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The function \(y(x, t)=(15.0 \mathrm{~cm}) \cos (\pi x-15 \pi t)\), with \(x\) in meters and \(t\) in seconds, describes a wave on a taut string. What is the transverse speed for a point on the string at an instant when that point has the displacement \(y=+12.0 \mathrm{~cm}\) ?

Short Answer

Expert verified
The transverse speed at the point is approximately \(-424.115 \text{ cm/s}\).

Step by step solution

01

Understand the Problem

We are given a wave function \(y(x, t) = (15.0 \text{ cm}) \cos(\pi x - 15\pi t)\) and need to find the transverse speed \(\frac{\partial y}{\partial t}\) at a point where the displacement \(y = +12.0 \text{ cm}\). This involves finding how quickly the position of the wave on the string is changing at a specific point and time.
02

Differentiate the Wave Function

To find the transverse speed, differentiate the wave function \(y(x, t)\) with respect to time \(t\). The partial derivative is:\[\frac{\partial y}{\partial t} = -15 \pi \times 15.0 \text{ cm} \times \sin(\pi x - 15\pi t)\]This derivative gives the velocity of the wave, or the transverse speed of a point on the string.
03

Find the Angle Corresponding to Displacement

Since the cosine function \(y(x, t) = 15.0 \cos(\pi x - 15\pi t)\) needs to equal \(+12.0 \text{ cm}\), set up the equation:\[\cos(\pi x - 15\pi t) = \frac{12.0}{15.0} = 0.8\]Determine the angle using the inverse cosine function: \(\pi x - 15\pi t = \cos^{-1}(0.8)\).
04

Calculate the Transverse Speed Using the Angle

Substitute the angle back into the expression for the derivative:The angle \(\theta = \cos^{-1}(0.8)\) so \(\sin(\theta) = \sqrt{1-0.8^2} = \sin(\theta)\).Substitute into the velocity equation:\[\frac{\partial y}{\partial t} = -15\pi \times 15.0 \times \sqrt{1-0.8^2} = -15\pi \times 15.0 \times \sqrt{0.36}\]Compute the expression to get \(-15\pi \times 15.0 \times 0.6\).
05

Evaluate the Expression

Calculate the final expression for the transverse speed:\[\frac{\partial y}{\partial t} = -15\pi \times 15.0 \times 0.6 \]Where \(\pi \approx 3.1416\), substitute and solve to find the transverse speed.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Transverse Speed
In wave motion, the transverse speed represents the rate at which a point on a wave moves up and down, horizontally across a medium. This movement is perpendicular to the direction of wave propagation. To find the transverse speed of a wave described by the function \(y(x, t)=(15.0 \, \text{cm}) \cos (\pi x-15 \pi t)\), we need to take the derivative of this wave function with respect to time \(t\). The formula is simple to understand. Derivating the function with respect to \(t\) gives us the transverse speed:
  • \(\frac{\partial y}{\partial t} = -15 \pi \times 15.0 \, \text{cm} \times \sin(\pi x - 15\pi t)\),
which indicates how fast the point moves across time. The speed will be negative or positive depending on the direction of the movement.By understanding this concept, you can grasp how the speed is determined by oscillation within the wave, calculated using the partial derivative of the wave function.
Wave Equation
The wave equation is a cornerstone in physics, providing a mathematical description of how wave phenomena manifest in different mediums. In this context, the wave equation yields a pattern to describe a vibrating string. The general form of the wave equation for a stretched string is given by:
  • \(y(x, t) = A \cos(kx - \omega t)\)
where \(A\) stands for amplitude, \(k\) for wave number, and \(\omega\) for angular frequency.In the given problem, \(y(x, t) = (15.0 \, \text{cm}) \cos(\pi x - 15\pi t)\) represents a traveling wave where the maximum amplitude is 15.0 cm. The terms \(\pi x\) and \(15\pi t\) play crucial roles:
  • \(\pi\) signifies the wave number \(k\). It determines how many complete wave cycles fit into a given length.
  • \(15\pi\) links to \(\omega\), describing how quickly the wave oscillates over time.
The wave equation can be solved to find quantities such as maximum displacement, speed, or period of the wave.
Partial Derivatives
Partial derivatives are an essential tool in calculus, especially when dealing with functions of multiple variables. In the context of wave motion, they help us explore how wave functions change over space \(x\) and time \(t\).For the wave function \(y(x, t) = (15.0 \, \text{cm}) \cos(\pi x - 15\pi t)\), we calculate the following partial derivatives:
  • \(\frac{\partial y}{\partial x}\): This indicates how the wave displacement \(y\) changes with respect to position \(x\).
  • \(\frac{\partial y}{\partial t}\): This tells us how the wave displacement \(y\) changes over time, which is related to the transverse speed.
In this exercise, focusing on the partial derivative with respect to time provides insight into the wave's movement across the medium (transverse speed). Remember, a partial derivative hones in on how one variable changes while holding others constant, allowing a closer look at the dynamics involved.
Wave Function Analysis
Wave function analysis involves dissecting the wave equation to identify crucial characteristics like amplitude, frequency, period, wave speed, and more. For the function \(y(x, t)=(15.0 \, \text{cm}) \cos(\pi x-15 \pi t)\), let's break down each component:
  • Amplitude (A): The amplitude of the wave, here 15.0 cm, shows the maximum displacement from the equilibrium position.
  • Wave Number (k): Given by \(\pi\), it signifies the spatial frequency of the wave, indicating how many wavelengths fit into a unit distance.
  • Angular Frequency (\(\omega\)): Represented by \(15\pi\), it defines how fast the wave oscillates over time.
  • Phase (\(\theta\)): The term inside the cosine, \(\pi x - 15\pi t\), describes the phase of the wave, crucial in determining the wave's precise value at any point \((x, t)\).
Analyzing such a function is vital in understanding the behavior of waves, noting how changes in variables affect the wave's shape, speed, and direction.

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Most popular questions from this chapter

A sinusoidal wave of angular frequency \(1200 \mathrm{rad} / \mathrm{s}\) and amplitude \(3.00 \mathrm{~mm}\) is sent along a cord with linear density \(2.00 \mathrm{~g} / \mathrm{m}\) and tension \(1200 \mathrm{~N}\). (a) What is the average rate at which energy is transported by the wave to the opposite end of the cord? (b) If, simultaneously, an identical wave travels along an adjacent, identical cord, what is the total average rate at which energy is transported to the opposite ends of the two cords by the waves? If, instead, those two waves are sent along the same cord simultaneously, what is the total average rate at which they transport energy when their phase difference is (c) \(0,(\mathrm{~d}) 0.4 \pi \mathrm{rad}\), and \((\mathrm{e}) \pi \mathrm{rad} ?\)

What phase difference between two identical traveling waves, moving in the same direction along a stretched string, results in the combined wave having an amplitude \(1.50\) times that of the common amplitude of the two combining waves? Express your answer in (a) degrees, (b) radians, and (c) wavelengths.

The equation of a transverse wave traveling along a string is $$ y=0.15 \sin (0.79 x-13 t) $$ in which \(x\) and \(y\) are in meters and \(t\) is in seconds. (a) What is the displacement \(y\) at \(x=2.3 \mathrm{~m}, t=0.16 \mathrm{~s} ?\) A second wave is to be added to the first wave to produce standing waves on the string. If the second wave is of the form \(y(x, t)=y_{m} \sin (k x \pm \omega t)\), what are (b) \(y_{m},(\mathrm{c})\) \(k\), (d) \(\omega\), and (e) the correct choice of sign in front of \(\omega\) for this second wave? (f) What is the displacement of the resultant standing wave at \(x=2.3 \mathrm{~m}, t=0.16 \mathrm{~s}\) ?

If a transmission line in a cold climate collects ice, the increased diameter tends to cause vortex formation in a passing wind. The air pressure variations in the vortexes tend to cause the line to oscillate (gallop), especially if the frequency of the variations matches a resonant frequency of the line. In long lines, the resonant frequencies are so close that almost any wind speed can set up a resonant mode vigorous enough to pull down support towers or cause the line to short out with an adjacent line. If a transmission line has a length of \(347 \mathrm{~m}\), a linear density of \(3.35 \mathrm{~kg} / \mathrm{m}\), and a tension of \(65.2 \mathrm{MN}\), what are (a) the frequency of the fundamental mode and (b) the frequency difference between successive modes?

Use the wave equation to find the speed of a wave given by $$ y(x, t)=(3.00 \mathrm{~mm}) \sin \left[\left(4.00 \mathrm{~m}^{-1}\right) x-\left(7.00 \mathrm{~s}^{-1}\right) t\right] . $$

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