Home
Class 11
PHYSICS
Equations of a stationary and a travelli...

Equations of a stationary and a travelling waves are as follows `y_(1) = sin kx cos omega t` and `y_(2) = a sin ( omega t - kx)`. The phase difference between two points `x_(1) = pi//3k` and `x_(2) = 3 pi// 2k is phi_(1)` in the standing wave `(y_(1))` and is `phi_(2)` in the travelling wave `(y_(2))` then ratio `phi_(1)//phi_(2)` is

A

`1`

B

`5//6`

C

`3//4`

D

`6//7`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the phase difference between two points in a stationary wave and a traveling wave, and then calculate the ratio of these phase differences. ### Step 1: Identify the wave equations The stationary wave is given by: \[ y_1 = \sin(kx) \cos(\omega t) \] The traveling wave is given by: \[ y_2 = a \sin(\omega t - kx) \] ### Step 2: Determine the positions We have two positions: - \( x_1 = \frac{\pi}{3k} \) - \( x_2 = \frac{3\pi}{2k} \) ### Step 3: Calculate the phase difference in the stationary wave (\( \phi_1 \)) For the stationary wave, the phase at \( x_1 \) is: \[ \phi_1(x_1) = kx_1 = k \left(\frac{\pi}{3k}\right) = \frac{\pi}{3} \] For the stationary wave at \( x_2 \): \[ \phi_1(x_2) = kx_2 = k \left(\frac{3\pi}{2k}\right) = \frac{3\pi}{2} \] Now, the phase difference \( \phi_1 \) between these two points in the stationary wave is: \[ \phi_1 = \phi_1(x_2) - \phi_1(x_1) = \frac{3\pi}{2} - \frac{\pi}{3} \] To subtract these fractions, we need a common denominator: - The common denominator of 2 and 3 is 6. Converting the fractions: \[ \frac{3\pi}{2} = \frac{9\pi}{6} \] \[ \frac{\pi}{3} = \frac{2\pi}{6} \] Now, substituting back: \[ \phi_1 = \frac{9\pi}{6} - \frac{2\pi}{6} = \frac{7\pi}{6} \] ### Step 4: Calculate the phase difference in the traveling wave (\( \phi_2 \)) For the traveling wave, the phase difference \( \phi_2 \) is given by: \[ \phi_2 = k \Delta x \] where \( \Delta x = x_2 - x_1 \). Calculating \( \Delta x \): \[ \Delta x = \frac{3\pi}{2k} - \frac{\pi}{3k} \] Finding a common denominator (which is 6k): \[ \Delta x = \frac{9\pi}{6k} - \frac{2\pi}{6k} = \frac{7\pi}{6k} \] Now substituting into the phase difference formula: \[ \phi_2 = k \Delta x = k \left(\frac{7\pi}{6k}\right) = \frac{7\pi}{6} \] ### Step 5: Calculate the ratio \( \frac{\phi_1}{\phi_2} \) Now we can find the ratio of the phase differences: \[ \frac{\phi_1}{\phi_2} = \frac{\frac{7\pi}{6}}{\frac{7\pi}{6}} = 1 \] ### Final Answer The ratio \( \frac{\phi_1}{\phi_2} \) is: \[ \frac{\phi_1}{\phi_2} = 1 \] ---

To solve the problem, we need to find the phase difference between two points in a stationary wave and a traveling wave, and then calculate the ratio of these phase differences. ### Step 1: Identify the wave equations The stationary wave is given by: \[ y_1 = \sin(kx) \cos(\omega t) \] The traveling wave is given by: \[ y_2 = a \sin(\omega t - kx) \] ...
Promotional Banner

Topper's Solved these Questions

  • SUPERPOSITION AND STANDING WAVES

    CENGAGE PHYSICS|Exercise Multiple|26 Videos
  • SUPERPOSITION AND STANDING WAVES

    CENGAGE PHYSICS|Exercise Assertion - Reasoning|6 Videos
  • SUPERPOSITION AND STANDING WAVES

    CENGAGE PHYSICS|Exercise Subjective|24 Videos
  • SOUND WAVES AND DOPPLER EFFECT

    CENGAGE PHYSICS|Exercise Integer|16 Videos
  • THERMODYNAMICS

    CENGAGE PHYSICS|Exercise 24|1 Videos

Similar Questions

Explore conceptually related problems

Two waves are given by y_(1) = a sin (omega t - kx) and y_(2) = a cos (omega t - kx) . The phase difference between the two waves is

Equations of a stationery and a travelling waves are y_(1)=a sin kx cos omegat and y_(2)=a sin (omegat-kx) The phase differences between two between x_(1)=(pi)/(3k) and x_(2)=(3pi)/(2k) are phi_(1) and phi_(2) respectvely for the two waves. The ratio (phi_(1))/(phi_(2)) is

Two waves are given by y_(1)=asin(omegat-kx) and y_(2)=a cos(omegat-kx) . The phase difference between the two waves is -

y_1 =4sin( omega t + kx), y2 = -4 cos( omega t + kx), the phase difference is

Two waves are represented by Y_1=a_1 cos (omegat-kx) and Y-2 =a_2 sin (omegat-kx+pi//3) Then the phase difference between them is-

Two waves are represented by y_(1)=a_(1)cos (omega t - kx) and y_(2)=a_(2)sin (omega t - kx + pi//3) Then the phase difference between them is-

Two light waves are represented by y_(1)=a sin_(omega)t and y_(2)= a sin(omega t+delta) . The phase of the resultant wave is

Two wave are represented by equation y_(1) = a sin omega t and y_(2) = a cos omega t the first wave :-

The equation of a travelling and stationary waves are y_1=asin(omegat-kx) and y_2=asinkxcosomegat . The phase difference between two points x_1=(pi)/(4k) and (4pi)/(3k) are phi_1 and phi_2 respectively for two waves, where k is the wave number. The ratio phi_(1)//phi_(2)

CENGAGE PHYSICS-SUPERPOSITION AND STANDING WAVES-Single Correct
  1. A 100 - m long rod of density 10.0 xx 10^(4) kg//m^(3) and having Youn...

    Text Solution

    |

  2. Figure 7.88 shows a stretched string of length L and pipes of length L...

    Text Solution

    |

  3. Equations of a stationary and a travelling waves are as follows y(1) =...

    Text Solution

    |

  4. In the resonance tube experiment , the first resonance is heard when l...

    Text Solution

    |

  5. Microwaves from a transmitter are directed normally toward a plane ref...

    Text Solution

    |

  6. A man standing in front of a mountain beats a drum at regular interval...

    Text Solution

    |

  7. Let the two waves y(1) = A sin ( kx - omega t) and y(2) = A sin ( kx +...

    Text Solution

    |

  8. A standing wave on a string is given by y = ( 4 cm) cos [ x pi] sin [ ...

    Text Solution

    |

  9. If the velocity of sound in air is 320 m//s, then the maximum and mini...

    Text Solution

    |

  10. Mark out the correct statement(s) regarding waves.

    Text Solution

    |

  11. A harmonic wave is travelling on a stretched string . At any particula...

    Text Solution

    |

  12. Two strings , one thick and other thin are connected as shown in Fig. ...

    Text Solution

    |

  13. A string fixed at both ends whose fundamental frequency is 240 Hz is ...

    Text Solution

    |

  14. If a string fixed at both ends having fundamental frequency of 240 Hz ...

    Text Solution

    |

  15. A string of length 0.4 m and mass 10^(-2) kg is clamped at one end . T...

    Text Solution

    |

  16. A strain of sound waves is propagated along an organ pipe and gets ref...

    Text Solution

    |

  17. An ideal organ pipe resonates at successive frequencies of 50 Hz , 150...

    Text Solution

    |

  18. A source of sound attached to the bob of a simple pendulum execute SHM...

    Text Solution

    |

  19. A standing wave arises on a string when two waves of equal amplitude ,...

    Text Solution

    |

  20. Two tunig forks of frequency 250Hz and 256Hz produce beats. If a maxim...

    Text Solution

    |