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Subrata Saha, Ph.D and Paul Allen Williams, B.S., Biomechanics Laboratory, Dept. of Orthopaedic Surgery, Louisiana State University Medical Center, P.O. Box 33932, Shreveport, LA 71130-3932
In this study the effects of various storage environments on the electrical properties of bone were evaluated. Cortical bone specimens from canine femora and tibiae were prepared and divided into three groups with one group maintained at room temperature (24°C), a second group stored in a refrigerator at 3°C, and the third group stored in a freezer at −10°C to −20°C. In each group, both the resistance and the capacitance decreased with time, the percentage of change being maximum for the samples stored in the freezer. This suggests that storage of bone specimens in a refrigerator or freezer with repeated thawing at room temperture does effect the electrical properties of bone, with the effect being dependent on the method of storage.
KEYWORDS
Electrical Properties
Bone
Storage Medium
Resistance
Capacitance
Although Orthopaedic surgeons are increasingly using electrical stimulation to treat non-unions and congenital pseudoarthrosis, the mechanism of action of bio-electricity is still unknown. For a better understanding of the role of electrical stimulation in bone remodeling and for an analysis of the distribution of direct or induced current in bone, we need accurate data on the electrical properties of bone. Although some investigators have measured electrical properties in vivo, this creates uncertainties regarding the current paths between a pair of electrodes placed in such a material and the nature of the tissue-electrode interface (Singh and Saha, 1984). Therefore, in vitro measurement techniques on standardized bone specimens have been utilized to characterize the electrical properties of bone.
With in vitro measurement methods it is important to know how various factors and parameters effect the measured value. Previously, Reddy and Saha (1984) have shown that the electrical properties of bone are anisotropic in nature and frequency dependent. Saha, Reddy, and Albright (1984) have shown that the electrical properties of bone are dependent on the moisture content, temperature, pH, time of exposure to the air, and measurement procedures. Other authors (Kosterich, Foster, Pollack, 1984; Singh and Saha, 1984) have shown that the electrical properties of bone are dependent on the conductivity of the immersion fluid, perserving solution, principles and techniques of measurement, and others. However, the effect of the environment in which the bone sample is stored, when not being measured, has not been properly investigated.
The fact that in most studies the bones are stored frozen or refrigerated prior to testing indicates a need to know the effect of this type of storage on the electrical properties of bone. The objective of this study was to evaluate and determine if such storage changes the electrical properties of bone, and to compare this with other type of storage environments. Three storage environments were chosen which were room temperature, a refrigerator, and a freezer.
Canine femora and tibiae were used in the study. The bones were removed soon after the sacrifice of the animal and wrapped in towels soaked in lactated Ringer’s solution to prevent the bones from drying. Two to three centimeter long specimens were then machined from the mid-diaphysis of each bone. Each specimen was then further machined in the axial direction to produce two to four matched specimens from each bone. During the entire machining process the bone were kept moist at all times. After machining, a total number of eleven bone specimens were individually placed into containers with lactated Ringer’s solution and an added bacteriostatic agent.
After the specimens were prepared, the resistance and capacitance were measured using a LCR meter (HP model 4262A), as described before (Saha, Reddy, and Albright, 1984). All measurements were made at 1 kHz. This initial measurment was made approximately two and a half hours after the sacrifice of the animal. The measurments were repeated throughout the day. At the end of the first day the samples were divided into three groups. The first group was maintained at room temperature (24°C); the second group was stored in a refrigerator at 3°C; and the third group was stored at −10° to −20°C. The next day the samples were removed from their storage environment and allowed to thaw and equilibrate to room temperature. Then the resistance and capacitance were measured repeatedly through the course of the day, being placed back into their respective storage environments at the end of the day. The procedure was repeated for upto four days with the times in which the bone specimens were removed from their environments and placed back being the same.
The electrical properties were measured using chlorided silver-metal electrodes. Surface moisture was removed from the bone prior to the measurement and a layer of conductive gel (AquasonicR 100, Parker lab) was applied to the bone surface and to the electrodes. The amount of time between the removal of the sample from the solution and the measurement was kept constant for each measurement due to the effect of exposure time (Saha, Reddy, and Albright, 1984).
Figure 1 shows the change in resistance for the three groups. The values for each day were calculated as the mean for the hourly readings for that day. As is shown, the resistance of the samples maintained at room temperature decreased slightly, similar to that of the specimens stored at refrigerator temperature. The resistance of the frozen specimens decreased at a noticeably faster rate than those stored at room temperature or in the refrigerator. The resistance of one sample at room temperature began to increase at day 5 while that of other specimens continued to decrease which was the reason for the large standard deviation noted. The reason for this increase is still unknown.
Fig. 1 Change in resistance with time for bone specimens stored in different environment.
Figure 2 shows the change in capacitance versus time for the three groups of specimens. The values for each day were calculated by the same method as those for the resistance. The capacitance of the refrigerated specimens decreased at a slower rate than did the capacitance of those stored at room temperature or those in the freezer. The capacitance of the frozen specimens decreased by approximately 50% after the first night of storage and then it did not change to any noticeable extent. The capacitance of the room temperature specimens decreased until they reached approximately 50% of their original values and then the values paralleled those for the frozen specimens.
Fig. 2 Change in capacitance with time for bone specimens stored in different environment.
Previously, other authors have reported changes in other physical properties of bone over time, when preserved in various ways. Steinberg and coworkers (1976) found decreases in strain related potentials in adult rat femora for 4–7 days, after the bone had been excised. Elwood and Smith (1984) have reported decreases in the zeta-potentials of bone during storage.
Although we have reported our results at one frequency (1KHz), it is possible that the nature of change in resistance and capacitance at other frequencies may be different. Also, Elwood and Smith (1984) found that different storage methods utilizing different fluids in which the bone is stored in, minimized the effect of storage.
From our study we have shown that the resistance and capacitance of bone is effected by the method in which it is stored and the rate of change is dependent on the storage method. Further studies are in progress to evaluate if the change in electrical properties can be minimized by different storage methods, other than those reported here. We also plan to study the effect of storage methods on frequency dependence of the electrical properties of bone.
This research was partially supported by National Science Foundation grant No. ECS - 8312680.
Elwood, W. K., Smith, S. D. Effects of Refrigerated (4°C) and Deepfreez (−80°C) storage in Buffered HEPES pH 7.4 on the Zeta - Potentials of Bone. J. Bioelectricity. 1984; 3:385–407.
Kosterich, J. D., Foster, K. R., Pollack, S. R. Dielectric Properties of Fluid-Saturated Bone: The Effect of Variation in Conductivity of Immersion Fluid. IEEE Trans. Bio-med. Engng. 1984; 31:347–369.
Reddy, G. N., Saha, S. Electrical and Dielectric Properties of Wet Bone as a Function of Frequency. IEEE Trans. Bio-med. Engng. 1984; 31:296–303.
Saha, S., Reddy, G. N., Albright, J. A. Factors...
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