Acoustic impedance changes in cartilage and subchondral bone due to primary arthrosis

This study aimed at assessing elastic changes of cartilage and subchondral bone in sections from osteoarthritic human tibia plateaus using a 50-MHz scanning acoustic microscope (SAM). Samples were obtained from 28 human individuals during alloplastic implant surgery. Sagittal sections were explored using a time-resolved acoustic microscope in hyperosmolar (2.5 molar) saline solution at 25 degrees C. Cartilage and bone impedance distributions were evaluated as a function of the distance to the cartilage-bone interface. The degree of cartilage degeneration was derived from histological and immunohistochemical analyses. The mean impedance value in cartilage was 2.12+/-0.02 Mrayl. The layered cartilage structure was revealed by means of distinctly different impedance values in most samples. Generally, values were higher close to the bone interface and decreased continuously towards the cartilage surface. Higher grades of degeneration show a loss of the layered structure and remarkable cartilage surface undulations. The mean impedance value in subchondral bone was 6.28+/-0.54 Mrayl. A significant increase of the acoustic impedance within the first 150 microm relative to cartilage-bone interface was observed in 65.5% of the investigated sections. We hypothesize that the impedance increase close to the bone cartilage boundary is an indicator for subchondral sclerosis.     

A combined analysis and magnetic resonance imaging technique for computerised automatic measurement of cartilage thickness in the distal interphalangeal joint

It is well known that magnetic resonance imaging (MRI) contrast can be controlled, albeit sometimes at the expense of image resolution and signal-to-noise ratio, and most studies of articular joints have used a single MRI protocol, which is optimised for subjective image analysis. Inevitably that single protocol frequently compromises the detection of one or another of the boundaries between which any measurement must be made. This paper describes an alternative approach in which the criteria for computerised edge detection necessary for fully automated measurement of cartilage thickness are used to define the MRI acquisition parameters. This necessitates the combined use of two MRI sequences, one optimised for the cartilage-bone boundary, and the other for cartilage-synovial fluid. This provides a highly effective combination and its efficacy is demonstrated for the distal interphalangeal joint of a range of asymptomatic adults.     

弯月面涂胶及其胶厚均匀性的测量

为实现大面积基片的均匀涂胶,设计组装了一台小型弯月面涂胶样机,实验了200 mm200 mm基片的涂胶。利用白光干涉光谱仪扫描测量了弯月面涂胶的胶厚分布,其胶厚均匀性峰谷值偏差低于5%。对弯月面涂胶系统引起的均匀度偏差做了初步分析研究,并对比了测试系统与经校准的台阶仪胶厚测量结果,偏差小于0.8%。     

Classification of degraded cartilage through multiparametric MRI analysis

MRI analysis of cartilage matrix may play an important role in early detection and development of therapeutic protocols for degenerative joint disease. Correlations between MRI parameters and matrix integrity have been established in many studies, but the substantial overlap in values observed for normal and for degraded cartilage greatly limits the specificity of these analyses. We implemented established multiparametric analysis methods to define data clusters corresponding to control and degraded bovine nasal cartilage in two-, three-, and four-dimensional parameter spaces, and applied these results to discriminant analysis of a validation data set. Analyses were performed using the parameters (T₁, T₂, k_m, ADC), where k_m is the magnetization transfer rate and ADC is the apparent diffusion coefficient. Results were compared to univariate analyses. Multiparametric k-means clustering led to no improvement over univariate analyses, with a maximum sensitivity and specificity in the range of 60–70% for the detection of degradation using T₁, and in the range of 80% sensitivity but only 36% specificity using the parameter pair (T₁, k_m). In contrast, model-based analysis using more general Gaussian clusters resulted in markedly improved classification, with sensitivity and specificity reaching levels of 80–90% using the pair (T₁, k_m). Finally, a fuzzy clustering technique was implemented which may be still more appropriate to the continuum of degradation seen in degenerative cartilage disease. In view of its success in identifying mild cartilage degradation, the formal multiparametric approach implemented here may be applicable to the nondestructive evaluation of other biomaterials using MRI.     

A non-invasive technique for 3-dimensional assessment of articular cartilage thickness based on MRI part 2: Validation using CT arthrography

Established methods for the measurement of articular cartilage thickness are invasive and cannot be sequentially applied in living subjects. In the present study, the distribution of cartilage thickness throughout entire joint surfaces was determined from MR images obtained with a fat-suppressed gradient-echo sequence at a resolution of 0.31 × 0.31 × 2.00 mm³, and compared to that derived from CT arthrography. A minimal distance algorithm was employed to produce 3D cartilage thickness maps of seven cadaveric human knee joints. The mean amount of deviation of the cartilage volumes was 5.6% (±4.6), statistical analysis showing that there was high agreement between the two methods (r = 0.995, slope = 1.037, y-intercept = -90.5 mm³). The 3D thickness maps yielded a striking agreement between the two methods, the maximum values generally yielding a deviation of none or one thickness interval of 0.5 mm. This investigation shows that accurate 3D assessment of articular cartilage thickness can be performed with MRI, this technique having the advantage that it is suitable for investigating living subjects.     

nm量级薄膜厚度测量

为了获得nm量级薄膜样品的精确厚度,采用软X射线反射率拟合方法、Bragg衍射方程方法和反射率Fourier变换方法分析了常规Cu靶X射线衍射数据及软X射线反射率数据。对厚度测量结果进行比较,3种方法得到的结果一致性很好。其中,软X射线反射率拟合和Bragg衍射方程方法精度很高,优于1 nm,Fourier变换方法精度稍低。对于单层W薄膜样品,3种方法获得厚度分别为(15.21±0.60) nm,(14.0±1.0) nm和(13.8±1.5) nm;对于双层W/C薄膜样品,W层厚度分别为(12.64±0.60) nm,(13.0±1.0) nm和(13.9±1.5) nm。这3种方法测量结果精度主要取决于反射率数据测量精度,而Fourier变换方法精度随着能量升高而提高,随着掠入射角范围增大而提高。     

nm量级薄膜厚度测量

 为了获得nm量级薄膜样品的精确厚度,采用软X射线反射率拟合方法、Bragg衍射方程方法和反射率Fourier变换方法分析了常规Cu靶X射线衍射数据及软X射线反射率数据。对厚度测量结果进行比较,3种方法得到的结果一致性很好。其中,软X射线反射率拟合和Bragg衍射方程方法精度很高,优于1 nm,Fourier变换方法精度稍低。对于单层W薄膜样品,3种方法获得厚度分别为(15.21±0.60) nm,(14.0±1.0) nm和(13.8±1.5) nm;对于双层W/C薄膜样品,W层厚度分别为(12.64±0.60) nm,(13.0±1.0) nm和(13.9±1.5) nm。这3种方法测量结果精度主要取决于反射率数据测量精度,而Fourier变换方法精度随着能量升高而提高,随着掠入射角范围增大而提高。     

Raman analysis of proteoglycans simultaneously in bone and cartilage

Bone and cartilage are connective tissues with distinct organic matrix (collagen and non‐collagenous proteins) composition facilitating their biological function. Proteoglycans (PGs), a member of the non‐collagenous proteins fulfill functions that are determined by both their core protein and their glycosaminoglycan chains. The purpose of the present study was to identify Raman bands that are representative of PG concentration and may be used in both bone and cartilage tissues. To achieve this goal, we analyzed a series of reference PGs and collagens, as well as turkey leg tendon to verify the laser polarization independency of the identified bands. Additionally, the applicability of these bands in both cartilage and bone tissue simultaneously was tested in a healthy femoral head by Raman imaging and hierarchical cluster analysis to describe the distribution of PGs at the micron level from articular cartilage to subchondral bone. The results of the study show that the Raman band ~1375 cm⁻¹ can be used as a PGs marker band in both cartilage and bone. Moreover, articular cartilage has a lower content of organic matrix (mostly type II collagen), while the middle and deep transitional zone haves a higher concentration of PGs. The calcified cartilage is characterized by a lower content of PGs and total organic matrix (estimated from the integrated area of the amide III band). Copyright © 2014 John Wiley & Sons, Ltd.     

一种非接触测量光学零件厚度的方法

为了实现光学零件厚度的非接触测量,设计了一种基于电光扫描的非接触测量方法。采用电扫描技术控制光开关,形成半径依次减小的环状光束,经过锥透镜后在光轴上形成连续移动的光点,当光点瞄准待测光学零件表面时,反射能量出现峰值,即定位了待测零件的表面,进而获得光学零件的几何厚度。建立了测量平板零件厚度和透镜中心厚度的数学模型;从理论上探讨了该方法的测量范围和测量精度。结果表明:设定锥面镜口径为100mm,材料折射率为1.52,当锥面镜的锥角从1°变化到40°时,测量动态范围可以从5507mm变化到26mm;当测量范围为26mm时,测量精度可以达到2.5μm。该方法可基本满足目前光学零件中心厚度的测量需求。     

Optimization and validation of a rapid high-resolution T1-w 3D FLASH water excitation MRI sequence for the quantitative assessment of articular cartilage volume and thickness

In view of follow up, survey and development of therapeutic strategies for osteoarthritis where cartilage deterioration plays an important role, a non invasive, reliable and quantitative assessment of the articular cartilage is desirable. The currently available high resolution T(1)-weighted (T1-w) 3D FLASH pulse sequences with frequency selective fat suppression are very time consuming. We have 1) optimized a high resolution T1-w 3D FLASH water excitation (WE) sequence for short acquisition time and cartilage visualization, and 2) validated this sequence for cartilage volume and thickness quantification. The spectral fat presaturation was replaced by selective water excitation. The flip angle of the WE sequence was optimized for the contrast to noise (C/N(cart)) ratio of cartilage. Sagittal datasets (voxel size: 0.31 x 0.31 x 2 mm(3)) of the knees of nine healthy volunteers were acquired both, with the 3D FLASH WE (17.2/6.6/30 degrees ) sequence (WE) and a previously validated 3D FLASH fat saturated (42/11/30 degrees ) sequence (FS). For validation of the WE sequence, cartilage volume, mean and maximal cartilage thickness of the two sequences were compared. Reproducibility was assessed by calculating the coefficient of variation (COV %) of 4 consecutive WE data sets in the volunteers. The acquisition time was reduced from 16'30" (FS) down to 7'14" for the WE sequence. Image contrast and visualization of the cartilage was very similar, but delineation of the basal layer of the cartilage was slightly improved with the WE sequence. A flip angle of 30 degrees provided the best C/N(cart) ratios (WE). Reproducibility (COV) was between 1.9 and 5.9%. Cartilage volume and thickness agreed within 4% between FS and WE sequence. The WE sequence allows for rapid, valid and reproducible quantification of articular cartilage volume and thickness, prerequisites for follow-up examinations. The reduced acquisition time (50% of FS) enables routine clinical application and thus may contribute to a broader assessment of osteoarthritis.     

Observer reliability in CT and MRI of the abdomen/pelvis

The purpose of this research was to evaluate two sources of error in the performance of computerized tomography (CT) and magnetic resonance imaging (MRI) of the abdomen/pelvis. The sources of error assessed were inter- and intra-observer reliability. Thirty abdomen/pelvis CT scans were randomly selected from each of three hospitals (university, VA, military) with different CT scanners. Two radiologists were recruited from each site to be CT observers. Forty-five abdomen/pelvis MRI scans were randomly selected from two institutions with different MRI scanners. Four observers were recruited to read the MRI scans. All scans were read blind without clinical information or patient identification. Overall inter-observer and intra-observer diagnostic agreement was significantly higher for MRI compared to CT. Inter-observer diagnostic agreement rates were also significantly higher for MRI when the etiologies of neoplastic vascular and metabolic/toxic were assigned. Observer experience in CT (range: 5-9 yr) or MRI (range: 2-4 yr) was not statistically associated with improved diagnostic agreement. This research addresses many of the criticisms of the MRI literature and compares MRI favorably to CT.     

Differentiation of bone metastases from prostate cancer and benign red marrow depositions of the pelvic bone with multiparametric MRI

PurposeTo investigate the diagnostic utilities of imaging parameters derived from T1-weighted imaging (T1WI), diffusion-weighted imaging (DWI) and dynamic contrast-enhanced magnetic resonance imaging (DCE-MRI) to differentiate bone metastases from prostate cancer and benign red marrow depositions of the pelvic bone.Materials and methodsThirty-six lesions from 36 patients with prostate cancer were analyzed with T1WI, DWI, and DCE-MRI. The lesions were classified in the bone metastases (n = 22) and benign red marrow depositions (n = 14). Lesion-muscle ratio (LMR), apparent diffusion coefficient (ADC), volume transfer constant (K^trans), reflux rate (Kep), and volume fraction of the extravascular extracellular matrix (Ve) values were obtained from the lesions. The imaging parameters of the both groups were compared using the Mann-Whitney U test, receiver operating characteristics (ROC) curves were analyzed. For the ROC curves, area under the curves (AUCs) were compared.ResultsThe ADC, K^trans, K_ep, and V_e values of bone metastases were significantly higher than those of benign red marrow depositions (Mann-Whitney U test, p < 0.05). However, there was no significant difference in LMR between the two groups (Mann-Whitney U test, p = 0.360). The AUCs of K^trans_, K_ep, ADC, V_e, and LMR were 0.896, 0.844, 0.812, 0.724, and 0.448, respectively. In the pairwise comparison of ROC curves, the AUCs of K^trans and K_ep was significantly higher than LMR.ConclusionsK^trans, K_ep, V_e, and ADC values can be used as imaging tools to differentiate bone metastases from prostate cancer and benign red marrow depositions of the pelvic bone.     

Volumetric measurement of canine gliomas using MRI

The evaluation of tumor size by neurodiagnostic imaging is an important tool in determining disease progression or treatment efficacy. Apparent tumor size on any single slice image is sensitive to tumor shape and slice orientation. Volumetric measurements which use multiple, stacked images attenuate that sensitivity and can provide insights into tumor architecture. Volumetric measurements were made of induced canine gliomas using three common MR imaging protocols and with and without a contrast agent. Comparisons of the volumes described by each technique are made.     

The type I thyroplasty window: Implications of normal thyroid cartilage thickness

This paper describes the dimensions and placement of a standardizedIsshiki Type I thyroplasty window and the thickness of the thyroid cartilage at the window corners. In addition, the intraoperative optimal medialization of a series of windows is compared to these cartilage thickness measurements and these comparisons analyzed for their implications in surgical approach.Fifty-one Type I thyroplasty windows were fashioned on 42 larynges (cadavericand surgical). Measurements were taken of the window sizes, depth of medialization (surgical cases), and thickness of the thyroid cartilage at the four corners of the rectangular window. Sexes were kept separate because of inherent size differences of male and female larynges. From these physical measurements it is found that: (1) the thyroid cartilage window is not uniform in thickness throughout; there is a gradation of thickness from anterior to posterior and from superior to inferior; (2) when comparing the average depth of medialization to the window cartilage thickness in a standardized Isshiki window, the average distance of window depression almost equals the thyroid cartilage thickness, whereas posteriorly there is slightly more distance between the external surface of the window cartilage and the internal surface of the surrounding thyroid cartilage. Implications of the varying thickness of the thyroid cartilage and its relationship to the average depth of medialization in a standardized Isshiki thyroplasty window are discussed.     

Computer-aided quantification of focal cartilage lesions of osteoarthritic knee using MRI

Noninvasive assessment of articular cartilage using magnetic resonance imaging (MRI) has gained popularity in the diagnosis of osteoarthritis (OA), a condition that affects 20 million Americans. Focal cartilage lesions, a defect found in roughly 19% of the OA population, currently can only be evaluated with confidence using minimally invasive arthroscopy. This article presents a computer-aided procedure using MRI to quantify focal cartilage lesions and aims to support clinical practices of diagnosis and monitoring of lesion progress. Upon a local minima search for identifying focal lesions, the proposed gradient peak method outlines lesion boundaries and then generates morphological properties, such as lesion volume and lesion area. The procedure was evaluated using simulated and in vivo data. First, a simulated lesion was created and analyzed, and the results were compared with the exact solutions. Second, an in vivo evaluation was carried out on seven human knees in which nine focal lesions were identified and quantified. Three of the subjects had follow-up analyses, at either 1 or 2 years. Finally, in an attempt to characterize local biochemical changes underlying focal lesions, MR-derived T2 values of defective cartilage within the lesion boundaries were examined and compared with the values of adjacent cartilage compartments.     

Film thickness measurement and defect inspection using optical coherence tomography

An optical sensing technology based on optical coherence tomography is presented for film thickness measurement and defect inspection. In order to improve the imaging quality, a simple interference spectrum processing procedure is proposed to eliminate the DC and the autocorrelation noise. With the proposed method, we obtain high quality one-dimensional depth and two-dimensional cross-sectional images of the films. Then, the thickness and the defect information of the film can be obtained from the acquired images. The experiment result demonstrates that this nondestructive imaging technique is applicable for measuring film thickness and inspecting defects.     

Absolute thickness measurement of pyrolytic graphite spheroids by STEM-EELS

This paper studies the absolute thickness measurement of pyrolytic graphite spheroids (GSs) by using STEM-EELS mode with log-ratio method and Kramers-Kroning (K-K) method, taking the measured thickness from TEM image as reference that is the diameter of GSs ranging from 60 to 250 nm. The effect of collection semi-angle (β) on thickness measurement has been investigated. It is found that in general the thickness obtained by K-K analysis with surface effect corrected shows the best accuracy, followed by K-K sum rule and then log-ratio method for the three different collection semi-angles of 12.4, 17.3 and 21.1 mrad applied. Of these angles, the smallest one gives an overestimated result and the largest one gives an underestimated result, whereas between the two, the angle of 17.3 mrad that is about 2x convergence semi-angle (9.0 mrad) is identified as more appropriate for K-K analysis. The surface-scattering correction, inelastic mean free path of GS and effect of refractive index n on thickness measurement for different β angles are also investigated. Moreover, the optical property deduced from the data collected at the center of graphite spheroid, which is related to its microstructure, is characterized by K-K analysis.     

Local thickness measurement through scattering contrast and electron energy-loss spectroscopy

Scattering contrast measurements were performed on thin films of amorphous carbon and polycrystalline Au, as well as single-crystal MgO nanocubes. Based on the exponential absorption law, mass-thickness can be obtained within 10% accuracy by measuring the incident and transmitted intensities in the same image. For mass-thickness measurement of a thin amorphous specimen, a small collection semiangle improves the measurement sensitivity, whereas for the measurement of polycrystalline or single-crystal specimens, a large collection semiangle should be used to reduce diffraction-contrast effects. EELS thickness measurements on MgO nanocubes suggest that the Kramers-Kronig sum-rule method (with correction for plural and surface scattering) gives 10% accuracy at medium collection semiangles but overestimates the thickness at small collection semiangles, due to underestimation of the surface-mode scattering. The log-ratio method, with a formula for inelastic mean free path proposed by Malis et al. (1988), provides 10% accuracy at small collection semiangle, while that proposed by Iakoubovskii et al. (2008a) is preferable for medium and large collection semiangles. As a result of this work, we provide recommendations of preferred methods and conditions for local-thickness measurement in the TEM.     

Optoacoustic technique for thickness measurement of submicron metal coatings

The new nondestructive method for thickness measurement of submicron metal coatings on transparent substrate is developed. The method is based on the optoacoustic (OA) transformation in the system, where the coating is covered by an optically transparent liquid. Theoretical treatment of the problem consists of two steps. At the first step laser-induced thermal field in the system is calculated, taking into account the large thermal conductivity of the metal film and partial heat diffusion into the liquid. At the second step the system of wave equations for scalar potential of vibration velocities is solved. Heat sources, determined at the first step, are free form of wave equations. Three chrome coatings of different thickness (approximately 0.2, 0.3, and 0.6 μm) deposited on the quartz substrate are tested experimentally. Two different organic liquids (acetone and ethanol) are used to cover chrome coatings. Nanosecond diode-pumped Nd:YAG laser operated at the main harmonic is used to perform OA transformation (laser pulse duration is τ _L = 12 ns, the laser energy is about 0.2 mJ). Two detection modes are used. In forward mode laser pulse irradiates the film from the side of the substrate and in backward mode—from the side of the liquid. Detection of induced ultrasonic pulses is performed by the wide-band piezoelectric transducer in the liquid in both cases. The thickness of the coatings is determined by the least squares fitting of the theoretical dependencies of spectral transfer functions of OA transformation to experimental data. It is demonstrated, that the developed technique can be used for measurement of metal coatings thickness within the range from 50 nm to 5 μm with the error about 50 nm.