Schlieren & Shadowgraph Methods 311L Aerospace Engineering 311L Aerospace Engineering

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Schlieren & Shadowgraph Methods
Aerospace Engineering 311L
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311L
Models of Light
Physical (wave) model
Wave Peaks
V  c o  3x10 8 m/s
Geometric model
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Light Rays
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Light From a Point Source
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Speed of Light in a Medium
Index of Refraction:
n
Typical values:
Medium
n = co/c
1.0003
Water
1.33
Crown glass 1.52
Plexiglas
1.51
Diamond
2.42
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c = speed of light in the medium
For gases:
Air
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co
c
n  1  kρ
ρ = gas density
k = 0.23 cm3/g for air
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Light Refraction
Snell’s Law:
θ1
n1sin θ1  n 2sin θ 2
n1  n 2
Medium 1
Medium 2
θ2
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Example, Refraction in Water
Water Surface
Pole
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Lenses
Focus
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Lenses
Point Source
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Direct Shadowgraphy
Point Source
Bubble of high
density gas
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Shadowgraph Image
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Some Math
y
εy
εy 
or
x
z
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L n
n y
εy 
kL ρ
n y
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The Basic Schlieren System
Point Source
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The Real Schlieren System
Extended Source
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Schlieren Image
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Schlieren vs. Shadowgraph
Schlieren
Shadowgraph
•
•
•
•
Displays a mere shadow
Shows light ray displacement
 2n
Illuminance level responds to 2
x
No knife edge used
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•
•
•
•
Displays a focused image
Shows ray refraction angle, 
Illuminance level responds to nx
Knife edge used for cutoff
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Mirrors
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ISU’s Z-type Schlieren System
Light Source
2nd Field Mirror
1st Field Mirror
Test Section
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Screen/Instrument Panel
Knife Edge
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Light Source
Condenser Lens
Lamp
A-A
Section A-A
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Setting Up The Schlieren System
Step 1: Find the focal length of the field mirrors
Focal Length
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Setting Up The Schlieren System
Step 2: Set up the first field mirror
Light Source
1st Field Mirror
Test Section
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Setting Up The Schlieren System
Step 3: Set up the second field mirror
Light Source
2nd Field Mirror
1st Field Mirror
Test Section
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Screen/Instrument Panel
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Setting Up The Schlieren System
Step 4: Set up the knife edge
Focus the
source image
on the knife
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Adjust the cutoff
Obtain a uniform
darkening of the image
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Uniform Darkening
Knife edge too close
to second field mirror
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Knife edge too far from
second field mirror
Uniform darkening
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Some Notes
• The angle between the illuminator axis and the collimated
beam should be kept to a minimum
– Coma: Smearing of the mirror focus into a comet shape (cancelled out by
tilting the mirrors in opposite directions, i.e. z-type system)
– Astigmatism: Changes the focus into two short lines perpendicular to each
other (limited by orienting the knife edge the same as the light source)
• A sheet of white paper is a good alignment tool
• A threaded bolt works well as a focusing tool
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References
• G.S. Settles, Schlieren & Shadowgraph Techniques,
Springer-Verlag, 2001.
• D.C. Giancoli, Physics for Scientists & Engineers, Prentice
Hall, 1988.
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