$A$ sound wave passing through an ideal gas at $NTP$ produces a pressure change of $0.001 \text{ dyne}/cm^2$ during adiabatic compression. The corresponding change in temperature $(\gamma = 1.5$ for the gas and atmospheric pressure is $1.013 \times 10^6 \text{ dyne}/cm^2)$ is:

  • A
    $8.97 \times 10^{-4} \text{ K}$
  • B
    $8.97 \times 10^{-6} \text{ K}$
  • C
    $8.97 \times 10^{-8} \text{ K}$
  • D
    $8.97 \times 10^{-9} \text{ K}$

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