Effect Of Target Size Research Articles

Ray tracing for modeling of small footprint airborne laser scanning returns

Airborne Laser Scanning (ALS) has been established as a valuable tool for the estimation of biophysical canopy variables, such as tree height and vegetation density. However, up to now most approaches are built upon empirical stand based methods for linking ALS data with the relevant canopy properties estimated by field work. These empirical methods mostly comprise regression models, where effects of site conditions and sensor configurations are contained in the models. Thus, these models are only valid for a specific study, which renders inter-comparison of different approaches difficult. Physically based approaches exist e.g. for the estimation of tree height and tree location, however systematic underestimation depending upon sampling and vegetation type remains an issue. Using a radiative transfer model that builds on the foundation of the Open-Source ray tracer povray we are simulating return signals for two ALS system settings (footprint size and laser wavelength). The tree crowns are represented by fractal models (L-systems), which explicitly resolve the position and orientation of single leafs. The model is validated using ALS data from an experiment with geometric reference targets. We were able to reproduce the effects of target size and target reflectance that were found in the real data with our modeling approach. A sensitivity study was carried out in order to determine the effect of properties such as beam divergence (0.5, 1, and 2 mrad), canopy reflectance (laser wavelength, 1064 and 1560 nm) on the ALS return statistics. Using the two laser wavelengths above, we were able to show that the laser wavelength will not significantly influence discrete return statistics in our model. It was found that first echo return statistics only differ significantly if the footprint size was altered by a factor of 4. Last return distributions were significantly different for all three modelled footprint sizes, and we were able to reproduce the effect of an increased number of ground returns for large footprint sizes. These forward simulations are a first step in the direction of physically based derivation of biophysical ALS data products and could improve the accuracy of the derived parameters by establishing correction terms.

Forbidden transitions in excitation by proton impact in Li-like Al ions

This paper presents cross-sections and collision strengths for proton-impact excitation of optically forbidden transitions in Al10+. These data, calculated in the impact-parameter formalism, covering the expected range of energies/temperature in laser-produced plasmas, are believed to represent the first such detailed treatment of this system. The cross-sections decrease with energy as E−1, while the collision strengths tend to finite limits as the energy of colliding proton becomes infinitely great. This high-energy limiting value has been evaluated combining results from the semi-classical treatment of ion-impact excitation processes and the Born approximation for high-energy behavior of the collision strength. The effective target size has been estimated from the calculated high-energy limit of the collision strength in the Born approximation.

Effects of Target Length on the Hybridization Efficiency and Specificity of rRNA-Based Oligonucleotide Microarrays

The effect of target size on microarray hybridization efficiencies and specificity was investigated using a set of 166 oligonucleotide probes targeting the 16S rRNA gene of Escherichia coli. The targets included unfragmented native rRNA, fragmented rRNA ( approximately 20 to 100 bp), PCR amplicons (93 to 1,480 bp), and three synthetic single-stranded DNA oligonucleotides (45 to 56 bp). Fluorescence intensities of probes hybridized with targets were categorized into classes I (81 to 100% relative to the control probe), II (61 to 80%), III (41 to 60%), IV (21 to 40%), V (6 to 20%), and VI (0 to 5%). Good hybridization efficiency was defined for those probes conferring intensities in classes I to IV; those in classes V and VI were regarded as weak and false-negative signals, respectively. Using unfragmented native rRNA, 13.9% of the probes had fluorescence intensities in classes I to IV, whereas the majority (57.8%) exhibited false-negative signals. Similar trends were observed for the 1,480-bp PCR amplicon (6.6% of the probes were in classes I to IV). In contrast, after hybridization of fragmented rRNA, the percentage of probes in classes I to IV rose to 83.1%. Likewise, when DNA target sizes were reduced from 1,480 bp to 45 bp, this percentage increased approximately 14-fold. Overall, microarray hybridization efficiencies and specificity were improved with fragmented rRNA (20 to 100 bp), short PCR amplicons (<150 bp), and synthetic targets (45 to 56 bp). Such an understanding is important to the application of DNA microarray technology in microbial community studies.

The effects of target size and tissue density on the minimum margin required for random errors

The minimum margins required to compensate for random geometric uncertainties in the delivery of radiotherapy treatment were determined for a spherical Clinical Target Volume, using an analytic model for the cumulative dose. Margins were calculated such that the minimum dose in the target would be no less than 95% of the prescribed dose for 90% of the patients. The dose distribution model incorporated two Gaussians, and could accurately represent realistic dose profiles for various target sizes in lung and water. It was found that variations in target size and tissue density lead to significant changes in the minimum margin required for random errors. The random error margin increased with tissue density, and decreased with target size. The required margins were similar for dose distributions of spherical and cylindrical symmetry. Significant dose outside the spherical high dose region, as could result from multiple incident beams, lead to an increased margin for the larger targets. We could confirm that the previously proposed margin of 0.7 times the standard deviation of the random errors is safe for standard deviations up to 5 mm, except for very small targets in dense material.

Evaluation of (Z)‐9‐tricosene baited targets for control of the housefly (Musca domestica) in outdoor situations

Abstract:Houseflies (Musca domestica L.) are a major pest species in a variety of outdoor situations, notably on and around livestock farms and landfill used for the disposal of domestic waste. Currently no effective options are available for control of houseflies outdoors, because many populations exhibit at least some resistance to all available synthetic pesticides. (Z)‐9‐tricosene is the only commercially available pheromone for use in lure‐and‐kill approaches to housefly control, and it is widely used in indoor livestock units in combination with sugar/insecticide bait. Here we examine the potential of this approach for use outdoors, on a landfill site. We investigate the efficacy of toxic targets painted with a sugar/insecticide/(Z)‐9‐tricosene mix. The effects of target size and pheromone concentration were examined in two replicate trials, conducted in June and September 2003. As expected, catch consisted largely of males, was consistently higher on larger traps, and generally increased with (Z)‐9‐tricosene concentration even up to very high levels. However, in repeated trials, and despite mass release of marked flies, catch rates appeared to be insufficient to provide adequate control. We suggest that this is probably because (Z)‐9‐tricosene is primarily a short‐range attractant, and fly populations in outdoor situations are generally distributed over a large area. Catch declined rapidly to zero within 2 weeks, indicating that improved formulation or target design is needed to slow the weathering of active ingredients on the targets. It seems unlikely that (Z)‐9‐tricosene is sufficiently attractive to houseflies to provide an effective and economic lure in outdoor situations.

Constraints on the spatiotemporal accuracy of interceptive action: effects of target size on hitting a moving target.

Results of two experiments are reported that examined how people respond to rectangular targets of different sizes in simple hitting tasks. If a target moves in a straight line and a person is constrained to move along a linear track oriented perpendicular to the target's motion, then the length of the target along its direction of motion constrains the temporal accuracy and precision required to make the interception. The dimensions of the target perpendicular to its direction of motion place no constraints on performance in such a task. In contrast, if the person is not constrained to move along a straight track, the target's dimensions may constrain the spatial as well as the temporal accuracy and precision. The experiments reported here examined how people responded to targets of different vertical extent (height): the task was to strike targets that moved along a straight, horizontal path. In experiment 1 participants were constrained to move along a horizontal linear track to strike targets and so target height did not constrain performance. Target height, length and speed were co-varied. Movement time (MT) was unaffected by target height but was systematically affected by length (briefer movements to smaller targets) and speed (briefer movements to faster targets). Peak movement speed (Vmax) was influenced by all three independent variables: participants struck shorter, narrower and faster targets harder. In experiment 2, participants were constrained to move in a vertical plane normal to the target's direction of motion. In this task target height constrains the spatial accuracy required to contact the target. Three groups of eight participants struck targets of different height but of constant length and speed, hence constant temporal accuracy demand (different for each group, one group struck stationary targets = no temporal accuracy demand). On average, participants showed little or no systematic response to changes in spatial accuracy demand on any dependent measure (MT, Vmax, spatial variable error). The results are interpreted in relation to previous results on movements aimed at stationary targets in the absence of visual feedback.

Saccades to spatially extended targets: the role of eccentricity.

Size and eccentricity of visual targets are known to modulate saccade parameters. Here we asked for a possible interaction between these target properties. We investigated latency and amplitude of saccades to targets of varying diameter presented at various eccentricities in the visual field. Effects of target size on saccadic eye movements highly depended on eccentricity of saccade targets. For large saccade targets, latencies increased and mean amplitudes decreased mainly at parafoveal eccentricities. By contrast, scatter of saccade amplitudes increased nearly linearly with target size and eccentricity. These effects are consistent with the known functional anatomy of the superior colliculus. Size- and eccentricity-related changes in saccade parameters may depend on distinct subpopulations of collicular neurons.

Further evidence for, and some against, a planning–control dissociation

Further evidence for, and some against, a planning–control dissociation

Gain and Target Size Effects on Cursor-Positioning Time with a Mouse

Movement time to align a cursor with targets on a computer screen a mouse was examined across settings of gain and target size. Empirical evidence was sought in light of previous suggestions that performance declines observed at higher gains can be explained by decreased effective cursor resolution, not gain per se. We tested this hypothesis by holding the effective cursor resolution constant while systematically varying gain and target size. Analysis of movement times showed a significant gain effect as a function of target size. Specifically, movement time increased with gain at the smallest target size (i.e. 1.5 mm) but decreased with gain at the largest target size (i.e. 12 mm). These results do not support the no-effect of gain hypothesis and suggest that target size is an important factor in determining the effects of gain on mouse movement performance.

Timing accuracy in motion extrapolation: reverse effects of target size and visible extent of motion at low and high speeds.

By varying target size, speed, and extent of visible motion we examined the timing accuracy in motion extrapolation. Small or large targets (0.2 or 0.8 deg) moved at either 2.5, 5, or 10 deg s(-1) across a horizontal path (2.5 or 10 deg) and then vanished behind an occluder. Observers responded when they judged that the target had reached a randomly specified position between 0 and 12 deg. With higher speeds, the timing accuracy (the reverse of absolute error) was better for small than for large targets, and for long than for short visible extents. With low speed, these effects were reversed. In addition, while long visible extents yielded a greater accuracy at high than at low speeds, for short extents the accuracy was much better with the low speed. The findings suggest that, when extrapolating motion with targets and visible extents of different sizes, the visual system implements different scaling algorithms depending on target speed. At higher speeds, processing of visible and occluded motion is likely to share a common scaling mechanism based on velocity transposition. Reverse effects for target size and extent of visible motion at low and high speeds converge with the assumption of two distinct speed-tuned motion-processing mechanisms in human vision.

A track structure model for simulation of strand breaks in plasmid DNA after heavy ion irradiation.

We present a track structure model based on the local dose deposited around heavy ion tracks to explain the cross sections for single-strand and double-strand break induction in plasmid DNA in different aqueous buffers. The model is based only on measurable quantities, namely the effect distribution for inducing strand breaks after x-ray irradiation as a function of dose, and the radial dose distribution of the heavy ion track. The effect of indirect DNA damage mediated by free radicals produced in the water surrounding the DNA is accounted for by allowing the radial dose distribution to be smeared in space by an effective target size corresponding to the squared sum of the geometrical extension of the plasmid molecule and the mean free drift path of the radicals in the buffer solution. Our calculations reproduce well the measured cross sections for single-strand and double-strand break induction in SV40 plasmid DNA in various buffer solutions both as a function of the LET and of the specific energy of the heavy ion.

Temporal precision of interceptive action: differential effects of target size and speed

The duration of movements made to intercept moving targets decreases and movement speed increases when interception requires greater temporal precision. Changes in target size and target speed can have the same effect on required temporal precision, but the response to these changes differs: changes in target speed elicit larger changes in response speed. A possible explanation is that people attempt to strike the target in a central zone that does not vary much with variation in physical target size: the "effective size" of the target is relatively constant over changes in physical size. Three experiments are reported that test this idea. Participants performed two tasks: (1). strike a moving target with a bat moved perpendicular to the path of the target; (2). press on a force transducer when the target was in a location where it could be struck by the bat. Target speed was varied and target size held constant in experiment 1. Target speed and size were co-varied in experiment 2, keeping the required temporal precision constant. Target size was varied and target speed held constant in experiment 3 to give the same temporal precision as experiment 1. Duration of hitting movements decreased and maximum movement speed increased with increases in target speed and/or temporal precision requirements in all experiments. The effects were largest in experiment 1 and smallest in experiment 3. Analysis of a measure of effective target size (standard deviation of strike locations on the target) failed to support the hypothesis that performance differences could be explained in terms of effective size rather than actual physical size. In the pressing task, participants produced greater peak forces and shorter force pulses when the temporal precision required was greater, showing that the response to increasing temporal precision generalizes to different responses. It is concluded that target size and target speed have independent effects on performance.

Speech-based cursor control: understanding the effects of target size, cursor speed, and command selection

Speech recognition can be a powerful tool when physical disabilities, environmental factors, or the tasks in which an individual is engaged hinders the individual’s ability to use traditional input devices. While state-of-the-art speech-recognition systems typically provide mechanisms for both data entry and cursor control, speech-based interactions continue to be slow when compared to similar keyboard- or mouse-based interactions. Although numerous researchers continue to investigate methods of improving speech-based interactions, most of these efforts focus on the underlying technologies or dictation-oriented applications. As a result, the efficacy of speech-based cursor control has received little attention. In this article, we describe two experiments that provide insight into the issues involved when using speech-based cursor control. The first compares two variations of a common speech-based cursor-control mechanism. One employs the standard mouse cursor while the second provides a predictive cursor designed to help users compensate for the delays often associated with speech recognition. As expected, larger targets and shorter distances resulted in shorter target selection times, while larger targets also resulted in fewer errors. Interestingly, there were no differences between the standard and predictive cursors. The second experiment investigates the delays associated with spoken input, explains why the original predictive-cursor implementation failed to provide the expected benefits, and provides insight that guided the design of a new predictive cursor.

Assembly of the cleavage and polyadenylation apparatus requires about 10 seconds in vivo and is faster for strong than for weak poly(A) sites.

We have devised a cis-antisense rescue assay of cleavage and polyadenylation to determine how long it takes the simian virus 40 (SV40) early poly(A) signal to commit itself to processing in vivo. An inverted copy of the poly(A) signal placed immediately downstream of the authentic one inhibited processing by means of sense-antisense duplex formation in the RNA. The antisense inhibition was gradually relieved when the inverted signal was moved increasing distances downstream, presumably because cleavage and polyadenylation occur before the polymerase reaches the antisense sequence. Antisense inhibition was unaffected when the inverted signal was moved upstream. Based on the known rate of transcription, we estimate that the cleavage-polyadenylation process takes between 10 and 20 s for the SV40 early poly(A) site to complete in vivo. Relief from inhibition occurred earlier for shorter antisense sequences than for longer ones. This indicates that a brief period of assembly is sufficient for the poly(A) signal to shield itself from a short (50- to 70-nucleotide) antisense sequence but that more assembly time is required for the signal to become immune to the longer ones (approximately 200 nucleotides). The simplest explanation for this target size effect is that the assembly process progressively sequesters more and more of the RNA surrounding the poly(A) signal up to a maximum of about 200 nucleotides, which we infer to be the domain of the mature apparatus. We compared strong and weak poly(A) sites. The SV40 late poly(A) site, one of the strongest, assembles several times faster than the weaker SV40 early or synthetic poly(A) site.

The effect of target size and inertial load on the control of rapid aiming movements. A test of speed-sensitive and speed-insensitive strategies.

Two experiments are reported that investigated the effects of target size and inertial load on the control of rapid aiming movements. Based on kinematic profiles, movements were partitioned into their preprogrammed initial impulse- and feedback-based error correction phases. Electromyographic (EMG) rise rates were examined to investigate whether participants used a speed-sensitive or speed-insensitive control strategy. The results from both experiments showed that initial impulse velocity and EMG rise rates varied as a function of target size, i.e., a speed-sensitive strategy. This was the case whether participants were allowed to make error corrections to their movements (experiment 1) or were instructed to produce initial impulses that hit the target (experiment 2). Both experiments also showed that initial impulse velocity and endpoint variability were inversely related to inertial load. The results from experiment 2 indicated that, while the manipulation of inertial load had no effect on EMG rise rates for movements to a large target, EMG slopes were modulated between inertial load conditions when the target was small.

The effect of target size and eccentricity on reflex disparity vergence.

This study examined the effects of stimulus size and eccentricity on reflex disparity vergence: the small, involuntary corrections of eye alignment which serve to minimize the binocular disparity of fixated targets. Subjects were instructed to fixate steadily on a small, stationary mark superimposed on the center of a dynamic random dot stereogram. The stereogram was binocularly uncorrelated except for a fully correlated patch whose size and eccentricity were varied systematically across trials. The disparity of the patch was varied sinusoidally over time to stimulate vergence following movements. The overall purpose was to determine the relative contributions of various field loci in controlling binocular fixation by finding the smallest patch which would reliably drive vergence against the effort to fixate steadily. Psychophysical thresholds for detection of the correlated patch stimuli were also measured for comparison to the oculomotor results. Results showed that the smallest effective patch increased with eccentricity similarly for both vergence responses and psychophysical detection, suggesting they depend on a common, presumably cortical matching process. The dependence of response on eccentricity is roughly consistent with changes in the cortical magnification factor, suggesting that the area of cortex stimulated may be the determining factor in vergence responses to this class of stimulus.

Impact Fragmentation: From the Laboratory to Asteroids

In this paper, we study the effect of target size on the fragmentation outcome of rock targets using a 2D numerical hydrocode. After comparing our hydrocode calculations to laboratory data (including explosive disruption experiments) to validate the results, we use the code to calculate how the critical specific energy (Q*) needed to catastrophically fracture a body varies with target size in the regimes not accessible to experiment. Impact velocity is generally kept constant at about 2.0 km s−1, although some higher velocity (∼5 km s−1) simulations were run to determine a velocity dependence for the fragmentation outcome. To reflect the asteroid population, target diameters range from 10 cm to 1000 km, spanning the regimes where strength and self-gravity (radially varying lithostatic stress) each dominate resistance to fragmentation. We find that there is a significant difference in fragmentation outcome when the lithostatic stress is included in the computations. As expected, surface layers fragment more easily, while the strength of the central regions is greatly enhanced.We derive theQ* versus size relationship for three materials, (basalt, strong-, and weak-cement mortar) each having different static compressive strengths and representing a range of asteroid materials. The hydrocode results showed thatQ* decreased with increasing target size in the strength regime, with slopes of 0.43, 0.59, and 0.6 for basalt, strong and weak mortar, respectively. This decrease is directly related to the decrease in strain rate as target size grows. In the gravity regime,Q* increases with increasing target size, with a slope equal to 2.6 for all three of the materials modeled. These values are much steeper than those previously derived from scaling theories.Ejecta velocity distributions as a function of target size are examined as well. For large bodies, resultant ejecta speeds tend to be well below escape velocity, implying that these asteroids are likely to be reaccumulated rubble piles. In simulating the creation of the asteroid family Eos, we find that the code-calculated fragment size distribution is similar in character to the observed data, but secondary fragment sizes are significantly underestimated. More importantly, the determined ejecta speeds were too low for these fragments to have achieved escape velocity, and thus we fail to actuallyformthe separate bodies comprising the Eos family, and are left instead with a single rubble pile conglomerate.

Aiming Accuracy of the Line of Gaze and Redesign of the Gaze-Pointing System

The current experiment tested the aiming accuracy of the eye for targets at nine different positions and of two different sizes. The left eye was tracked to record the line of gaze with an infrared eye-monitoring device. For each subject, horizontal shift, vertical shift, standard deviations of the X and Y coordinates, and 95th percentile of the horizontal and vertical shifts from the nine target centers were calculated to indicate the precision, accuracy, and possible design limits of the gaze points. Analysis showed that the target's position had a strong effect on the vertical shift, standard deviations of the Y coordinate, and 95th percentile of the vertical shift. The effect of target size was not significant on any of the dependent measures. The research findings have important implications for the redesign of the gaze-pointing device. Visual targets appearing below the horizontal line of sight should be larger than those above. Based on the 95th percentile of the horizontal and vertical shifts, targets should be approximately 2.0 degrees wide and 2.4 degrees long above or coinciding with the horizontal line of gaze and 2.6 degrees wide and 3.9 degrees (cm) long below the horizontal line of gaze.

Motion extrapolation and velocity transposition.

A study of the effect of the size of a moving target and the extent of its visible motion on motion extrapolation is reported. Targets (a horizontal pair of dots separated by either 0.2 or 0.8 deg) moved across a 10 deg rectilinear path and were then occluded. Observers pressed a key when they thought the leading dot of a hidden target had reached a randomly specified position (0-12 deg from the point of occlusion). In experiment 1, in agreement with velocity-transposition predictions, at moderate (5 deg s-1) and rapid (10 deg s-1) velocities extrapolation times were longer for large targets than for small ones. At slow velocity (2.5 deg s-1) this effect was reversed. In experiment 2 the effect of target size at moderate velocity was found for a short (2.5 deg) visible path. However, the extrapolation time increased with shorter (2.5 deg versus 10 deg) paths. A proposed account of these effects suggests that the visual system performs a spatiotemporal scaling, according to the velocity-transposition principle, not only of visible motion but also of extrapolated motion.

Effect of target size on dose uniformity in plasma-based ion implantation

Plasma-based ion implantation of a square bar is modeled using a particle-in-cell plasma simulation for three different size bars. When the sheath width is significantly greater than the bar width, it is found that the incident ion dose is largest at the center of the bar and decreases precipitously at the corners. When the sheath width is comparable to the bar width, the incident dose is largest near to, but not at, the corners. It may be possible to optimize dose uniformity by straddling these two regimes.