Module 7/8 Flashcards

1
Q

LASER

A

is the acronym for Light Amplification by Simulated Emission of Radiation. Laser light is made of waves with the same wavelength, moving in
the same direction and in phase. These properties
of laser light are referred
as monochroma-city, collima-on
and coherence.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

3D laser scanners employ

A

Nd:YAG-­‐Neodymium-­‐doped

YttriumAluminum Garnet, Nd:Y3Al5O12.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

LIDAR

A

Light Detection and Ranging

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

TLS

A

Terrestrial Laser Scanning

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

ALS

A

Airborne Laser Scanning

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Terrestrial Laser

A

Reigl z420i (1000m range)
Nd:YAG 1064 nm lasers
• Laser rangefinder error = 4 mm at 1000m
• Laser backscatter off ground. Mirror and rotational stepper motors direct laser beam
• Distance = (c x Tflight)/2

Bare Ground Error Budget:
• Laser rangefinder error = 0.4 cm at 1000m
• GPS error ~1-4 cm+
• Registration Error = 2-5 cm
• Estimated RMSE
• 2.6-6.5 cm vertical
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

TLS (LIDAR) for Civil Engineer Geotechnical

A
• Topographic design
• Landslides, Liquefaction,Lat.
Spread
• Accretion & Erosion
• Settlement measurement
• River Scour
• Excavation displacements
• Quay & sea walls
• Geomorphic change
detection
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

TLS (LIDAR) for Civil Engineer Structural

A
  • Structural displacements\ deflections \rotations
  • Failure patterns
  • Design vs. built differences
  • Concrete deformations
  • Modeling interior space/utilities.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Typical Terrestrial LIDAR Setup

A
RTK-DGPS Base
Photogrammetric Camera
RTK-DGPS Rover
Benchmark
Laser
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

3D Terrestrial Laser Scanner

A
  1. Range finder electronics
  2. Laser beam
  3. Polygon mirror
  4. Body
  5. TCP/IP Ethernet interface
  6. Laptop computer
  7. Camera
  8. USB interface
  9. Software

A diagram for the RIEGL Z-SeriesTerrestrial 3D laser scanners.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Solar Spectrum:

A

Non-­‐MonochromaAc
Non-­‐Collimated
Non-­‐Coherent

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

Laser Light

A

Monochromatic (single wavelength)
Collimated (in the same direction)
Coherent (in phase)

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

The electromagnetic spectrum

A

V=ƒ λ
The propagating velocity of electromagnetic waves (V), commonly known as the speed of light, is 299,792,458 m/sec in a vacuum. The relationship of V, λ, and f is the same for all wave types.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

The wavelength of peak power is predicted for a given target temperature by

A

Wien’s law:
λmax = 2,898,000 nm-­‐K/T
Human body 310°K (98.6°F, 37°C)
λmax ~ 9700 nm-­‐K/T

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

The energy of a single photon an electromagnetic wave

carries is a function of frequency be calculated as:

A

E=hf = h V/λ
where h is Plank’s constant, 4.135 x 10-15 electron volts-sec or 6.626069 x 10-34 J-sec.
Electronic waves have wave length (λ), and frequency (f) and carry energy (E).

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Electromagnetic Radiation from Our LIDAR laser.

A

Our scanner has a Nd:YAG laser has a wavelength of 1064 nm. Calculate the frequency of the laser wave and the energy that the wave
carries (1 photon) in a vacuum.
ƒ =V/λ=299792458/1064•10^­‐9 m/cycle = 2.8•10^14 cycles/sec
E=hƒ=hV/λ
=6.626069•10-­‐34J-­‐s 2.8 •10^14 cycles/sec=1.867•10^­‐19J

=Energy that the wave carries (of one photon in a vacuum at 1064 nm and 2.8 10^14cycles/sec.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
17
Q

Our Riegl z420i

A

is a low power 1064 nm

(infrared) Nd:YAG laser and eye safe.

18
Q

Reflector Registration

A

Registered from best
fit to common
reflectors.
500m

19
Q

Topnext RTN-DGPS Control for Positioning

A
Digital Photo Overlay
LIDAR 80° scanning window
GPS Controller
w/ Cellular Modem
CORS Network Differential
20
Q

TLS Processing Proc

A
A: Scan
B: Registration
C: Surface Modeling
TIN
Quantify +/or
Change
Detection
21
Q

Registration

A
Registering (Merging)
multiple scans eliminates
shadow zones
Picture--(2 false-colored scans in
white and red)
22
Q

Sometimes Tripods Do Not Work: Overcoming Obstacles and Shadows

A

Elevated (20 m) Terrestrial LIDAR

1) Downward view of terrain/vegetation
2) Improved grazing angle
3) Flat terrain max range = H / tan 3°-5°

23
Q

Registration by the Translation matrix

SOCS>PROCS>GLOCS

A

SOCS – Scanners
Own Coordinate System
PROCS –Project Coordinate System
GLOCS-­‐Global (Georeferenced) Coordinate System

24
Q

Scanner’s Own Coordinate System (SOCS)

A

the coordinate of the scanner’s raw data.

25
Q

Project Coordinate System (PRCS)

A

The coordinate system
defined by the user. We fix one of the scans as ‘Registered’, and adjust
all other scans to it’s coordinate system (SOCS–>PRCS).

26
Q

Global Coordinate System (GLCS)

A
is the Georeferenced coordinate system into which the entire project
is embedded (e.g. UTM, State Plane northings, eastings, elevation; (PRCS-->GLCS)
27
Q

2D Coordinate Transformation using Direction Cosines

A
  • x’A=xΑcosα+yAsinα+c

* y’A=-­xΑsinα+yAcosα+d

28
Q

3D Coordinate Transforma1on – Euler Angles

A

The transformation matrix we seek is the product of the three sequential transformations (in the correct order) or T(2,1)=T(2,F’‘,F’)T(F’,1)

29
Q

Direction Cosines-­‐3D Coordinate Transformation

A

3D coordinate transformation is similar to 2D with an added dimension, the objective
is to find the coordinates of Point A in the X’Y’Z’ system if the coordinates of that
point in the XYZ system are known. Again from analytical geometry:
• x’ = x cos(x’, x) + y cos(x’, y) + z cos(x’, z) + c
• y’ = x cos(y’, x) + y cos(y’, y) + z cos(y’, z) + d
• z’ = x cos(z’, x) + y cos(z’, y) + z cos(z’, z) + e

This transformation has nine independent parameters

30
Q

Point cloud vs. Reflector Registration

A

RMSE=Root Mean Square Error= sqrt((z1,i-z2,i)^2/n)

For a large sample population of n, RSME^2=M^2+o(omega)^2
For large unbiased population, RMSE=o(omega)

31
Q

Comparison between Terrestrial and Airborne LIDAR

A
-­‐ Laser Rangefinder:
Optech ALTM 3100
-­‐ 1064nm w/integrated
IMU&GPS.
-­‐ Pre-­‐Trench Flight 1: Fixed wing at 900m (Airborne1,El Segundo, California)
-­‐ Post Trench Flight 2:
Helicopter at 210m
(Terrapoint, The Woodlands, Texas)

• Laser rangefinder error
= 2-­‐3 cm
• GPS error=5-­‐10cm
• IMU error=~9cm@900m

Vendors quoted RMSE
– 18cm vertical (95%CI)
– 0.3-­‐0.45m horizontal (1σ)

32
Q

Airborne systems

A

Airborne systems collect
overlapping swaths of data
Waveform based lidar is typical in airborne systems

33
Q

Residual, Mean of the residuals, sample dispersion

A

Ri=Residual=(zi-zknown,i)
M=mean of residual=sample bias= sum of Ri/n
o(omega)=sample dispersion=sqrt(sumof(Ri-M)^2/(n-1))

34
Q

Blind Comparison of Airborne and Terrestrial

LIDAR

A

• Terrestrial LIDAR had almost no bias with pre- and post-trench
Airborne LIDAR had negative bias in both pre- and post-trench
μ = -23.6 - -8.7 cm, and σ = 5.6 - 20.0 cm
(errors exceeded both vendors specifications)
• Terrestrial data had 1/4-1/10 mean error and 1/1.4-1/5 dispersion of airborne
data.
• Multi-epoch elevation change terrestrial residuals were 1/3 of airborne residuals.

35
Q

Index of Refraction

A

• The ratio between the propagation rates in a
vacuum and in atmosphere is the index of
refraction which can be expressed as follows:
• n=c/V
• where c is the speed of light in a vacuum and n
is the index of refraction. The value of n is
around 1.0003.

36
Q

Refraction

A

The LASER wavelength of an electromagnetic wave decreases as the propagation velocity drops. Since the wave energy does not change and the frequency remains fixed. This effects the estimation of range distance.

37
Q

Index of refraction

A

λo/λ = (c/ƒ)/(v/ƒ)=c/v=n

n=index of refraction
ƒ=frequency
c=speed of light in a vacuum
v=speed of light in air
λo = wavelength in a vacuum
λ=wavelength in air
38
Q

Temperature

A
  1. The effect of temperature on the index of refraction is the most profound.
    For example, for a temperature change of 5 Cº from 10Cº to 15Cº, the corresponding change in
    the index is more than 5ppm.
39
Q

Minor effects on refraction: Atmospheric Pressure Humidity

A

The humidity has the least effect on the index of refraction.
For a 10 percent increase in humidity from 30 to 40 percent,
the change in the index is about 0.087 ppm when λ=0.915 μm

40
Q

Actual V, λ, and Error

A

n=c/V
λ =V/ƒ
t=Distance/V
DistanceError=Vt-­Distance(vacuum)

•Significant problem if the target distance is large.
•Understand how the
distance is being calculated.
•Be mindful of temperature.