Sound Waves and Intensity
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
PHXI15:WAVES

354812 The ratio of intensities between two coherent sound sources is \(4: 1\). The difference of loudness in decibels \((\mathrm{dB})\) between maximum and minimum intensities when they interfere in space is:

1 \(10 \log 2\)
2 \(20 \log 3\)
3 \(10 \log 3\)
4 \(20 \log 2\)
PHXI15:WAVES

354813 If \(T\) is the reverberation time of an auditorium of volume \(V\) then

1 \(T \propto \dfrac{1}{V^{2}}\)
2 \(T \propto \dfrac{1}{V}\)
3 \(T \propto V\)
4 \(T \propto V^{2}\)
PHXI15:WAVES

354814 The intensity of sound increases at night due to:

1 Increases in density of air
2 Decreases in density of air
3 High temperature
4 None of these
PHXI15:WAVES

354815 The intensity level of sound wave is said to be 4 decibel. If the intensity of wave is doubled, then the intensity level of sound as expressed in decibel would be

1 16
2 8
3 14
4 7
PHXI15:WAVES

354812 The ratio of intensities between two coherent sound sources is \(4: 1\). The difference of loudness in decibels \((\mathrm{dB})\) between maximum and minimum intensities when they interfere in space is:

1 \(10 \log 2\)
2 \(20 \log 3\)
3 \(10 \log 3\)
4 \(20 \log 2\)
PHXI15:WAVES

354813 If \(T\) is the reverberation time of an auditorium of volume \(V\) then

1 \(T \propto \dfrac{1}{V^{2}}\)
2 \(T \propto \dfrac{1}{V}\)
3 \(T \propto V\)
4 \(T \propto V^{2}\)
PHXI15:WAVES

354814 The intensity of sound increases at night due to:

1 Increases in density of air
2 Decreases in density of air
3 High temperature
4 None of these
PHXI15:WAVES

354815 The intensity level of sound wave is said to be 4 decibel. If the intensity of wave is doubled, then the intensity level of sound as expressed in decibel would be

1 16
2 8
3 14
4 7
PHXI15:WAVES

354812 The ratio of intensities between two coherent sound sources is \(4: 1\). The difference of loudness in decibels \((\mathrm{dB})\) between maximum and minimum intensities when they interfere in space is:

1 \(10 \log 2\)
2 \(20 \log 3\)
3 \(10 \log 3\)
4 \(20 \log 2\)
PHXI15:WAVES

354813 If \(T\) is the reverberation time of an auditorium of volume \(V\) then

1 \(T \propto \dfrac{1}{V^{2}}\)
2 \(T \propto \dfrac{1}{V}\)
3 \(T \propto V\)
4 \(T \propto V^{2}\)
PHXI15:WAVES

354814 The intensity of sound increases at night due to:

1 Increases in density of air
2 Decreases in density of air
3 High temperature
4 None of these
PHXI15:WAVES

354815 The intensity level of sound wave is said to be 4 decibel. If the intensity of wave is doubled, then the intensity level of sound as expressed in decibel would be

1 16
2 8
3 14
4 7
PHXI15:WAVES

354812 The ratio of intensities between two coherent sound sources is \(4: 1\). The difference of loudness in decibels \((\mathrm{dB})\) between maximum and minimum intensities when they interfere in space is:

1 \(10 \log 2\)
2 \(20 \log 3\)
3 \(10 \log 3\)
4 \(20 \log 2\)
PHXI15:WAVES

354813 If \(T\) is the reverberation time of an auditorium of volume \(V\) then

1 \(T \propto \dfrac{1}{V^{2}}\)
2 \(T \propto \dfrac{1}{V}\)
3 \(T \propto V\)
4 \(T \propto V^{2}\)
PHXI15:WAVES

354814 The intensity of sound increases at night due to:

1 Increases in density of air
2 Decreases in density of air
3 High temperature
4 None of these
PHXI15:WAVES

354815 The intensity level of sound wave is said to be 4 decibel. If the intensity of wave is doubled, then the intensity level of sound as expressed in decibel would be

1 16
2 8
3 14
4 7