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5至100兆赫频率范围内湿密质奶牛股骨中的声速与衰减

Sonic velocity and attenuation in wet compact cow femur for the frequency range 5 to 100 MHz.

作者信息

Lees S, Klopholz D Z

机构信息

Bioengineering Department, Forsyth Dental Center, Boston, MA 02115.

出版信息

Ultrasound Med Biol. 1992;18(3):303-8. doi: 10.1016/0301-5629(92)90099-v.

DOI:10.1016/0301-5629(92)90099-v
PMID:1595136
Abstract

Ultrasonic studies on bone have not been done as intensively as other tissues, probably because there is less opportunity to examine bone in vivo by this modality. There is considerable interest in using ultrasonics to learn about the material properties of bone for which purpose the sonic spectrum may be useful. The longitudinal sonic velocity and attenuation have been found for several sections from one sample of wet cow femur for both the axial and radial directions over the frequency range of 5 to 100 MHz. The basic technique was solid-to-solid contact using a fused quartz buffer rod coupled to the bone specimen. There is clear evidence of velocity dispersion which Lakes et al. (1986) did not find over a frequency range up to 16 MHz. While there seems to be a peak in both velocity and attenuation at 70 MHz, it is necessary to obtain measurements at higher frequencies to make sure this is not an artifact. The axial sonic velocity varied from 4.29 km/s at 5 MHz to 4.447 km/s at 50 MHz, while the radial velocity was 3.45 km/s at 5 MHz and increased to 3.62 km/s at 50 MHz. The attenuation coefficient axially started at a mean value of 3.5 db/mm at 5 MHz and increased to a mean of 19 db/mm at 100 MHz. The corresponding radial attenuation coefficients are 5.2 and 26, respectively.

摘要

对骨骼的超声研究不像对其他组织那样深入,这可能是因为通过这种方式在体内检查骨骼的机会较少。人们对利用超声来了解骨骼的材料特性有着浓厚的兴趣,为此声谱可能会有所帮助。在5至100兆赫的频率范围内,对一个湿奶牛股骨样本的几个部分在轴向和径向上的纵向声速和衰减进行了测量。基本技术是使用与骨标本耦合的熔融石英缓冲棒进行固体与固体接触。有明确的证据表明存在速度色散,而莱克斯等人(1986年)在高达16兆赫的频率范围内并未发现这一现象。虽然在70兆赫时速度和衰减似乎都有一个峰值,但有必要在更高频率下进行测量,以确保这不是一种假象。轴向声速在5兆赫时为4.29千米/秒,在50兆赫时为4.447千米/秒,而径向速度在5兆赫时为3.45千米/秒,在50兆赫时增加到3.62千米/秒。轴向衰减系数在5兆赫时的平均值为3.5分贝/毫米,在100兆赫时增加到平均值19分贝/毫米。相应的径向衰减系数分别为5.2和26。

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