A Gold Tru-fit spacer (George Taub Products, Jersey City, N.J.) bottle was left open for 0, 1, 4, 8, and 24 hours at 22°C. After each time interval, the bottles were closed (only for the mixing process) and mixed either by hand (shaking) according to the manufacturer's recommendations or by placing the bottle on a dental vibrator for 1 minute to disperse the material. After mixing, die spacer suspension was applied to clean glass slides with a single, even brush stroke. A new brush was used for each application. Samples were dried in air at 22°C. Three samples of die spacer suspension on glass slides were made for each combination of mixing technique and evaporation time variables.
Die coating thickness was determined using a Tencor Alpha-Step 200 profilometer (KLA-Tencor Instruments, San Jose, Calif.) with a diamond stylus tip 12.5 µm in radius (Fig. 1).
Fig. 1. Schematic drawing of side view of slide coated with die spacer in profilometer. Profilometer stylus travels across slide from uncoated area to region coated with die spacer. When in contact with coating, stylus rises and records its elevation change as coating thickness.
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A profilometer measures film thickness by tracing a stylus from an uncoated region to a coated region. When the stylus comes in contact with the coating, it rises with the elevation of the film thickness. The change in stylus elevation due to the film is recorded.
Three profile tracings were made for each sample (Fig. 2).
Fig. 2. Schematic drawing of top view of slide coated with die spacer. Dotted lines represent path of stylus across coating during profile trace. Open circles represent locations where film thickness measurements were made.
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For each tracing, 6 measurements of film thickness were made. These measurements were taken 250, 500, 750, 1000, 1250, and 1500 µm from the edge of the die spacer coating. Eighteen measurements (3 tracings × 6 measurements per tracing) were obtained for each sample. These 18 measurements were averaged to obtain 1 film thickness per sample.
A 2-way analysis of variance (ANOVA) was performed to determine the possible significance of any differences in film thickness with mixing technique or open bottle time (Sigma Stat, SPSS Inc, Chicago, Ill.). If a statistical difference was noted within a group, the Student-Newman-Keuls test with a set P
.05 was used as a multiple comparison procedure to isolate any differences.
A composite plot of averaged die space film thickness values for all variables with standard deviation bars was constructed (Sigma Plot, SPSS Inc).
Typical thickness profiles for both handshaken and vibrated films are provided in Figure 3.
Fig. 3. Typical film thickness profiles recorded by profilometer during single trace along die spacer coating. Profiles are for handshaken and vibrated mixing for die spacer bottles open for 24 hours.
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Mean values for each sample were obtained by averaging the thickness both over the 6 points along a single profile trace and over the 3 tracings per sample (Fig. 2
). A plot of the effects of mixing method and open bottle time on die space film thickness was made (Fig. 4).
Fig. 4. Plot of film thickness versus mixing mrethods and time die spacer bottle was left open. Bars represent averaged values; vertical lines on bars represent standard deviations.
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For mixing by hand (shaking), the thickness varied over time from 4.0 to 17.4 µm with an average of 8.7 µm. For mixing by vibration, film thickness varied over time from 2.4 to 6.6 µm with an average of 5.0 µm.
A 2-way ANOVA was performed to determine the significance of mixing method and open bottle time. The larger thickness found for the handshaken over the vibration group was statistically significant (P
.001). To isolate which times differed, the Student-Newman-Keuls method was used. The film thickness differences between handshaking and vibration existed at 4, 8, and 24 hours. The difference in die spacer thickness versus the time the bottles were left open was statistically significant (P
.001). The Student-Newman-Keuls results showed statistically different film thicknesses for all time comparisons except 0 versus 1 hour and 4 versus 8 hours. This result remained when considering only the samples within the handshaken group. Therefore, the results indicate that die spacer thickness increases with open bottle time when the bottle is handshaken. In contrast, within the vibration group, no statistical differences in film thickness existed with evaporation time except for 0 versus 4 hours. Therefore, the results indicate that, if the die spacer components are mixed by vibration, die spacer thickness does not increase with the time the bottle is left open.
The results indicate that evaporation of die spacer components does lead to larger die spacer film thickness. For handshaken bottles, die spacer thickness increased by 1%, 142%, 105%, and 329% for bottles left open for 1, 4, 8, and 24 hours, respectively, compared with bottles open for 0 hours (Fig. 4). This trend was less dramatic for bottles mixed on the dental vibrator: Die spacer thickness increased 74%, 171%, 111%, and 173% for bottles left open for 1, 4, 8, and 24 hours, respectively, compared with bottles open for 0 hours (Fig. 4
). These values are in the range of those found in a previous study, in which a 148% increase in film thickness was found with old versus new Tru-fit bottles.27 In that study, old bottles were simply defined as those previously used in the clinic; they therefore had been open for some unknown period. Similarly, Grajower et al23 found a 140% increase in Tru-fit thickness for 6-month-old bottles versus new. It is possible that such large increases in die spacer thickness with open bottle time are clinically significant.
For bottles that are handshaken per the manufacturer's instruction, increases in film thickness occur when the bottle is open for sometime between 1 and 4 hours. If it is assumed that a bottle is open for several minutes per application onto a clinical die, clinically significant increases may occur after painting 20 or 30 dies.
The clinical consequence of larger die spacer thickness found with open bottle time may be excessive cement film thickness. With all other variables held constant, an excessive luting agent film thickness may lead to lower restoration retention and/or higher luting agent solubility at the margin.26 Conflicting experimental results exist for crown retention7 versus cement thickness, possibly because of the multitude of experimental and/or clinical variables as well as differences in experimental design.
Greater die spacer film thickness with open bottle time probably is caused by the subsequent higher concentration of metal-oxide particles in the die spacer solution, with more metal oxides being applied per brush stroke. The higher concentration of adhesive during evaporation also may contribute to increased thickness.
During mixing, die spacer particles that have settled during the open bottle time must be evenly dispersed to obtain a sufficient quantity of particles, as well as adhesive, on the brush. Although vigorous shaking by hand for several minutes is recommended, such shaking is not always achieved clinically. Mixing bottles on the dental vibrator was chosen as a consistent technique for obtaining less-than-optimal mixing. Although thickness tended to increase with time with vibration, the vibrated thickness values were consistently lower than those obtained from handshaken samples. Our results suggest that, during vibration, the die spacer solution is not homogenized; a significant percentage of particles remain near the bottom of the bottle, possibly in congregates. The brush therefore does not capture a sufficient number of particles to obtain full thickness.
The increase in spacer thickness with open bottle time for vibration occurs earlier than that for handshaken samples (after 1 hour as opposed to 4 hours) and seems to remain fairly constant. It is possible that, even with the evaporation of liquid die spacer components with time, agitation with vibration is still not great enough to disperse the particles as well as shaking by hand.
The variation in applied die spacer thickness per brush application in the literature is quite large (6.0 to 19.8 µm per layer8,13,15,17,19,23-25,28) and probably is due to variations in clinical and experimental technique17 as well as differing positions on the dies,17 compositions, brushes, and substrate. The Tru-fit manufacturer claims that 4 thin coats provide 25 µm of internal relief,7 which averages to 6.3 µm per coat. The results of this study were within or close to these numbers. The average film thickness over time was 8.7 µm (range = 4.0-17.4 µm) after handshaking and 5.0 µm (range = 2.4-6.6 µm) after vibration.
For handshaken bottles in this study, 4 applications, on average, provided a die spacer thickness within the suggested optimal 25 to 40 µm range.4,11,12,17,22,23-25 Four coats of die spacer from bottles open for 0 or 1 hour provided a thickness of 16 µm, slightly less than the suggested optimal range. This lower thickness most likely was due to the wetting properties of die spacer liquid on smooth glass versus porous die stone. For bottles open for 24 hours, an excessive film thickness may occur with 3 or more applications.
Variation in the results of this study was low, with average standard deviations of 1.8 µm (range = 0.8-4.2 µm) for handshaking and 5.0 µm (range = 2.4-6.6 µm) for vibration mixing. Standard deviations in previous studies ranged from 4.5 to 19.9 µm for Tru-fit multicoated films.15,25,29
This study had limitations that hinder its direct clinical significance. Namely, it was designed to be a preliminary study to investigate only 2 of the many variables associated with die spacer thickness: the effects of evaporation of volatile liquid components and the intensity of bottle agitation during die spacer mixing. To keep the number of variables to a minimum and to attempt to decrease the high spacer film thickness variability found in other studies, only 1 brand of die spacer and 1 brand of glass slides were used. Decreasing film thickness variability was critical to determine statistical differences with mixing and/or open bottle time. As stated previously, the variation in film thickness found here was lower than in other studies. Additional studies that include other variables should be undertaken.
Several concerns arose regarding the choice of substrate for the die spacer films. Flat, smooth, uniform surfaces with little or no intersample surface variation were required, and glass microscope slides were deemed appropriate. Die spacer was not applied to stone for the following reasons: First, die stone is porous and comparatively rough. Applying spacer to die stone might have affected the film thickness found with profilometry. We wanted to be sure that variations found during the profile tracing were due to the die spacer film and not the roughness of the underlying stone. Moreover, because of the porosity of stone, some of the die spacer liquid might have entered the pores; the thickness of die spacer within the pores might not have been detected with profilometry. Second, the use of die stone would have introduced additional variables to the study. The choice of which brand of stone, the addition of hardener,15 and any manipulation variables incurred during stone mixing and setting would have increased the variability of the results. Therefore, for this preliminary study, smooth glass seemed appropriate.
Only 1 die spacer was chosen for this preliminary study. Most traditional die spacers are somewhat similar in composition; they comprise metal-oxide powders, adhesive, and a volatile organic matrix liquid. Differences in evaporation rates and the effects of evaporation, if any, are expected with die spacers from different manufacturers. However, the volatile components of all die spacers do evaporate, and it is expected that this evaporation may affect thickness. Therefore, for this preliminary study, the use of only 1 die spacer seemed reasonable. Gold Tru-fit was deemed a good choice because several studies related to die spacer thickness with Tru-fit exist in the literature8,13-15,17,23,24,27-29 and Tru-fit is commonly used in clinical settings.7 Because positive evaporation time and mixing agitation effects were found, future studies should include various brands of stones and die spacers to enhance the direct clinical significance of their findings.
This investigation, the first quantitative, well--controlled study to report the effects of evaporation and agitation on die spacer thickness, found that die spacer thickness increased with open bottle time and decreased with lower agitation during mixing. These findings compare well with other relevant results in the literature; however, variations in thickness values were lower in this study than in others. Further investigation is warranted to determine the clinical importance of the results reported previously.
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- aAssistant Professor of Clinical Dentistry, Division of Prosthodontics.
- bResearch Scientist, Division of Prosthodontics.
- cAssociate Professor, of Clinical Dentistry; Director, Division of Prosthodontics.
- dPrivate practice, Jersey City, N.J.
- This study was supported in part by grant No. NIH R29DE10980.
- Reprint requests to: Dr Jason J. Psillakis, Division of Prosthodontics, School of Dental and Oral Surgery, Columbia University, 630 W 168th St, New York, NY 10032, Fax: (212)305-8493, E-mail: [email protected]
Copyright © 2001 by The Editorial Council of The Journal of Prosthetic Dentistry.
- 0022-3913/2001/$35.00 + 0. 10/1/113028
- doi:10.1067/mpr.2001.113028