1
MHT CET 2021 21th September Morning Shift
+1
-0

A closed organ pipe of length '$$\mathrm{L}_c$$' and an open organ pipe of length '$$\mathrm{L}_{\mathrm{o}}$$' contain different gases of densities '$$\rho_1$$' and '$$\rho_2$$' respectively. The compressibility of the gases is the same in both the pipes. The gases are vibrating in their first overtone with the same frequency. What is the length of open organ pipe?

A
$$\frac{4 L_c}{3} \sqrt{\frac{\rho}{\rho_2}}$$
B
$$\frac{3 \mathrm{~L}_{\mathrm{c}}}{4} \sqrt{\frac{\rho_2}{\rho_1}}$$
C
$$\frac{4 L_c}{3} \sqrt{\frac{\rho_2}{\rho_1}}$$
D
$$\frac{2 L_c}{3} \sqrt{\frac{\rho_2}{\rho}}$$
2
MHT CET 2021 21th September Morning Shift
+1
-0

A progressive wave of frequency 50 Hz is travelling with velocity 350 m/s through a medium. The change in phase at a given time interval of 0.01 second is A
$$\frac{\pi}{4}$$ rad
B
$$\frac{3\pi}{2}$$ rad
C
$$\pi$$ rad
D
$$\frac{\pi}{2}$$ rad
3
MHT CET 2021 21th September Morning Shift
+1
-0

A simple harmonic progressive wave is given by $$Y=Y_0 \sin 2 \pi\left(n t-\frac{x}{\lambda}\right)$$. If the wave velocity is $$\left(\frac{1}{8}\right)^{\text {th }}$$ the maximum particle velocity then the wavelength is

A
$$\frac{\pi Y_0}{2}$$
B
$$\frac{\pi Y_0}{4}$$
C
$$\frac{\pi \mathrm{Y}_0}{8}$$
D
$$\frac{\pi Y_0}{16}$$
4
MHT CET 2021 21th September Morning Shift
+1
-0

In fundamental mode, the time required for the sound wave to reach upto the closed end of pipe filled with air is $$t$$ second. The frequency of vibration of air column is

A
$$\frac{1}{t}$$
B
$$\frac{2}{t}$$
C
$$\frac{3}{t}$$
D
$$\frac{0.25}{\mathrm{t}}$$
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Physics
Mechanics
Optics
Electromagnetism
Modern Physics
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Physical Chemistry
Inorganic Chemistry
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