Yes, it is more or less so. The string itself, vibrating in free air, would put very little air particles in motion. The cello's body, with its wide surface, helps to put in motion many more air particles all around, generating strong sound waves that are easily hearable.Daithi wrote:So if I understand this correctly the walls of the cello are designed to reproduce the frequency of and vibrate in sympathy with the vibrations generated by the strings
Well, not exactly... or better "no longer exactly". This is basically what the "ancient" theory said: that megaphones and similar objects worked because they concentrated the sound in one direction, but this is not what really happens.Daithi wrote:the horn is designed to be a dead thing and to not vibrate but simply direct the sound.
The acoustical impedance is to some degree similar to electric impedance (hence the similar name), should you be somewhat more familiar with it. Very shortly, it can be mathematically demonstrated that the power that can be transmitted from one device to another device is maximised if the two devices have the same impedance. For example, in tube radios or amplifiers, as tubes have an inherently very high impedance, if the output is connected directly to a loudspeaker (which conversely has tipically a very low impedance, around 8 Ohm or so) almost no sound can be heard. This is why tube radios have output transformers in order to connect the output tube to the loudspeaker: the transformer is calculated so that the impedance of the tube and of the loudspeaker are matched. The loudspeaker "sees" the tube through the transformer as if it had a low impedance, and on the other side the tube "sees" the loudspeaker through the transformer as if it had a high impedance. If the two impedances are exactly matched, the power transmitted reaches its maximum.
With gramophones, the vibrating diaphragm is the "high impedance" device, which generates in a small area in its surroundings sound waves of compressed air. The huge quantity of air filling the space of the room has "low impedance" and the tiny soundwaves surrounding the soundbox would not be able to put in motion all the huge quantity of air particles filling the room, and as a result only a feeble, almost un-hearable sound is generated. If a horn is applied to the diaphragm, then the air particles set in motion by the diaphragm will not interact directly with the entire room, but they will progressively transmit their motion to increasing and increasing surfaces inside the horn, while the waves expand as they travel from the small throat of the horn to the wide mouth of the horn. When the wavefront reaches the mouth of the horn, there is not too much impedance mismatch left, and the sound is delivered to the room efficiently.