Full text: Proceedings, XXth congress (Part 5)

  
  
   
  
  
  
  
  
   
  
   
    
   
   
   
  
  
   
   
  
   
  
   
  
   
  
  
    
  
  
   
  
   
   
   
    
A RESOLUTION MEASURE FOR TERRESTRIAL LASER SCANNERS 
Derek D. Lichti 
Department of Spatial Sciences, Curtin University of Technology, GPO Box U1987, Perth. WA, 6845, Australia — 
d.lichti ? curtiu.edu.au 
Commission V, WG V/1 
KEY WORDS: LIDAR, Sampling. Resolution, Spatial, Quality, Terrestrial. 
ABSTRACT: 
Terrestrial laser scanners are increasingly being used for cultural heritage recording and engineering applications that demand high 
spatial resolution. Knowledge of an instrument’s spatial resolution is necessary in order to prevent aliasing and estimate the level of 
detail that can be resolved from a scanned point cloud. In the context of laser scanners. spatial resolution can be decoupled into 
range and angular resolution. The latter is the focus of this paper and is governed primarily by angular sampling interval and laser 
beamwidth. Both factors give rise to uncertainty in the angular position of a range measurement, though in terms of reporting 
scanner resolution, it has become a common practise to emphasise one of these factors—typically sampling interval 
as an indicator 
  
of resolution. Since both affect the resolution of a scanned point cloud, consideration of only one can lead to a misunderstanding of 
a system's capabilities. The ramification of this is that the actual resolution may be much lower than that perceived when visually 
inspecting a scan cloud. It will be demonstrated that consideration of only one factor independent of the other is inappropriate 
except under very specific conditions. A new, more appropriate resolution measure for terrestrial laser scanners is therefore 
necessary and one is proposed in this paper. The effective instantaneous field of view (EIFOV) is derived by modelling the inherent 
uncertainties in equal angular increment sampling and laser beamwidth with ensemble average modulation transfer functions 
(AMTFs). The practical outcome of this approach is a scientifically sound method of quantifying laser scanner resolution for users 
of the technology. Four commercially available terrestrial laser scanner systems are modelled with AMTFs and analysed in terms of 
their angular resolution as measured by the EIFOV. It is demonstrated that point cloud resolution as indicated by the EIFOV is 
much more coarse (by up to 21 times) than the sampling interval. 
I. INTRODUCTION 
Laser scanning instruments are increasingly being used for tasks 
traditionally performed using photogrammetric and surveying 
methods. They provide users with a three-dimensional sampled 
representation—a point cloud—of an object or surface and are 
used in a diverse range of applications including metrology, as- 
built surveys, reverse engineering, airborne topographic 
surveying, cultural heritage recording and volume estimation on 
mine sites. Though the accuracy requirements for these 
applications may differ considerably, spatial resolution is an 
important aspect of any laser scanner survey. 
Spatial resolution governs the level of identifiable detail within 
a scanned point cloud and is particularly important for, say, 
recording of cultural heritage features with fine details. For 
laser scanners it can be decoupled into range and angular 
resolution. Range resolution is the ability of a rangefinder to 
resolve two objects on the same line of sight (Kamerman, 
1993), which is directly proportional to timing resoluüon for 
time-of-flight systems (Wehr and Lohr, 1999). Angular 
resolution, the ability to resolve two objects on adjacent sight 
lines, is a function of spatial sampling interval and the laser 
beamwidth. For airborne laser scanner (ALS) systems, the 
sampling interval is partially dependent upon aircraft motion, 
whereas scanning mechanisms control it for terrestrial laser 
scanners (TLSs). 
Resolution is a term often abused and misunderstood: emphasis 
in sales literature tends to be on the finest possible sampling 
interval. which is often much smaller than the laser beamwidth. 
Since both factors influence the resolution of a scanned point 
cloud. consideration of only one can lead to a misunderstanding 
of a system's capabilities. To illustrate, consider the article by 
lavarone (2002), in which the author states that high scan 
resolution can be achieved by correlated sampling (Le. 
overlapping laser spots) and, therefore, laser beam spot size is 
not a limiting factor. While this is partially true in the sense 
that a fine sampling increment yields a high Nyquist frequency, 
the benefit of correlated sampling is not fully realised because 
sampling is not the only factor that influences resolution. 
A scanned point cloud may appear to have very high spatial 
resolution by virtue of a fine sampling interval and 
corresponding high point density. The actual spatial resolution 
may be much lower if the beamwidth is large relative to the 
sampling interval because the fine details are effectively 
blurred. It will be demonstrated in this paper that beamwidth 
can be a significant factor in reducing the spatial resolution of a 
scan cloud. even in the presence of correlated sampling. 
Though perhaps not an issue for smooth surfaces, it certainly 
could be for intricate surfaces with rapidly varying details that 
might be encountered in cultural heritage recording or as-built 
surveys of industrial plants. 
A new angular resolution measure for laser scanners that 
models the contributions of both sampling and beamwidth, the 
effective instantaneous field of view (EIFOV), is proposed. Its 
need is highlighted with a real dataset example that illustrates 
positional uncertainty due to beamwidth. The EIFOV is 
derived from an ensemble average modulation transfer function 
(AMTF) that models the positional uncertainty due to both 
factors. Following derivations of the AMTF and EIFOV, the 
angular resolution of four commercially available terrestrial 
   
  
    
   
    
  
  
  
  
  
  
   
   
  
   
  
  
  
  
  
  
  
    
   
  
  
  
Internati 
laser sca 
on terres 
applied t 
2.1 San 
Samplin; 
substanti 
confusio 
of the sa 
]. The. 
their fin 
function 
(Mensi a 
one rang 
  
| Make 
| Mensi 
Optech 
Riegl 
  
Table 1. 
The Op 
beamwid 
linear. di 
diameter 
Mensi g 
beam di
	        
Waiting...

Note to user

Dear user,

In response to current developments in the web technology used by the Goobi viewer, the software no longer supports your browser.

Please use one of the following browsers to display this page correctly.

Thank you.