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Ultrasound Imaging. Sound having frequencies above the range of human hearing (about \(20,000 \mathrm{~Hz}\) ) is called ultrasound. Waves above this frequency can be used to penetrate the body and to produce images by reflecting from surfaces. In a typical ultrasound scan, the waves travel through body tissue with a speed of \(1500 \mathrm{~m} / \mathrm{s}\) For a good, detailed image, the wavelength should be no more than 1.0 \(\mathrm{mm} .\) What frequency sound is required for a good scan?

Short Answer

Expert verified
The frequency required for a good scan is \(1.5×10^6 Hz\).

Step by step solution

01

Convert the wavelength to meters

The wavelength given in the exercise is in millimeters, but the speed is given in meters per second, so the wavelength needs to be converted to meters in order to use this in the wave equation. 1 mm is equal to 0.001 m, so the wavelength is \(0.001 m\).
02

Solve the wave equation for frequency

The wave equation is \(v = f \lambda\). Solve this equation for \(f\) to find: \(f = v / \lambda\).
03

Insert values and calculate frequency

Now that we have the equation for the frequency, we can insert the values for the speed and the wavelength: \(f = 1500 m/s / 0.001 m = 1.5×10^6 Hz\).

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Key Concepts

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

Sound Frequency
Sound frequency is a key concept in understanding how different types of sound are classified. Simply put, frequency is the number of times a sound wave's cycle occurs in one second, measured in hertz (Hz). The human ear can typically hear frequencies between 20 Hz and 20,000 Hz. Frequencies below 20 Hz are known as infrasound, while those above 20,000 Hz are referred to as ultrasound.

When we delve into the realm of ultrasound, we encounter frequencies that are too high-pitched for the human ear to detect. However, these frequencies are incredibly useful in medical diagnostics, particularly in ultrasound imaging. The physics behind ultrasound imaging rely on these high-frequency sound waves to penetrate the body and reflect off organs and tissues, creating images that can be used for medical analysis.
Ultrasound Frequency
Ultrasound frequencies, which typically range from 1 million to 15 million Hz (1 MHz to 15 MHz), are much higher than what our ears can perceive. In the context of medical imaging, the exact frequency chosen for an ultrasound scan affects the image quality. Higher frequencies provide better resolution because they produce shorter wavelengths, allowing for more detailed images of small structures.

In the case of our exercise, finding the right ultrasound frequency necessitates a trade-off between resolution and penetration depth. Higher frequencies do not travel as far into the body as lower frequencies, leading to lesser imaging depth. Therefore, medical professionals have to select an ultrasound frequency that is high enough to provide clear images and yet can penetrate sufficiently to reach the areas of interest. For the purposes of a detailed image with a wavelength of 1 mm, a frequency in the megahertz range, such as 1.5 MHz, is typically used.
Wave Equation
The wave equation is a fundamental principle in physics, connecting the speed (\(v\)), frequency (\(f\)), and wavelength (\( \text{\lambda} \text{(lambda)} \text{)} \)) of any wave. Mathematically, it is expressed as \(v = f \text{\lambda} \). For sound waves, this equation becomes critically important, as it allows us to calculate one of the variables if the other two are known.

Using the wave equation, ultrasound frequencies necessary for medical diagnostics can be determined. As done in the exercise's solution, you can rearrange the equation to solve for frequency when you are given the speed of sound in a medium (like tissue) and the desired wavelength for imaging. In the medical context, precise calculations are crucial to ensure that the ultrasound waves produce the best possible images while maintaining safety standards for patient exposure.

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Most popular questions from this chapter

One end of a horizontal rope is attached to a prong of an electrically driven tuning fork that vibrates the rope transversely at \(120 \mathrm{~Hz}\). The other end passes over a pulley and supports a \(1.50 \mathrm{~kg}\) mass. The linear mass density of the rope is \(0.0480 \mathrm{~kg} / \mathrm{m} .\) (a) What is the speed of a transverse wave on the rope? (b) What is the wavelength? (c) How would your answers to parts (a) and (b) change if the mass were increased to \(3.00 \mathrm{~kg} ?\)

You are designing a two-string instrument with metal strings \(35.0 \mathrm{~cm}\) long, as shown in Fig. \(\mathrm{P} 15.52 .\) Both strings are under the same tension. String \(S_{1}\) has a mass of \(8.00 \mathrm{~g}\) and produces the note middle \(\mathrm{C}\) (frequency \(262 \mathrm{~Hz}\) ) in its fundamental mode. (a) What should be the tension in the string? (b) What should be the mass of string \(S_{2}\) so that it will produce A-sharp (frequency \(466 \mathrm{~Hz}\) ) as its fundamental? (c) To extend the range of your instrument, you include a fret located just under the strings but not normally touching them. How far from the upper end should you put this fret so that when you press \(S_{1}\) tightly against it, this string will produce \(\mathrm{C}\) -sharp (frequency \(277 \mathrm{~Hz}\) ) in its fundamental? That is, what is \(x\) in the figure? (d) If you press \(S_{2}\) against the fret, what frequency of sound will it produce in its fundamental?

The wave function of a standing wave is \(y(x, t)=(4.44 \mathrm{~mm})\) \(\sin [(32.5 \mathrm{rad} / \mathrm{m}) x] \sin [(754 \mathrm{rad} / \mathrm{s}) t] .\) For the two traveling waves that make up this standing wave, find the (a) amplitude; (b) wavelength; (c) frequency; (d) wave speed; (e) wave functions. (f) From the information given, can you determine which harmonic this is? Explain.

A transverse sine wave with an amplitude of \(2.50 \mathrm{~mm}\) and a wavelength of \(1.80 \mathrm{~m}\) travels from left to right along a long, horizontal, stretched string with a speed of \(36.0 \mathrm{~m} / \mathrm{s}\). Take the origin at the left end of the undisturbed string. At time \(t=0\) the left end of the string has its maximum upward displacement. (a) What are the frequency, angular frequency, and wave number of the wave? (b) What is the function \(y(x, t)\) that describes the wave? (c) What is \(y(t)\) for a particle at the left end of the string? (d) What is \(y(t)\) for a particle \(1.35 \mathrm{~m}\) to the right of the origin? (e) What is the maximum magnitude of transverse velocity of any particle of the string? (f) Find the transverse displacement and the transverse velocity of a particle \(1.35 \mathrm{~m}\) to the right of the origin at time \(t=0.0625 \mathrm{~s}\)

A rectangular neoprene sheet has width \(W=1.00 \mathrm{~m}\) and length \(L=4.00 \mathrm{~m}\). The two shorter edges are affixed to rigid steel bars that are used to stretch the sheet taut and horizontal. The force applied to either end of the sheet is \(F=81.0 \mathrm{~N}\). The sheet has a total mass \(M=4.00 \mathrm{~kg} .\) The left edge of the sheet is wiggled vertically in a uniform sinusoidal motion with amplitude \(A=10.0 \mathrm{~cm}\) and frequency \(f=1.00 \mathrm{~Hz}\). This sends waves spanning the width of the sheet rippling from left to right. The right side of the sheet moves upward and downward freely as these waves complete their traversal. (a) Use a twodimensional generalization of the discussion in Section 15.4 to derive an expression for the velocity with which the waves move along the sheet in terms of generic values of \(W, L, F, M, f,\) and \(A .\) What is the value of this speed for the specified choices of these parameters? (b) If the positive \(x\) -axis is oriented rightward and the steel bars are parallel to the \(y\) -axis, the height of the sheet may be characterized as \(z(x, y)=A \sin (k x-\omega t)\) What is the value of the wave number \(k ?\) (c) Write down an expression with generic parameters for the rate of rightward energy transfer by the slice of sheet at a given value of \(x\) at generic time \(t\). (d) The power at \(x=0\) is supplied by the agent wiggling the left bar upward and downward. How much energy is supplied each second by that agent? Express your answer in terms of generic parameters and also as a specific energy for the given parameters.

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