Someone evaluates the classical absorption formula for air at and concludes that a…

PHYSICS · Multi-part · Fermi University Physics · Oscillations, Waves & Acoustics · Acoustics of fluids: generation, propagation and attenuation · Acoustics of fluids: generation, propagation and attenuation

Signal Speeds in Fluids, Ch Sound in a moving, absorbing fluid: sources, refraction and loss

Problem

Someone evaluates the classical absorption formula for air at 20∘C20^\circ\mathrm{C} and concludes that a 4 kHz4\,\mathrm{kHz} alarm loses only about 25 dB25\,\mathrm{dB} over 10 km10\,\mathrm{km}. Take μ=1.81×10−5 Pa s\mu=1.81\times10^{-5}\,\mathrm{Pa\,s}, μb=0.6μ\mu_{\rm b}=0.6\mu, kT=0.0257 W m−1 K−1k_T=0.0257\,\mathrm{W\,m^{-1}\,K^{-1}}, γ=1.4\gamma=1.4, cp=1005 J kg−1 K−1c_p=1005\,\mathrm{J\,kg^{-1}\,K^{-1}}, ρ0=1.204 kg m−3\rho_0=1.204\,\mathrm{kg\,m^{-3}} and c0=343.2 m s−1c_0=343.2\,\mathrm{m\,s^{-1}}. ((a)) Evaluate the classical α\alpha at 4 kHz4\,\mathrm{kHz} in Np m−1\mathrm{Np\,m^{-1}} and in dB km−1\mathrm{dB\,km^{-1}}, and confirm the 25 dB25\,\mathrm{dB}. ((b)) The measured absorption at 4 kHz4\,\mathrm{kHz} and 5050 per cent relative humidity is about 30 dB km−130\,\mathrm{dB\,km^{-1}}. What does the classical formula leave out, and what is the real loss over 10 km10\,\mathrm{km}? ((c)) For water at 3 MHz3\,\mathrm{MHz} (ρ0=998 kg m−3\rho_0=998\,\mathrm{kg\,m^{-3}}, c0=1482 m s−1c_0=1482\,\mathrm{m\,s^{-1}}, μ=1.0×10−3 Pa s\mu=1.0\times10^{-3}\,\mathrm{Pa\,s}, μb=2.8×10−3 Pa s\mu_{\rm b}=2.8\times10^{-3}\,\mathrm{Pa\,s}, conduction negligible), evaluate α\alpha and the distance over which a beam's intensity halves.

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