As reported previously, the tumor could be visualized as a relatively hyperechoic region beneath the superior sclera that changed in size as the HF-US probe was moved nasally across the right eye.
13 HF-US images of a C918 tumor xenograft growing in the same rat eye at different times after implantation are shown in the upper panels of
Figure 1. These images were taken from approximately the center of the eye and qualitatively demonstrate the growth of the tumor over the course of 28 days. A small tumor was already present 5 days after implantation. By Day 19, it had grown enough to fill the vitreous and had pushed the lens noticeably anteriorly into the anterior chamber. By Day 28, it had grown anteriorly and had deformed the globe superiorly.
In each rat, a series of three scans were typically collectedat each imaging session, with an average of 2.9 ± 0.3 series per session (
n = 37 sessions). Tumor volume could be estimated from the series of HF-US images as demonstrated previously.
13 There was variability in growth rates among the tumors (
Fig. 2A). In particular, one tumor grew extremely slowly (▴) and two tumors grew very rapidly (▪ and ♦). The variable growth patterns resulted in large standard deviations in tumor volume at later measurement times. The average tumor volumes on Days 19 and 23 were 15.7 ± 11.3 mm
3 and 34.6 ± 21.4 mm
3, respectively (
n = 6).
Anesthesia of the rats twice a week did not cause significant weight loss. There was a trend for the mean weight to increase, and repeated measures one-way ANOVA revealed a significant effect of time on body weight (P = 0.011). The rats initially weighed 164 ± 9 g (n = 6). Two rats transiently lost weight during the study, but by Day 28, the average weight was 169 ± 7 g.
Fits of equation 1 to the volume data are shown by the curves in
Figure 2A. The three circled points on Day 28 were not included in the fits, since the entire tumor could not be reliably imaged on that day (see Discussion). In three of the six cases, the fitted value of τ was greater than the time of the last measurement, t
end. For one of these fits, the value of τ was within three days of the last measurement day (i.e., τ ≤ t
end + 3). That fit yielded relatively tight 95% confidence intervals, while the parameters from the other two fits had very broad confidence intervals. In those two instances, there was a very shallow minimum sum-of-squares error, and a wide range of τ values resulted in fits with very similar errors. Based on these considerations, it was decided to accept the fitted parameters if the fitted τ was less than or equal to t
end + 3, and to set τ = t
end if the fitted τ was greater than t
end + 3.
Table 1 shows that this model, given these restrictions, fitted all of the data well, and runs tests showed that the data did not deviate systematically from the curve (
P > 0.64). Values of
r 2 ranged from 0.967-1.000, indicating that the model accounted for most of the variability in the data. The average RMS error was only 0.8 mm
3. The relatively tight 95% confidence intervals of the parameters g
M and r
0 demonstrated that these parameters could be fitted uniquely.
When the model parameters were used to calculate the time-to-reach 20 mm3, tT=20, the average value was 21.8 ± 5.8 days (n = 6). The interpolation method yielded a value of 21.5 ± 5.8 days, which was similar to, but statistically less than, the value calculated from the model fits (P = 0.004).