### Table 2 Results of fitting cylinders

1995

"... In PAGE 5: ...3 m away from the camera system. As can be seen from Table2 , the mean absolute error of fit is less than 1 mm. 6 Observations on accuracy We have achieved better than 1mm accuracy.... ..."

Cited by 27

### Table 2 Results of fitting cylinders

1995

"... In PAGE 5: ...3 m away from the camera system. As can be seen from Table2 , the mean absolute error of fit is less than 1 mm. 6 Observations on accuracy We have achieved better than 1mm accuracy.... ..."

Cited by 27

### Table 1: Cylinder data 2D and 3D Cylinder 2D Cylinder 3D

"... In PAGE 5: ... Most parameters, however, will a ect the Emission and Transmission contributions in the same way (through ij only), and therefore the model and its output is considered adequate for the purpose of identifying areas in the E-T plane where one source is dominating. From Table1 it is seen that the blank scan contribution to the noise as expected is only a small fraction of the transmission for same duration, the ratio being well ex- plained by the average attenuation of the (central part of) the 20 cm Cylinder phantom. For all practical purposes, therefore, the application of a 20 minutes blank scan will ensure that the blank scan contribution is negligible since the cases where a longer transmission scan might be ap- plied are those with a higher attenuation.... ..."

### Table 2 Results of fitting cylinders

"... In PAGE 23: ...3 m away from the camera system. As can be seen from Table2 , the mean absolute error of fit is less than 1 mm. 6 Observations on accuracy We have exceeded one millimeter accuracy.... ..."

### Table 2 Results of fitting cylinders

1994

"... In PAGE 23: ...3 m away from the camera system. As can be seen from Table2 , the mean absolute error of fit is less than 1 mm. 6 Observations on accuracy We have exceeded one millimeter accuracy.... ..."

### Table 11: Generating set for the equivariants when D4 acts as #3 + #5.

"... In PAGE 26: ... ii) A Hilbert basis for the ring of smooth IR-valued D4-invariant functions on V is given by i, i = 1; :::; 4, in Table 10. iii) The generators for the module of D4-equivariant smooth mappings from V to V , over the above ring of invariants, are given by bi in Table11 . Therefore, the normal form for the D4-equivariant map f in (1) is f(x) = 6 X i=1 Ai( 1(x); :::; 4(x))bi(x) (27) where, Ai are smooth functions.... ..."

### Table 2: The ne scale relative errors. Harmonic Harmonic Exp.

"... In PAGE 7: ... On the ne scale, we compare with the full ne scale solution in W V , and we include the -problem corrections to the upscaled solutions. It is important to note that Table2 is more germane to nonlinear problems, since we need accurate ne scale so- lutions to predict relative permeabilities and capillary pressures. Figure 1: Harmonic coarse scale solution (Exp.... ..."

### Table 1: Harmonic current limits

2001

"... In PAGE 3: ... For a front-end converter, this requirement implies that a large energy storage capacitor is required. As listed in Table1 , limits are set on the line current harmonics as well. Generally the first few odd triplen and odd non-triplen harmonics dominate the frequency spectrum, which implies a THD of less than 10%.... ..."

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