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Diagnostic ultrasound of frequency \(4.50 \mathrm{MHz}\) is used to examine tumors in soft tissue. (a) What is the wavelength in air of such a sound wave? (b) If the speed of sound in tissue is \(1500 \mathrm{~m} / \mathrm{s}\), what is the wavelength of this wave in tissue?

Short Answer

Expert verified
(a) Wavelength in air: \( 7.62 \times 10^{-5} \, \mathrm{m} \); (b) Wavelength in tissue: \( 3.33 \times 10^{-4} \, \mathrm{m} \).

Step by step solution

01

Identify Given Values for Air

We are given the frequency of the ultrasound wave as \( f = 4.50 \, \mathrm{MHz} \). To find the wavelength in air, we will use the speed of sound in air, \( v_{\text{air}} = 343 \, \mathrm{m/s} \).
02

Calculate Wavelength in Air

The wavelength \( \lambda \) of a wave is given by the formula \( \lambda = \frac{v}{f} \), where \( v \) is the speed of sound and \( f \) is the frequency. Substituting the values for air:\[\lambda_{\text{air}} = \frac{343 \, \mathrm{m/s}}{4.50 \times 10^6 \, \mathrm{Hz}} = 7.62 \times 10^{-5} \, \mathrm{m}\]
03

Identify Given Values for Tissue

The speed of sound in tissue is given as \( v_{\text{tissue}} = 1500 \, \mathrm{m/s} \). We will use this to calculate the wavelength in tissue using the same frequency \( f = 4.50 \, \mathrm{MHz} \).
04

Calculate Wavelength in Tissue

Using the formula for wavelength \( \lambda = \frac{v}{f} \) again, but substituting the values for tissue:\[\lambda_{\text{tissue}} = \frac{1500 \, \mathrm{m/s}}{4.50 \times 10^6 \, \mathrm{Hz}} = 3.33 \times 10^{-4} \, \mathrm{m}\]

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Key Concepts

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

Ultrasound
Ultrasound refers to sound waves with a frequency higher than the upper audible limit of human hearing. While humans can typically hear sounds between 20 Hz and 20 kHz, ultrasound waves have frequencies above 20 kHz. For medical diagnostics, such as examining tumors or other internal body structures, ultrasound typically falls within the range of 1 to 15 MHz.

The high frequency of ultrasound waves allows them to produce detailed images of structures within the body. This is because higher frequencies can provide images with better resolution, making them essential for tasks like examining tissue.
  • Non-invasive: Used extensively in medical imaging without the need for surgical procedures.
  • Safe: Does not use ionizing radiation like X-rays, reducing potential harm.
  • Versatile: Capable of providing images of various types of soft tissue - from organs to tumors.
Wavelength
The wavelength of a sound wave is the distance between successive points of the wave with the same phase, such as crest to crest or trough to trough. It is inversely related to frequency, meaning as frequency increases, wavelength decreases.

In the equation for wavelength \( \lambda = \frac{v}{f} \) the variables are:
  • \(\lambda\): wavelength
  • \(v\): speed of sound in the medium
  • \(f\): frequency of the wave
Higher frequency waves will have shorter wavelengths, while lower frequency waves will have longer wavelengths. This relationship is crucial in contexts like ultrasound imaging, where the wavelength determines how sharp or detailed the produced images will be. For ultrasound in air and tissue, we see different wavelengths due to varying speeds of sound in these mediums.
Speed of Sound
The speed of sound is how quickly sound waves move through a medium. This speed can vary significantly based on the medium's properties such as density and elasticity. In the air, the speed of sound is approximately 343 m/s at room temperature, while in more dense media like tissue, it is generally faster, around 1500 m/s.

Factors influencing the speed of sound include:
  • Temperature: Higher temperatures generally increase speed due to more energetic particles causing faster transmission.
  • Medium Density: Typically, sound travels faster in liquids and solids compared to gases.
  • Elasticity of the Medium: More elastic materials allow sound to bounce back and forth, increasing speed.
In medical ultrasound, knowing the speed of sound in various tissues is crucial for accurately calculating wavelengths, which affects the clarity and quality of the diagnostic images.
Frequency
Frequency is a fundamental concept when discussing sound waves, referring to the number of times a wave's cycle repeats per second. Higher frequency means more cycles per second and is measured in Hertz (Hz). In ultrasound, frequencies usually are in the megahertz (MHz) range, making the waves inaudible to humans but perfect for medical imaging.

The frequency of a wave is closely tied to its wavelength and the speed of sound via the relationship: \( f = \frac{v}{\lambda} \) where:
  • \(f\): frequency
  • \(v\): speed of sound
  • \(\lambda\): wavelength
High-frequency ultrasound waves are ideal for detecting small details and providing higher resolution images, which is why they are heavily relied upon in medical diagnostics. The manipulation of frequency can make use of different modalities, providing either broader overviews or focusing on fine details within tissues.

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Most popular questions from this chapter

A sound source sends a sinusoidal sound wave of angular frequency \(3000 \mathrm{rad} / \mathrm{s}\) and amplitude \(12.0 \mathrm{nm}\) through a tube of air. The internal radius of the tube is \(2.00 \mathrm{~cm} .\) (a) What is the average rate at which energy (the sum of the kinetic and potential energies) is transported to the opposite end of the tube? (b) If, simultaneously, an identical wave travels along an adjacent, identical tube, what is the total average rate at which energy is transported to the opposite ends of the two tubes by the waves? If, instead, those two waves are sent along the same tube simultaneously, what is the total average rate at which they transport energy when their phase difference is (c) \(0,\) (d) \(0.40 \pi\) rad, and (e) \(\pi\) rad?

When you "crack" a knuckle, you suddenly widen the knuckle cavity, allowing more volume for the synovial fluid inside it and causing a gas bubble suddenly to appear in the fluid. The sudden production of the bubble, called "cavitation," produces a sound pulse \(-\) the cracking sound. Assume that the sound is transmitted uniformly in all directions and that it fully passes from the knuckle interior to the outside. If the pulse has a sound level of \(62 \mathrm{~dB}\) at your ear, estimate the rate at which energy is produced by the cavitation.

A detector initially moves at constant velocity directly toward a stationary sound source and then (after passing it) directly from it. The emitted frequency is \(f\). During the approach the detected frequency is \(f_{\text {app }}^{\prime}\) and during the recession it is \(f_{\text {rec }}^{\prime}\). If the frequencies are related by \(\left(f_{\text {app }}^{\prime}-f_{\text {rec }}^{\prime}\right) / f=0.500,\) what is the ratio \(v_{D} / v\) of the speed of the detector to the speed of sound?

Pipe \(A,\) which is \(1.20 \mathrm{~m}\) long and open at both ends, oscillates at its third lowest harmonic frequency. It is filled with air for which the speed of sound is \(343 \mathrm{~m} / \mathrm{s}\). Pipe \(B,\) which is closed at one end, oscillates at its second lowest harmonic frequency. This frequency of \(B\) happens to match the frequency of \(A .\) An \(x\) axis extends along the interior of \(B,\) with \(x=0\) at the closed end. (a) How many nodes are along that axis? What are the (b) smallest and (c) second smallest value of \(x\) locating those nodes? (d) What is the fundamental frequency of \(B ?\)

A state trooper chases a speeder along a straight road; both vehicles move at \(160 \mathrm{~km} / \mathrm{h}\). The siren on the trooper's vehicle produces sound at a frequency of \(500 \mathrm{~Hz}\). What is the Doppler shift in the frequency heard by the speeder?

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