### ``Piano hammer in flight''

Suppose we wish to model a situation in which a mass of size kilograms is traveling with a constant velocity. This is an appropriate model for a piano hammer after its key has been pressed and before the hammer has reached the string.Figure F.2 shows the ``wave digital mass'' derived previously. The derivation consisted of inserting an infinitesimal waveguide

^{F.3}having (real) impedance , solving for the force-wave reflectance of the mass as seen from the waveguide, and then mapping it to the discrete time domain using the bilinear transform. We now need to attach the other end of the transmission line to a ``force source'' which applies a force of zero newtons to the mass. In other words, we need to terminate the line in a way that corresponds to zero force. Let the force-wave components entering and leaving the mass be denoted and , respectively (

*i.e.*, we are dropping the subscript `d' in Fig.F.2). The physical force associated with the mass is

*implementation*, Fig.F.8b would be more typical in practice. This is because we can always negate the state variable if needed to convert it from to . It is very common to see final simplifications like this to maximize efficiency. Note that Fig.F.8b can be interpreted physically as a wave digital

*spring*displaced by a constant force .

#### Extracting Physical Quantities

Since we are using a force-wave simulation, the state variable (delay element output) is in units of physical force (newtons). Specifically, . (The physical force is, of course, 0, while its traveling-wave components are not 0 unless the mass is at rest.) Using the fundamental relations relating traveling force and velocity waves*I.e.*, the square of the state variable can be scaled by to produce the physical kinetic energy associated with the mass.

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Force Driving a Mass

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General Series Adaptor for Force Waves