a violin-length string to reach the pitch of a cello's (low) C string would require that it be thicker and/or looser than practical.
                      – supercat
                      8 hours ago






                    • 1




                      @supercat I'm a physicist. I make my strings out of unobtanium.
                      – Carl Witthoft
                      7 hours ago














                    • 1




                      It may be good to amplify "within mechanical and material limits" to note that for a cello-length string to reach the pitch of a violin's (high) E string would require that it be thinner and/or tighter than practical, and for a violin-length string to reach the pitch of a cello's (low) C string would require that it be thicker and/or looser than practical.
                      – supercat
                      8 hours ago






                    • 1




                      @supercat I'm a physicist. I make my strings out of unobtanium.
                      – Carl Witthoft
                      7 hours ago








                    1




                    1




                    It may be good to amplify "within mechanical and material limits" to note that for a cello-length string to reach the pitch of a violin's (high) E string would require that it be thinner and/or tighter than practical, and for a violin-length string to reach the pitch of a cello's (low) C string would require that it be thicker and/or looser than practical.
                    – supercat
                    8 hours ago




                    It may be good to amplify "within mechanical and material limits" to note that for a cello-length string to reach the pitch of a violin's (high) E string would require that it be thinner and/or tighter than practical, and for a violin-length string to reach the pitch of a cello's (low) C string would require that it be thicker and/or looser than practical.
                    – supercat
                    8 hours ago




                    1




                    1




                    @supercat I'm a physicist. I make my strings out of unobtanium.
                    – Carl Witthoft
                    7 hours ago




                    @supercat I'm a physicist. I make my strings out of unobtanium.
                    – Carl Witthoft
                    7 hours ago










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