Titlebook: Understanding Acoustics; An Experimentalist’s Steven L. Garrett Textbook 20171st edition Springer International Publishing AG 2017 Acoustic

Maudlin

書(shū)目名稱Understanding Acoustics影響因子(影響力)




書(shū)目名稱Understanding Acoustics影響因子(影響力)學(xué)科排名




書(shū)目名稱Understanding Acoustics網(wǎng)絡(luò)公開(kāi)度




書(shū)目名稱Understanding Acoustics網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書(shū)目名稱Understanding Acoustics被引頻次




書(shū)目名稱Understanding Acoustics被引頻次學(xué)科排名




書(shū)目名稱Understanding Acoustics年度引用




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書(shū)目名稱Understanding Acoustics讀者反饋




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手勢(shì)

占線

FLOAT

fatty-streak

Comfort for the Computationally Crippled,ics. This chapter is intended as an introduction to some of the more useful mathematical concepts, strategies, and techniques that are employed in the description of vibrational and acoustical systems and the calculations of their behavior.

PALL

String Theoryasy to visualize and it introduces concepts and techniques that will recur throughout our study of vibration and the acoustics of continua. A retrospective of these concepts and techniques is provided in Sect. ., near the end of this chapter. You might want to skip ahead to read that section to understand the plot before you meet the characters.

無(wú)目標(biāo)

Elasticity of Solidsolid to deform by an amount that is directly proportional to the applied forces. When the forces are removed the sample will return to its original shape and size. These are the characteristics that are required if we say the behavior of the solid is “elastic.”

假設(shè)

清晰

Dissipative Hydrodynamicsn Figs. . and ., and in Eq. (.), did not include any dissipation. By introducing D.EC, we were able to calculate the amount of power dissipated in the neck (inertance) and volume (compliance) of a 500-mL boiling flask. In this chapter, those losses will be calculated from hydrodynamic “first principles.”

取之不竭

One-Dimensional Propagationsions for acoustic intensity and the acoustic kinetic and potential energy densities. The “machinery” developed to describe waves on strings will be sufficient to describe one-dimensional sound propagation in fluids, even though the waves on the string were transverse and the one-dimensional waves in fluids are longitudinal.