Light propagating through a sound waveThe nature of lightWhy does sound travel faster in iron than mercury even though mercury has a higher density?light color and refractionwhy does the optical media have different refractive indices?Intensity of Sound WaveWhat exactly are light waves?How can muons travel faster than light through ice?Why doesn't a medium travel along with the wave propagating through it?What prevents sound to be just wind?Why does the speed of sound relate to temperature in increasing altitude?

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Light propagating through a sound wave


The nature of lightWhy does sound travel faster in iron than mercury even though mercury has a higher density?light color and refractionwhy does the optical media have different refractive indices?Intensity of Sound WaveWhat exactly are light waves?How can muons travel faster than light through ice?Why doesn't a medium travel along with the wave propagating through it?What prevents sound to be just wind?Why does the speed of sound relate to temperature in increasing altitude?













18












$begingroup$


We know that the speed of light depends on the density of the medium it is travelling through. It travels faster through less dense media and slower through more dense media.



When we produce sound, a series of rarefactions and compressions are created in the medium by the vibration of the source of sound. Compressions have high pressure and high density, while rarefactions have low pressure and low density.



If light is made to propagate through such a disturbance in the medium, does it experience refraction due to changes in the density of the medium? Why don't we observe this?










share|cite|improve this question











$endgroup$







  • 12




    $begingroup$
    An effect like this is used in acousto-optic modulators.
    $endgroup$
    – Emil
    2 days ago















18












$begingroup$


We know that the speed of light depends on the density of the medium it is travelling through. It travels faster through less dense media and slower through more dense media.



When we produce sound, a series of rarefactions and compressions are created in the medium by the vibration of the source of sound. Compressions have high pressure and high density, while rarefactions have low pressure and low density.



If light is made to propagate through such a disturbance in the medium, does it experience refraction due to changes in the density of the medium? Why don't we observe this?










share|cite|improve this question











$endgroup$







  • 12




    $begingroup$
    An effect like this is used in acousto-optic modulators.
    $endgroup$
    – Emil
    2 days ago













18












18








18


6



$begingroup$


We know that the speed of light depends on the density of the medium it is travelling through. It travels faster through less dense media and slower through more dense media.



When we produce sound, a series of rarefactions and compressions are created in the medium by the vibration of the source of sound. Compressions have high pressure and high density, while rarefactions have low pressure and low density.



If light is made to propagate through such a disturbance in the medium, does it experience refraction due to changes in the density of the medium? Why don't we observe this?










share|cite|improve this question











$endgroup$




We know that the speed of light depends on the density of the medium it is travelling through. It travels faster through less dense media and slower through more dense media.



When we produce sound, a series of rarefactions and compressions are created in the medium by the vibration of the source of sound. Compressions have high pressure and high density, while rarefactions have low pressure and low density.



If light is made to propagate through such a disturbance in the medium, does it experience refraction due to changes in the density of the medium? Why don't we observe this?







visible-light speed-of-light acoustics refraction






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited 2 days ago









Rodrigo de Azevedo

1617




1617










asked 2 days ago









Mrigank PawagiMrigank Pawagi

5691311




5691311







  • 12




    $begingroup$
    An effect like this is used in acousto-optic modulators.
    $endgroup$
    – Emil
    2 days ago












  • 12




    $begingroup$
    An effect like this is used in acousto-optic modulators.
    $endgroup$
    – Emil
    2 days ago







12




12




$begingroup$
An effect like this is used in acousto-optic modulators.
$endgroup$
– Emil
2 days ago




$begingroup$
An effect like this is used in acousto-optic modulators.
$endgroup$
– Emil
2 days ago










4 Answers
4






active

oldest

votes


















23












$begingroup$

Actually this effect has been discovered in 1932 with light diffracted by ultra-sound waves.
In order to get observable effects you need ultra-sound
with wavelengths in the μm range (i.e. not much longer than light waves),
and thus sound frequencies in the MHz range.



See for example here:




  • On the Scattering of Light by Supersonic Waves

    by Debye and Sears in 1932




    image





  • Propriétés optiques des milieux solides et liquides soumis aux
    vibrations élastiques ultra sonores

    (Optical properties of solid and liquid media subjected to ultrasonic elastic vibrations)

    by Lucas and Biquard in 1932



    translated from French:




    Abstract : This article describes the main optical properties presented by solid and liquid media, subjected to ultra sonic elastic vibrations whose frequencies range from 600,000 to 30 million per second. These ultra sounds were obtained by Langevin's method using piezoelectric quartz excited in high frequency. Under these conditions, and according to the relative values of the elastic wavelength dimensions, the wavelengths of light, and the opening of the light beam passing through the medium studied, different optical phenomena are observable. In the case of the smallest elastic wavelengths of up to a few tenths of a millimeter, grating-like light diffraction patterns are observed when the incident light rays run parallel to the elastic wave planes.
    image





  • The diffraction of light by high frequency sound waves: Part I

    by Raman and Nagendra Nathe in 1935


    A theory of the phenomenon of the diffraction of light by sound-waves of high frequency in a medium, discovered by Debye and Sears and Lucas and Biquard, is developed.








share|cite|improve this answer











$endgroup$








  • 1




    $begingroup$
    I'd note that AOMs (Acousto-optic Modulators) are devices that use this effect precisely to alter the properties of light passing through them
    $endgroup$
    – CharlieB
    2 days ago


















4












$begingroup$

I have seen it with standing waves in water, a PhyWe demonstration experiment. The frequency 800 kHz, which gives a distance between nodes of about a millimeter. The standing wave is in a cuvette, between the head of a piezo hydrophone transducer and the bottom. When looking through the water, one sees the varying index of refraction as a "wavyness" of the background.



I could not find a description of this online, but I found this about demonstration experiments in air: https://docplayer.org/52348266-Unsichtbares-sichtbar-machen-schallwellenfronten-im-bild.html






share|cite|improve this answer











$endgroup$




















    2












    $begingroup$

    A few factors contribute to this:



    • Air has low index of refraction therefore optical effects arising from its mechanical pressure will be weak;

    • Even loud sounds have low mechanical pressure. Wolfram Alpha database lists 200 pascals as pressure of jet airplane at 100 meters, which works out as ~0.5% pressure difference between peak and trough;

    • Waves do not cause harsh boundary between high and low pressures;

    • Sources of loud sounds typically cause other phenomena that obscure this. Combustion creates light and heat, and rapid pressure release can force water in the air to become opaque.

    Even with all that, it is possible to magnify the effect using distant point light and either by merely observing refracted patterns or creating a setup where half of the refocused image is blocked. Using the second technique it is possible to observe clap of hands.






    share|cite|improve this answer








    New contributor




    transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
    Check out our Code of Conduct.






    $endgroup$












    • $begingroup$
      Thank You for the answer!
      $endgroup$
      – Mrigank Pawagi
      yesterday


















    1












    $begingroup$

    You can see the effect of density change on refractive index due to heating of air. For a simple example, light a candle and look through the air column directly above the flame. The flame heats air which rises, but the flow is turbulent, so you'll see objects on the other side of the air column shimmer as the stream of hot air wavers from side to side.



    You can see this effect when you look across a paved surface on a hot sunny day.



    You won't see this effect with sound, at least not at typical listening levels because the density changes are too small (as noted in one of the other answers).






    share|cite|improve this answer









    $endgroup$












    • $begingroup$
      Thanks for the Answer!
      $endgroup$
      – Mrigank Pawagi
      yesterday










    Your Answer





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    4 Answers
    4






    active

    oldest

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    4 Answers
    4






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

    votes









    23












    $begingroup$

    Actually this effect has been discovered in 1932 with light diffracted by ultra-sound waves.
    In order to get observable effects you need ultra-sound
    with wavelengths in the μm range (i.e. not much longer than light waves),
    and thus sound frequencies in the MHz range.



    See for example here:




    • On the Scattering of Light by Supersonic Waves

      by Debye and Sears in 1932




      image





    • Propriétés optiques des milieux solides et liquides soumis aux
      vibrations élastiques ultra sonores

      (Optical properties of solid and liquid media subjected to ultrasonic elastic vibrations)

      by Lucas and Biquard in 1932



      translated from French:




      Abstract : This article describes the main optical properties presented by solid and liquid media, subjected to ultra sonic elastic vibrations whose frequencies range from 600,000 to 30 million per second. These ultra sounds were obtained by Langevin's method using piezoelectric quartz excited in high frequency. Under these conditions, and according to the relative values of the elastic wavelength dimensions, the wavelengths of light, and the opening of the light beam passing through the medium studied, different optical phenomena are observable. In the case of the smallest elastic wavelengths of up to a few tenths of a millimeter, grating-like light diffraction patterns are observed when the incident light rays run parallel to the elastic wave planes.
      image





    • The diffraction of light by high frequency sound waves: Part I

      by Raman and Nagendra Nathe in 1935


      A theory of the phenomenon of the diffraction of light by sound-waves of high frequency in a medium, discovered by Debye and Sears and Lucas and Biquard, is developed.








    share|cite|improve this answer











    $endgroup$








    • 1




      $begingroup$
      I'd note that AOMs (Acousto-optic Modulators) are devices that use this effect precisely to alter the properties of light passing through them
      $endgroup$
      – CharlieB
      2 days ago















    23












    $begingroup$

    Actually this effect has been discovered in 1932 with light diffracted by ultra-sound waves.
    In order to get observable effects you need ultra-sound
    with wavelengths in the μm range (i.e. not much longer than light waves),
    and thus sound frequencies in the MHz range.



    See for example here:




    • On the Scattering of Light by Supersonic Waves

      by Debye and Sears in 1932




      image





    • Propriétés optiques des milieux solides et liquides soumis aux
      vibrations élastiques ultra sonores

      (Optical properties of solid and liquid media subjected to ultrasonic elastic vibrations)

      by Lucas and Biquard in 1932



      translated from French:




      Abstract : This article describes the main optical properties presented by solid and liquid media, subjected to ultra sonic elastic vibrations whose frequencies range from 600,000 to 30 million per second. These ultra sounds were obtained by Langevin's method using piezoelectric quartz excited in high frequency. Under these conditions, and according to the relative values of the elastic wavelength dimensions, the wavelengths of light, and the opening of the light beam passing through the medium studied, different optical phenomena are observable. In the case of the smallest elastic wavelengths of up to a few tenths of a millimeter, grating-like light diffraction patterns are observed when the incident light rays run parallel to the elastic wave planes.
      image





    • The diffraction of light by high frequency sound waves: Part I

      by Raman and Nagendra Nathe in 1935


      A theory of the phenomenon of the diffraction of light by sound-waves of high frequency in a medium, discovered by Debye and Sears and Lucas and Biquard, is developed.








    share|cite|improve this answer











    $endgroup$








    • 1




      $begingroup$
      I'd note that AOMs (Acousto-optic Modulators) are devices that use this effect precisely to alter the properties of light passing through them
      $endgroup$
      – CharlieB
      2 days ago













    23












    23








    23





    $begingroup$

    Actually this effect has been discovered in 1932 with light diffracted by ultra-sound waves.
    In order to get observable effects you need ultra-sound
    with wavelengths in the μm range (i.e. not much longer than light waves),
    and thus sound frequencies in the MHz range.



    See for example here:




    • On the Scattering of Light by Supersonic Waves

      by Debye and Sears in 1932




      image





    • Propriétés optiques des milieux solides et liquides soumis aux
      vibrations élastiques ultra sonores

      (Optical properties of solid and liquid media subjected to ultrasonic elastic vibrations)

      by Lucas and Biquard in 1932



      translated from French:




      Abstract : This article describes the main optical properties presented by solid and liquid media, subjected to ultra sonic elastic vibrations whose frequencies range from 600,000 to 30 million per second. These ultra sounds were obtained by Langevin's method using piezoelectric quartz excited in high frequency. Under these conditions, and according to the relative values of the elastic wavelength dimensions, the wavelengths of light, and the opening of the light beam passing through the medium studied, different optical phenomena are observable. In the case of the smallest elastic wavelengths of up to a few tenths of a millimeter, grating-like light diffraction patterns are observed when the incident light rays run parallel to the elastic wave planes.
      image





    • The diffraction of light by high frequency sound waves: Part I

      by Raman and Nagendra Nathe in 1935


      A theory of the phenomenon of the diffraction of light by sound-waves of high frequency in a medium, discovered by Debye and Sears and Lucas and Biquard, is developed.








    share|cite|improve this answer











    $endgroup$



    Actually this effect has been discovered in 1932 with light diffracted by ultra-sound waves.
    In order to get observable effects you need ultra-sound
    with wavelengths in the μm range (i.e. not much longer than light waves),
    and thus sound frequencies in the MHz range.



    See for example here:




    • On the Scattering of Light by Supersonic Waves

      by Debye and Sears in 1932




      image





    • Propriétés optiques des milieux solides et liquides soumis aux
      vibrations élastiques ultra sonores

      (Optical properties of solid and liquid media subjected to ultrasonic elastic vibrations)

      by Lucas and Biquard in 1932



      translated from French:




      Abstract : This article describes the main optical properties presented by solid and liquid media, subjected to ultra sonic elastic vibrations whose frequencies range from 600,000 to 30 million per second. These ultra sounds were obtained by Langevin's method using piezoelectric quartz excited in high frequency. Under these conditions, and according to the relative values of the elastic wavelength dimensions, the wavelengths of light, and the opening of the light beam passing through the medium studied, different optical phenomena are observable. In the case of the smallest elastic wavelengths of up to a few tenths of a millimeter, grating-like light diffraction patterns are observed when the incident light rays run parallel to the elastic wave planes.
      image





    • The diffraction of light by high frequency sound waves: Part I

      by Raman and Nagendra Nathe in 1935


      A theory of the phenomenon of the diffraction of light by sound-waves of high frequency in a medium, discovered by Debye and Sears and Lucas and Biquard, is developed.









    share|cite|improve this answer














    share|cite|improve this answer



    share|cite|improve this answer








    edited yesterday

























    answered 2 days ago









    Thomas FritschThomas Fritsch

    1,115313




    1,115313







    • 1




      $begingroup$
      I'd note that AOMs (Acousto-optic Modulators) are devices that use this effect precisely to alter the properties of light passing through them
      $endgroup$
      – CharlieB
      2 days ago












    • 1




      $begingroup$
      I'd note that AOMs (Acousto-optic Modulators) are devices that use this effect precisely to alter the properties of light passing through them
      $endgroup$
      – CharlieB
      2 days ago







    1




    1




    $begingroup$
    I'd note that AOMs (Acousto-optic Modulators) are devices that use this effect precisely to alter the properties of light passing through them
    $endgroup$
    – CharlieB
    2 days ago




    $begingroup$
    I'd note that AOMs (Acousto-optic Modulators) are devices that use this effect precisely to alter the properties of light passing through them
    $endgroup$
    – CharlieB
    2 days ago











    4












    $begingroup$

    I have seen it with standing waves in water, a PhyWe demonstration experiment. The frequency 800 kHz, which gives a distance between nodes of about a millimeter. The standing wave is in a cuvette, between the head of a piezo hydrophone transducer and the bottom. When looking through the water, one sees the varying index of refraction as a "wavyness" of the background.



    I could not find a description of this online, but I found this about demonstration experiments in air: https://docplayer.org/52348266-Unsichtbares-sichtbar-machen-schallwellenfronten-im-bild.html






    share|cite|improve this answer











    $endgroup$

















      4












      $begingroup$

      I have seen it with standing waves in water, a PhyWe demonstration experiment. The frequency 800 kHz, which gives a distance between nodes of about a millimeter. The standing wave is in a cuvette, between the head of a piezo hydrophone transducer and the bottom. When looking through the water, one sees the varying index of refraction as a "wavyness" of the background.



      I could not find a description of this online, but I found this about demonstration experiments in air: https://docplayer.org/52348266-Unsichtbares-sichtbar-machen-schallwellenfronten-im-bild.html






      share|cite|improve this answer











      $endgroup$















        4












        4








        4





        $begingroup$

        I have seen it with standing waves in water, a PhyWe demonstration experiment. The frequency 800 kHz, which gives a distance between nodes of about a millimeter. The standing wave is in a cuvette, between the head of a piezo hydrophone transducer and the bottom. When looking through the water, one sees the varying index of refraction as a "wavyness" of the background.



        I could not find a description of this online, but I found this about demonstration experiments in air: https://docplayer.org/52348266-Unsichtbares-sichtbar-machen-schallwellenfronten-im-bild.html






        share|cite|improve this answer











        $endgroup$



        I have seen it with standing waves in water, a PhyWe demonstration experiment. The frequency 800 kHz, which gives a distance between nodes of about a millimeter. The standing wave is in a cuvette, between the head of a piezo hydrophone transducer and the bottom. When looking through the water, one sees the varying index of refraction as a "wavyness" of the background.



        I could not find a description of this online, but I found this about demonstration experiments in air: https://docplayer.org/52348266-Unsichtbares-sichtbar-machen-schallwellenfronten-im-bild.html







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited 2 days ago

























        answered 2 days ago









        PieterPieter

        9,02331536




        9,02331536





















            2












            $begingroup$

            A few factors contribute to this:



            • Air has low index of refraction therefore optical effects arising from its mechanical pressure will be weak;

            • Even loud sounds have low mechanical pressure. Wolfram Alpha database lists 200 pascals as pressure of jet airplane at 100 meters, which works out as ~0.5% pressure difference between peak and trough;

            • Waves do not cause harsh boundary between high and low pressures;

            • Sources of loud sounds typically cause other phenomena that obscure this. Combustion creates light and heat, and rapid pressure release can force water in the air to become opaque.

            Even with all that, it is possible to magnify the effect using distant point light and either by merely observing refracted patterns or creating a setup where half of the refocused image is blocked. Using the second technique it is possible to observe clap of hands.






            share|cite|improve this answer








            New contributor




            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.






            $endgroup$












            • $begingroup$
              Thank You for the answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday















            2












            $begingroup$

            A few factors contribute to this:



            • Air has low index of refraction therefore optical effects arising from its mechanical pressure will be weak;

            • Even loud sounds have low mechanical pressure. Wolfram Alpha database lists 200 pascals as pressure of jet airplane at 100 meters, which works out as ~0.5% pressure difference between peak and trough;

            • Waves do not cause harsh boundary between high and low pressures;

            • Sources of loud sounds typically cause other phenomena that obscure this. Combustion creates light and heat, and rapid pressure release can force water in the air to become opaque.

            Even with all that, it is possible to magnify the effect using distant point light and either by merely observing refracted patterns or creating a setup where half of the refocused image is blocked. Using the second technique it is possible to observe clap of hands.






            share|cite|improve this answer








            New contributor




            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.






            $endgroup$












            • $begingroup$
              Thank You for the answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday













            2












            2








            2





            $begingroup$

            A few factors contribute to this:



            • Air has low index of refraction therefore optical effects arising from its mechanical pressure will be weak;

            • Even loud sounds have low mechanical pressure. Wolfram Alpha database lists 200 pascals as pressure of jet airplane at 100 meters, which works out as ~0.5% pressure difference between peak and trough;

            • Waves do not cause harsh boundary between high and low pressures;

            • Sources of loud sounds typically cause other phenomena that obscure this. Combustion creates light and heat, and rapid pressure release can force water in the air to become opaque.

            Even with all that, it is possible to magnify the effect using distant point light and either by merely observing refracted patterns or creating a setup where half of the refocused image is blocked. Using the second technique it is possible to observe clap of hands.






            share|cite|improve this answer








            New contributor




            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.






            $endgroup$



            A few factors contribute to this:



            • Air has low index of refraction therefore optical effects arising from its mechanical pressure will be weak;

            • Even loud sounds have low mechanical pressure. Wolfram Alpha database lists 200 pascals as pressure of jet airplane at 100 meters, which works out as ~0.5% pressure difference between peak and trough;

            • Waves do not cause harsh boundary between high and low pressures;

            • Sources of loud sounds typically cause other phenomena that obscure this. Combustion creates light and heat, and rapid pressure release can force water in the air to become opaque.

            Even with all that, it is possible to magnify the effect using distant point light and either by merely observing refracted patterns or creating a setup where half of the refocused image is blocked. Using the second technique it is possible to observe clap of hands.







            share|cite|improve this answer








            New contributor




            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.









            share|cite|improve this answer



            share|cite|improve this answer






            New contributor




            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.









            answered 2 days ago









            transistor09transistor09

            1211




            1211




            New contributor




            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.





            New contributor





            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.






            transistor09 is a new contributor to this site. Take care in asking for clarification, commenting, and answering.
            Check out our Code of Conduct.











            • $begingroup$
              Thank You for the answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday
















            • $begingroup$
              Thank You for the answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday















            $begingroup$
            Thank You for the answer!
            $endgroup$
            – Mrigank Pawagi
            yesterday




            $begingroup$
            Thank You for the answer!
            $endgroup$
            – Mrigank Pawagi
            yesterday











            1












            $begingroup$

            You can see the effect of density change on refractive index due to heating of air. For a simple example, light a candle and look through the air column directly above the flame. The flame heats air which rises, but the flow is turbulent, so you'll see objects on the other side of the air column shimmer as the stream of hot air wavers from side to side.



            You can see this effect when you look across a paved surface on a hot sunny day.



            You won't see this effect with sound, at least not at typical listening levels because the density changes are too small (as noted in one of the other answers).






            share|cite|improve this answer









            $endgroup$












            • $begingroup$
              Thanks for the Answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday















            1












            $begingroup$

            You can see the effect of density change on refractive index due to heating of air. For a simple example, light a candle and look through the air column directly above the flame. The flame heats air which rises, but the flow is turbulent, so you'll see objects on the other side of the air column shimmer as the stream of hot air wavers from side to side.



            You can see this effect when you look across a paved surface on a hot sunny day.



            You won't see this effect with sound, at least not at typical listening levels because the density changes are too small (as noted in one of the other answers).






            share|cite|improve this answer









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            • $begingroup$
              Thanks for the Answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday













            1












            1








            1





            $begingroup$

            You can see the effect of density change on refractive index due to heating of air. For a simple example, light a candle and look through the air column directly above the flame. The flame heats air which rises, but the flow is turbulent, so you'll see objects on the other side of the air column shimmer as the stream of hot air wavers from side to side.



            You can see this effect when you look across a paved surface on a hot sunny day.



            You won't see this effect with sound, at least not at typical listening levels because the density changes are too small (as noted in one of the other answers).






            share|cite|improve this answer









            $endgroup$



            You can see the effect of density change on refractive index due to heating of air. For a simple example, light a candle and look through the air column directly above the flame. The flame heats air which rises, but the flow is turbulent, so you'll see objects on the other side of the air column shimmer as the stream of hot air wavers from side to side.



            You can see this effect when you look across a paved surface on a hot sunny day.



            You won't see this effect with sound, at least not at typical listening levels because the density changes are too small (as noted in one of the other answers).







            share|cite|improve this answer












            share|cite|improve this answer



            share|cite|improve this answer










            answered 2 days ago









            Anthony XAnthony X

            2,78611220




            2,78611220











            • $begingroup$
              Thanks for the Answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday
















            • $begingroup$
              Thanks for the Answer!
              $endgroup$
              – Mrigank Pawagi
              yesterday















            $begingroup$
            Thanks for the Answer!
            $endgroup$
            – Mrigank Pawagi
            yesterday




            $begingroup$
            Thanks for the Answer!
            $endgroup$
            – Mrigank Pawagi
            yesterday

















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