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Write down the equation of a progressive wave that superimposes the above to form a stationary wave and determine the equation of the resultant stationary wave and state the amplitude.

Physics

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4 parts
i

y2=20sin⁡(300πt+πx15)y_2 = 20 \sin \left(300\pi t + \frac{\pi x}{15}\right)

ii

y=40cos⁡(πx15)sin⁡(300πt)y = 40 \cos\left(\frac{\pi x}{15}\right) \sin\left(300\pi t\right)

40 cm40 \text{ cm}

iii

30 cm30 \text{ cm}

iv

π6 radians\frac{\pi}{6} \text{ radians}

Step-by-step solution

9 steps

Here's the solution to your wave problem:

The given progressive wave equation is y=20sin⁡(300πt−πx15)y = 20 \sin \left(300\pi t - \frac{\pi x}{15}\right), where tt is in seconds and xx is in cm.
Comparing this to the standard wave equation y=Asin⁡(ωt−kx)y = A \sin(\omega t - kx), we have:
Amplitude A=20A = 20 cm
Angular frequency ω=300π\omega = 300\pi rad/s
Wave number k=π15k = \frac{\pi}{15} rad/cm

Part i· 2 steps

Write down the equation of a progressive wave that superimposes the above to form a stationary wave.

A stationary wave is formed by two identical progressive waves traveling in opposite directions. If the first wave is y1=Asin⁡(ωt−kx)y_1 = A \sin(\omega t - kx), the second wave traveling in the opposite direction will be y2=Asin⁡(ωt+kx)y_2 = A \sin(\omega t + kx).

  1. Identify the parameters from the given wave.

    From y1=20sin⁡(300πt−πx15)y_1 = 20 \sin \left(300\pi t - \frac{\pi x}{15}\right), we have A=20A = 20, ω=300π\omega = 300\pi, and k=π15k = \frac{\pi}{15}.

  2. Write the equation for the second progressive wave.

    The equation for the progressive wave traveling in the opposite direction is:

    y2=20sin⁡(300πt+πx15)y_2 = 20 \sin \left(300\pi t + \frac{\pi x}{15}\right)

    The equation of the progressive wave is y2=20sin⁡(300πt+πx15)\boxed{y_2 = 20 \sin \left(300\pi t + \frac{\pi x}{15}\right)}.

Part ii

y=40cos⁡(πx15)sin⁡(300πt)y = 40 \cos\left(\frac{\pi x}{15}\right) \sin\left(300\pi t\right)

Using the given progressive wave equation and the equation within (i) above, determine the equation of the resultant stationary wave and state the amplitude.

The resultant stationary wave is the superposition of the two progressive waves: y=y1+y2y = y_1 + y_2.

y=20sin⁡(300πt−πx15)+20sin⁡(300πt+πx15)y = 20 \sin \left(300\pi t - \frac{\pi x}{15}\right) + 20 \sin \left(300\pi t + \frac{\pi x}{15}\right)
  1. Apply the trigonometric identity sin⁡A+sin⁡B=2sin⁡(A+B2)cos⁡(A−B2)\sin A + \sin B = 2 \sin\left(\frac{A+B}{2}\right) \cos\left(\frac{A-B}{2}\right).

    Let A=300πt+πx15A = 300\pi t + \frac{\pi x}{15} and B=300πt−πx15B = 300\pi t - \frac{\pi x}{15}.

    A+B2=(300πt+πx15)+(300πt−πx15)2=600πt2=300πt\frac{A+B}{2} = \frac{\left(300\pi t + \frac{\pi x}{15}\right) + \left(300\pi t - \frac{\pi x}{15}\right)}{2} = \frac{600\pi t}{2} = 300\pi t A−B2=(300πt+πx15)−(300πt−πx15)2=2(πx15)2=πx15\frac{A-B}{2} = \frac{\left(300\pi t + \frac{\pi x}{15}\right) - \left(300\pi t - \frac{\pi x}{15}\right)}{2} = \frac{2 \left(\frac{\pi x}{15}\right)}{2} = \frac{\pi x}{15}
  2. Substitute these into the identity.

    y=20[2sin⁡(300πt)cos⁡(πx15)]y = 20 \left[2 \sin\left(300\pi t\right) \cos\left(\frac{\pi x}{15}\right)\right] y=40cos⁡(πx15)sin⁡(300πt)y = 40 \cos\left(\frac{\pi x}{15}\right) \sin\left(300\pi t\right)
  3. State the amplitude of the stationary wave.

    The amplitude of the stationary wave is given by the term multiplying sin⁡(300πt)\sin(300\pi t), which is 40cos⁡(πx15)40 \cos\left(\frac{\pi x}{15}\right). The maximum amplitude occurs when cos⁡(πx15)=±1\cos\left(\frac{\pi x}{15}\right) = \pm 1.
    The maximum amplitude of the stationary wave is 40 cm.
    The equation of the resultant stationary wave is y=40cos⁡(πx15)sin⁡(300πt)\boxed{y = 40 \cos\left(\frac{\pi x}{15}\right) \sin\left(300\pi t\right)}.
    The maximum amplitude of the stationary wave is 40 cm\boxed{40 \text{ cm}}.

Part iii

30 cm30 \text{ cm}

Calculate the wavelength of a stationary wave.

The wavelength of a stationary wave is the same as the wavelength of the progressive waves that form it. We can find the wavelength from the wave number kk.

  1. Use the relationship between wave number and wavelength.

    The wave number k=2πλk = \frac{2\pi}{\lambda}. From the given equation, k=π15k = \frac{\pi}{15} rad/cm.

  2. Calculate the wavelength λ\lambda.

    2πλ=π15\frac{2\pi}{\lambda} = \frac{\pi}{15} λ=2ππ/15=2×15=30 cm\lambda = \frac{2\pi}{\pi/15} = 2 \times 15 = 30 \text{ cm}

    The wavelength of the stationary wave is 30 cm\boxed{30 \text{ cm}}.

Part iv

π6 radians\frac{\pi}{6} \text{ radians}

Determine the phase difference between two points of a progressive wave separated by 2.5 cm.

The phase difference Δϕ\Delta \phi between two points separated by a distance Δx\Delta x in a progressive wave is given by Δϕ=kΔx\Delta \phi = k \Delta x.

  1. Identify the wave number kk and the separation Δx\Delta x.

    From the given wave equation, k=π15k = \frac{\pi}{15} rad/cm.
    The separation Δx=2.5\Delta x = 2.5 cm.

  2. Calculate the phase difference.

    Δϕ=kΔx=(π15 rad/cm)×(2.5 cm)\Delta \phi = k \Delta x = \left(\frac{\pi}{15} \text{ rad/cm}\right) \times (2.5 \text{ cm}) Δϕ=π15×52=5π30=π6 radians\Delta \phi = \frac{\pi}{15} \times \frac{5}{2} = \frac{5\pi}{30} = \frac{\pi}{6} \text{ radians}

    The phase difference is π6 radians\boxed{\frac{\pi}{6} \text{ radians}}.

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