Bridge Modeling

In §6.3 we analyzed the effect of rigid string terminations on traveling waves. We found that waves derived by time-derivatives of displacement (displacement, velocity, acceleration, and so on) reflect with a sign inversion, while waves defined in terms of the first spatial derivative of displacement (force, slope) reflect with no sign inversion. We now look at the more realistic case of yielding terminations for strings. This analysis can be considered a special case of the loaded string junction analyzed in §C.12.

Yielding string terminations (at the bridge) have a large effect on the sound produced by acoustic stringed instruments. Rigid terminations can be considered a reasonable model for the solid-body electric guitar in which maximum sustain is desired for played notes. Acoustic guitars, on the other hand, must transduce sound energy from the strings into the body of the instrument, and from there to the surrounding air. All audible sound energy comes from the string vibrational energy, thereby reducing the sustain (decay time) of each played note. Furthermore, because the bridge vibrates more easily in one direction than another, a kind of ``chorus effect'' is created from the detuning of the horizontal and vertical planes of string vibration (as discussed further in §6.12.1). A perfectly rigid bridge, in contrast, cannot transmit any sound into the body of the instrument, thereby requiring some other transducer, such as the magnetic pickups used in electric guitars, to extract sound for output.^10.4

• Passive String Terminations
• A Terminating Resonator
• Bridge Reflectance
• Bridge Transmittance
• Digitizing Bridge Reflectance
• A Two-Resonance Guitar Bridge
• Measured Guitar-Bridge Admittance
• Building a Synthetic Guitar Bridge Admittance
• Passive Reflectance Synthesis--Method 1
• Passive Reflectance Synthesis--Method 2
• Matlab for Passive Reflectance Synthesis Method 1
• Matlab for Passive Reflectance Synthesis Method 2
• Matrix Bridge Impedance