A sinusoidal wave traveling on a string is moving in the positive \(x\) -direction. The wave has a wavelength of \(4 \mathrm{~m}, \mathrm{a}\) frequency of \(50.0 \mathrm{~Hz},\) and an amplitude of \(3.00 \mathrm{~cm} .\) What is the wave function for this wave?

Short Answer

Expert verified
Answer: The wave function for the sinusoidal wave is given by: \(y(x,t) = (3.00\,\mathrm{cm})\sin\left(\displaystyle\frac{\pi}{2} x - 100\pi t\right)\)

Step by step solution

01

Calculate wave number k

Using the given wavelength \(\lambda = 4\,m\), we can calculate the wave number k: \(k = \displaystyle\frac{2\pi}{\lambda}\) Plug in the value of \(\lambda\) to find k: \(k = \displaystyle\frac{2\pi}{4} = \displaystyle\frac{\pi}{2}\,\mathrm{m^{-1}}\)
02

Calculate angular frequency \(\omega\)

Using the given frequency \(f = 50.0\,Hz\), we can calculate the angular frequency \(\omega\): \(\omega = 2\pi f\) Plug in the value of f to find \(\omega\): \(\omega = 2\pi \cdot 50.0 = 100\pi\,\mathrm{rad/s}\)
03

Write the wave function

Now we have all the necessary values to write the wave function. The wave is traveling in the positive x-direction, so the wave function will have the form: \(y(x,t) = A\sin(kx - \omega t + \phi)\) Plug in the values of A, k, and \(\omega\). For simplicity, we assume the phase constant \(\phi = 0\): \(y(x,t) = (3.00\,\mathrm{cm})\sin\left(\displaystyle\frac{\pi}{2} x - 100\pi t\right)\) Our final wave function is: \(y(x,t) = (3.00\,\mathrm{cm})\sin\left(\displaystyle\frac{\pi}{2} x - 100\pi t\right)\)

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Key Concepts

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

Understanding Sinusoidal Waves
A sinusoidal wave is a smooth, periodic oscillation that is mathematically described by the sine or cosine function. Imagine it like the ebb and flow of ocean waves, where each wave crest and trough follows a smooth and regular pattern. These waves can exist in various mediums, such as strings, air (as sound), or even the surface of water.

The defining properties of any sinusoidal wave include amplitude, wavelength, frequency, and phase. The amplitude (\( A \) in the equation) is the height of the wave crests, which represents the maximum displacement of the wave from its equilibrium position. In the context of the exercise, the amplitude of the wave is given as 3.00 cm.

Sinusoidal waves are fundamental to our understanding of a variety of physical phenomena, especially in the fields of acoustics, optics, and electromagnetism. They're also essential in our daily lives, from the music we enjoy to the wireless communications we rely on.
Wavelength and Frequency Relationship
The wavelength and frequency of a wave are inversely related to each other. Wavelength, often denoted by \( \lambda \) for sinusoidal waves, is the distance between two consecutive points that are in phase, such as two successive crests or troughs. It informs us about the spatial period of the wave—the greater the wavelength, the more stretched out the wave is.

Frequency (denoted by \( f \)), on the other hand, is the number of wave crests that pass a given point in one second and is measured in hertz (Hz). The frequency tells us about how quickly the wave oscillates. As per the exercise information, our wave has a wavelength of 4 meters and a frequency of 50.0 Hz. These two values are connected by the simple equation \( c = \lambda f \), where \( c \) is the speed of the wave.

Understanding this relationship helps to predict how a wave will behave when it enters a different medium or interacts with various objects, which is valuable in designing wave-related technology such as musical instruments, radio transmitters, and even sonographic equipment.
What is Angular Frequency?
The angular frequency (represented by \( \omega \) in our equations) is a measure of how fast something rotates or revolves, relating to waves as to how quickly their cycles are completed. It's expressed in radians per second (rad/s) and is calculated as \( \omega = 2\pi f \). This quantity can be thought of as the 'speed' of the wave's oscillation, from a circular motion perspective.

In the step-by-step solution provided, the angular frequency was found by multiplying the standard frequency by \( 2\pi \) yielding \( 100\pi \) rad/s. This value signifies that the wave completes \( 50 \) oscillations (or cycles) each second, and at each oscillation, the point on the wave traces out a path that covers \( 2\pi \) radians.

Angular frequency is particularly useful in electrical engineering for understanding alternating currents and in mechanical systems that involve rotations or vibrations, such as engines or oscillating circuits.

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Most popular questions from this chapter

What is the wave speed along a brass wire with a radius of \(0.500 \mathrm{~mm}\) stretched at a tension of \(125 \mathrm{~N}\) ? The density of brass is \(8.60 \cdot 10^{3} \mathrm{~kg} / \mathrm{m}^{3}\).

A traveling wave propagating on a string is described by the following equation: $$ y(x, t)=(5.00 \mathrm{~mm}) \sin \left(\left(157.08 \mathrm{~m}^{-1}\right) x-\left(314.16 \mathrm{~s}^{-1}\right) t+0.7854\right) $$ a) Determine the minimum separation, \(\Delta x_{\min }\), between two points on the string that oscillate in perfect opposition of phases (move in opposite directions at all times). b) Determine the separation, \(\Delta x_{A B}\), between two points \(A\) and \(B\) on the string, if point \(B\) oscillates with a phase difference of 0.7854 rad compared to point \(A\). c) Find the number of crests of the wave that pass through point \(A\) in a time interval \(\Delta t=10.0 \mathrm{~s}\) and the number of troughs that pass through point \(B\) in the same interval. d) At what point along its trajectory should a linear driver connected to one end of the string at \(x=0\) start its oscillation to generate this sinusoidal traveling wave on the string?

Consider a linear array of \(n\) masses, each equal to \(m,\) connected by \(n+1\) springs, all massless and having spring constant \(k\), with the outer ends of the first and last springs fixed. The masses can move without friction in the linear dimension of the array. a) Write the equations of motion for the masses. b) Configurations of motion for which all parts of a system oscillate with the same angular frequency are called normal modes of the system; the corresponding angular frequencies are the system's normal-mode angular frequencies. Find the normal-mode angular frequencies of this array.

Write the equation for a sinusoidal wave propagating in the negative \(x\) -direction with a speed of \(120 . \mathrm{m} / \mathrm{s}\), if a particle in the medium in which the wave is moving is observed to swing back and forth through a \(6.00-\mathrm{cm}\) range in \(4.00 \mathrm{~s}\). Assume that \(t=0\) is taken to be the instant when the particle is at \(y=0\) and that the particle moves in the positive \(y\) -direction immediately after \(t=0\).

The different colors of light we perceive are a result of the varying frequencies (and wavelengths) of the electromagnetic radiation. Infrared radiation has lower frequencies than does visible light, and ultraviolet radiation has higher frequencies than visible light does. The primary colors are red (R), yellow (Y), and blue (B). Order these colors by their wavelength, shortest to longest. a) \(\mathrm{B}, \mathrm{Y}, \mathrm{R}\) b) \(B, R, Y\) c) \(\mathrm{R}, \mathrm{Y}, \mathrm{B}\) d) \(R, B, Y\)

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