Key relationship
v=√(γp/ρ)=√(γRT/M); M is molar mass in kg/mol; molecular vrms=√(3RT/M).
Physics · Class 11
Sound propagation depends on a gas’s adiabatic compressibility and density. In an ideal gas their pressure dependence cancels, leaving temperature, molar mass and heat-capacity ratio. Warm or light gases transmit sound faster.
Open the interactive experiment →நல்லியல்பு வாயுவில் ஒலி வேகம் √(γRT/M). வெப்பநிலை அதிகமாயின் அல்லது மோலார் நிறை குறைந்தால் வேகம் அதிகம்.
v=√(γp/ρ)=√(γRT/M); M is molar mass in kg/mol; molecular vrms=√(3RT/M).
Sound propagation depends on a gas’s adiabatic compressibility and density. In an ideal gas their pressure dependence cancels, leaving temperature, molar mass and heat-capacity ratio. Warm or light gases transmit sound faster.
Sound speed is not the RMS speed of gas molecules.
Small-amplitude adiabatic sound in an ideal gas; M converted to kg/mol, constant γ and negligible humidity. Sound speed is independent of pressure at fixed ideal-gas temperature and composition.
Relate adiabatic response and molecular properties to sound speed.
Try both scenarios, change one control, and predict the result before checking the graph and readouts.
Change one input while keeping the others fixed, as you would in a controlled experiment.
For air approximated by M=0.029 kg/mol, γ=1.4 and T=300 K, v≈347.0 m/s. Doubling pressure at that same state temperature does not change this ideal value.
The model connects change the speed of sound in a gas with an observable reading. Check the equation and assumptions before applying it.
SI units · algebra · graph reading
If kelvin temperature quadruples for the same gas, what happens to sound speed?
Sound speed is proportional to √T.
Course connection: Class XI Chapter 14. Consult the roadmap for CBSE, NEET, JEE Main and Advanced scope.