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sound waves ___ as they travel in the body
weaken, or attenuate
logarithm
represents the number of 10s that are multiplied to create the original number
decibel (dB)
common unit for measuring electrical signal strength and brightness of images
report relative changes
decibel notation
relative measurement
a comparison
a ratio
logarithmic
positive decibels
report signals that are increasing in strength, or getting larger
negative decibels
describe signals that are decreasing in strength, or getting smaller
3dB
double
10dB
ten times larger
-3dB
half
-10dB
one-tenth
attenuation
decrease in intensity, power, and amplitude as sound travels
attenuation is determined by:
path length
frequency of sound
more attenuation
longer distances
higher frequencies
less attenuation
shorter distances
lower frequencies
three processes that contribute to attenuation
reflection
scattering
absorption
reflection
weakens the portion of the sound wave that continues in the forward direction
two forms of reflection
specular
diffuse
specular reflection
when the boundary is smooth, the sound is reflected in only one direction in an organized manner
diffuse reflection (backscatter)
when a wave reflects off an irregular surface, it radiates in more than one directions
scattering
random redirection of sound in many directions
rayleigh scattering
occurs when a structure’s dimensions are much smaller than the beam’s wavelength
relationship between rayleigh scattering and frequency
rayleigh scattering is proportional to frequency^4
absorption
occurs when ultrasonic energy is converted into another energy form
attenuation coefficient
number of decibels of attenuation that occurs when sound travels one centimeter
Units: dB/cm
attenuation equation
total attenuation (dB) = atten. coefficient (dB/cm) x distance (cm)
attenuation coefficient equation
atten. coef. (dB/cm) = frequency (MHz)/2
atten. coef. = 0.5 dB/cm/MHz
half-value layer thickness
distance sound travels in a tissue that reduces the intensity of sound to ½ its original value
Units: cm
impedance
acoustic resistance to sound traveling in a medium
impedance equation
impedance = density x speed
normal incidence
the incident sound beam strikes the boundary at exactly 90 degrees
oblique incidence
incident sound beam strikes the boundary at any angle other than 90 degrees
incident intensity
the sound wave’s intensity immediately before it strikes a boundary
reflected intensity
intensity of the portion of the incident sound beam that after striking a boundary, returns back from where it came
transmitted intensity
intensity of the portion of the incident beam that after striking a boundary, continues forward in the same general direction that it was traveling