Figure 4
Numerical errors in the FDTD algorithm as a function of frequency for a model as in Fig. 3, computed at a propagation angle of 0°. (a) Variation of the normalized sound speed ratio . The solid line are the values computed for a model with no attenuation. The dots indicate values computed for η=ζ= 1.8 × 10−5 kg m−1 s−1 at a density ρo= 1 × 10−7 kg  m−3. (b) Variation in attenuation ratios  for a model with attenuation as in (a).

Numerical errors in the FDTD algorithm as a function of frequency for a model as in Fig. 3, computed at a propagation angle of 0°. (a) Variation of the normalized sound speed ratio graphic. The solid line are the values computed for a model with no attenuation. The dots indicate values computed for η=ζ= 1.8 × 10−5 kg m−1 s−1 at a density ρo= 1 × 10−7 kg m−3. (b) Variation in attenuation ratios graphic for a model with attenuation as in (a).

Close
This Feature Is Available To Subscribers Only

Sign In or Create an Account

Close

This PDF is available to Subscribers Only

View Article Abstract & Purchase Options

For full access to this pdf, sign in to an existing account, or purchase an annual subscription.

Close