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IMPACT CRATERS & SHOCK 
METAMORPHISM 
PRITHVI THAKUR 
Integrated Mtech, 
Geological Technology 4th year 
Enroll. No. 11410021
A PECULIAR PROCESS: 
Why impacts are different? 
RARITY large meteorites are rare, even on a 
geological timescale – there has been no 
historic example – this lack of direct human 
experience sets them apart from earthquakes, 
volcanoes, etc. 
IMMENSE ENERGY kinetic energy=1/2mv2 , 
very high even for small objects. The impact 
energy is only limited by m & v and not the 
Earth’s internal properties (volcanoes, 
earthquakes). 
INSTANT EFFECTS A 1km diameter crater (e.g. 
Barringer meteor crater- Arizona) forms in a 
few seconds. A 200km diameter structure(e.g. 
Sudbury- Canada or Vredefort- S.A.) forms in 
less than 10 mins. 
CONCENTRATED ENERGY RELEASE Internal 
terrestrial energy – Sub-continental to global 
in extent. Small Impact- effects are largely 
local. Large impacts(~100kms diameter) 
accompanied by catastrophic environmental 
effects on a global scale. 
EXTREME PHYSICAL CONDITIONS Typical 
impact velocities(5-8 km/s) results in shock 
waves – intense stresses in target rocks – 
large scale melting and vaporisation. 
UNIQUE DEFORMATION EFFECTS e.g. 
melting, Mineral deformation(PDF’s in 
quartz), Selective mineral melting, etc. These 
features are distinct from the normal 
geological features.
FORMATION OF IMPACT CRATERS 
1.Contact/Compression Stage 
• K.E is converted into Shock Waves 
• One set – transmitted from the interface into the target rock. 
• A complementary set – reflected back into the projectile 
(release wave). 
• The impact point is surrounded by concentric, hemispherical 
shock zones. 
• Near the crater rim – shock waves become elastic/seismic 
waves. This is the region of fracturing and brecciation. 
• Release wave results in melting/ vaporization of the projectile 
(vapor plume). 
Fig 1
FORMATION OF IMPACT CRATERS 
2. Excavation Stage 
• Upward ejection (spalling) of large near surface fragments and 
smaller ejecta curtain. 
• Subsurface flow of the target material to form the transient 
crater (bowl-shaped depression). 
• Excavated Zone – material is fractured, excavated & ejected 
beyond the transient crater rim. 
• Displaced Zone – target material is driven downward & 
outward coherently and does not reach the surface. 
Hat = final transient crater depth 
Hexc = depth of excavation 
Fig 2 
Theoretical transient crater
FORMATION OF IMPACT CRATERS 
3. Modification Stage 
• The excavation stage ends when the transient crater has grown to its maximum size, and the subsequent modification stage begins immediately. 
• Factors responsible for modification are gravity and rock mechanics (~ restoring forces). 
• The modification processes of uplift and collapse merge gradually into the normal processes of geological mass movement, isostatic uplift, erosion and 
sedimentation. 
• The extent to which the transient crater is modified depends on its size and properties of the target rock. 
• On this basis, impact structures can be classified as: Simple Craters, Complex Craters andMultiring Basins.
SIMPLE CRATER COMPLEX CRATER 
Fig 3
TYPES OF IMPACT CRATERS 
Simple Crater s 
• Bowl shaped depressions. 
• Less than a few kms across 
• Original transient cavity –shape & dimensions preserved 
• During modification, crater immediately filled to half its 
original depth – mixture of redeposited ejecta & debris 
from walls and rims. 
• This crater filling unit, called Breccia lens, is a mixture of 
rock fragments & impact melt. 
D = final crater diameter (10-20% greater than premodified 
transient crater) 
dt = true depth of the final crater 
da = apparent depth of the crater 
Fig 1
TYPES OF IMPACT CRATERS 
Complex Crater s 
• Characterized by central uplift region. 
• Formed in larger structures (>4km - crystalline rocks, >2km 
- sediments)  these values only applicable to earth. 
• Late stage modification – complex interactions b/w 
shock-wave effects, gravity, strength & structure of target 
rocks. 
• Rocks around periphery – collapse downward & inward 
along concentric faults (ring grabens) and a series of 
terraces along the outer margin. 
• Centre of the transient crater – forms central uplift. 
• The amount of Stratigraphic uplift (S.U) is about 1/10th 
the final diameter (D). 
Fig 4. Dr= diameter of the complex crater
TYPES OF IMPACT CRATERS 
Mul ti r ing Bas ins 
• Composed of multiple concentric uplifted rings and 
intervening down-faulted valleys. 
• They have 2 or more interior rings in addition to the outer 
rim. 
• The existence of multi-ring basin has not yet been 
demonstrated on earth. 
• The few possible candidates are Manicouagan (Canada, 
100 k.m.), Vredefort (South Africa, >200 k.m.), Sudbury 
(Canada, >200 k.m.) 
• It is not yet clear whether the transition b/w complex 
crater and multi-ring basin is purely based on size or 
some other special conditions are required. 
Fig 5. Multi-ring Basin, Moon
STAGES OF SHOCK METAMORPHISM 
• < 2 G P a - f r a c t u r i n g a n d b r e c c i a t i o n , w i t h o u t d e v e l o pme n t o f u n i q u e s h o c k f e a t u r e s . 
• > 2 G P a t o < 3 0 G P a - S h a t t e r c o n e s . A t l o w p r e s s u r e s ( < 1 0 G P a ) , o c c u r s w i t h o u t d i s t i n c t mi c r o s c o p i c 
d e f o rma t i o n f e a t u r e s . A t h i g h e r p r e s s u r e s , c o n t a i n s d i s t i n c t i v e mi c r o d e f o rma t i o n f e a t u r e s . 
• ~ 8 G P a t o 2 5 G p a - Mi c r o s c o p i c p l a n a r d e f o rma t i o n f e a t u r e s i n i n d i v i d u a l mi n e r a l s , e s p e c i a l l y q u a r t z 
a n d f e l d s p a r . 
• > 2 5 G P a t o 4 0 G P a - T r a n s f o rma t i o n o f i n d i v i d u a l mi n e r a l s t o amo r p h o u s p h a s e s ( d i a p l e c t i c g l a s s e s ) . 
• > 3 5 G P a t o 6 0 G P a - S e l e c t i v e p a r t i a l me l t i n g o f i n d i v i d u a l mi n e r a l s , t y p i c a l l y f e l d s p a r s . I n c r e a s i n g 
d e s t r u c t i o n o f o r i g i n a l t e x t u r e s . 
• > 6 0 G P a t o 1 0 0 G P a - C omp l e t e me l t i n g o f a l l mi n e r a l s t o f o rm a s u p e r h e a t e d r o c k me l t . 
• > 1 0 0 G P a - C omp l e t e r o c k v a p o r i s a t i o n . No p r e s e r v e d ma t e r i a l s f o rme d a t t h i s s t a g e . ( v a p o r i z a t i o n a n d 
s u b s e q u e n t c o n d e n s a t i o n t o g l a s s y ma t e r i a l h a v e b e e n i d e n t i f i e d s o f a r )
Shatter Cones Carbonate Phosphate Impact Melt 
Diaplectic Glass 
2 sets of decorated PDFs 
Quartz multiple sets of PDFs
REFERENCES 
• Traces of Catastrophe – NASA 
• www.mit.edu – MIT open course Impact Craters 
• www.en.Wikipedia.org 
• www.images.google.com 
• www.flickr.com 
• www.tumblr.com

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Impact Craters and Shock Metamorphism

  • 1. IMPACT CRATERS & SHOCK METAMORPHISM PRITHVI THAKUR Integrated Mtech, Geological Technology 4th year Enroll. No. 11410021
  • 2. A PECULIAR PROCESS: Why impacts are different? RARITY large meteorites are rare, even on a geological timescale – there has been no historic example – this lack of direct human experience sets them apart from earthquakes, volcanoes, etc. IMMENSE ENERGY kinetic energy=1/2mv2 , very high even for small objects. The impact energy is only limited by m & v and not the Earth’s internal properties (volcanoes, earthquakes). INSTANT EFFECTS A 1km diameter crater (e.g. Barringer meteor crater- Arizona) forms in a few seconds. A 200km diameter structure(e.g. Sudbury- Canada or Vredefort- S.A.) forms in less than 10 mins. CONCENTRATED ENERGY RELEASE Internal terrestrial energy – Sub-continental to global in extent. Small Impact- effects are largely local. Large impacts(~100kms diameter) accompanied by catastrophic environmental effects on a global scale. EXTREME PHYSICAL CONDITIONS Typical impact velocities(5-8 km/s) results in shock waves – intense stresses in target rocks – large scale melting and vaporisation. UNIQUE DEFORMATION EFFECTS e.g. melting, Mineral deformation(PDF’s in quartz), Selective mineral melting, etc. These features are distinct from the normal geological features.
  • 3. FORMATION OF IMPACT CRATERS 1.Contact/Compression Stage • K.E is converted into Shock Waves • One set – transmitted from the interface into the target rock. • A complementary set – reflected back into the projectile (release wave). • The impact point is surrounded by concentric, hemispherical shock zones. • Near the crater rim – shock waves become elastic/seismic waves. This is the region of fracturing and brecciation. • Release wave results in melting/ vaporization of the projectile (vapor plume). Fig 1
  • 4. FORMATION OF IMPACT CRATERS 2. Excavation Stage • Upward ejection (spalling) of large near surface fragments and smaller ejecta curtain. • Subsurface flow of the target material to form the transient crater (bowl-shaped depression). • Excavated Zone – material is fractured, excavated & ejected beyond the transient crater rim. • Displaced Zone – target material is driven downward & outward coherently and does not reach the surface. Hat = final transient crater depth Hexc = depth of excavation Fig 2 Theoretical transient crater
  • 5. FORMATION OF IMPACT CRATERS 3. Modification Stage • The excavation stage ends when the transient crater has grown to its maximum size, and the subsequent modification stage begins immediately. • Factors responsible for modification are gravity and rock mechanics (~ restoring forces). • The modification processes of uplift and collapse merge gradually into the normal processes of geological mass movement, isostatic uplift, erosion and sedimentation. • The extent to which the transient crater is modified depends on its size and properties of the target rock. • On this basis, impact structures can be classified as: Simple Craters, Complex Craters andMultiring Basins.
  • 6. SIMPLE CRATER COMPLEX CRATER Fig 3
  • 7. TYPES OF IMPACT CRATERS Simple Crater s • Bowl shaped depressions. • Less than a few kms across • Original transient cavity –shape & dimensions preserved • During modification, crater immediately filled to half its original depth – mixture of redeposited ejecta & debris from walls and rims. • This crater filling unit, called Breccia lens, is a mixture of rock fragments & impact melt. D = final crater diameter (10-20% greater than premodified transient crater) dt = true depth of the final crater da = apparent depth of the crater Fig 1
  • 8. TYPES OF IMPACT CRATERS Complex Crater s • Characterized by central uplift region. • Formed in larger structures (>4km - crystalline rocks, >2km - sediments)  these values only applicable to earth. • Late stage modification – complex interactions b/w shock-wave effects, gravity, strength & structure of target rocks. • Rocks around periphery – collapse downward & inward along concentric faults (ring grabens) and a series of terraces along the outer margin. • Centre of the transient crater – forms central uplift. • The amount of Stratigraphic uplift (S.U) is about 1/10th the final diameter (D). Fig 4. Dr= diameter of the complex crater
  • 9. TYPES OF IMPACT CRATERS Mul ti r ing Bas ins • Composed of multiple concentric uplifted rings and intervening down-faulted valleys. • They have 2 or more interior rings in addition to the outer rim. • The existence of multi-ring basin has not yet been demonstrated on earth. • The few possible candidates are Manicouagan (Canada, 100 k.m.), Vredefort (South Africa, >200 k.m.), Sudbury (Canada, >200 k.m.) • It is not yet clear whether the transition b/w complex crater and multi-ring basin is purely based on size or some other special conditions are required. Fig 5. Multi-ring Basin, Moon
  • 10. STAGES OF SHOCK METAMORPHISM • < 2 G P a - f r a c t u r i n g a n d b r e c c i a t i o n , w i t h o u t d e v e l o pme n t o f u n i q u e s h o c k f e a t u r e s . • > 2 G P a t o < 3 0 G P a - S h a t t e r c o n e s . A t l o w p r e s s u r e s ( < 1 0 G P a ) , o c c u r s w i t h o u t d i s t i n c t mi c r o s c o p i c d e f o rma t i o n f e a t u r e s . A t h i g h e r p r e s s u r e s , c o n t a i n s d i s t i n c t i v e mi c r o d e f o rma t i o n f e a t u r e s . • ~ 8 G P a t o 2 5 G p a - Mi c r o s c o p i c p l a n a r d e f o rma t i o n f e a t u r e s i n i n d i v i d u a l mi n e r a l s , e s p e c i a l l y q u a r t z a n d f e l d s p a r . • > 2 5 G P a t o 4 0 G P a - T r a n s f o rma t i o n o f i n d i v i d u a l mi n e r a l s t o amo r p h o u s p h a s e s ( d i a p l e c t i c g l a s s e s ) . • > 3 5 G P a t o 6 0 G P a - S e l e c t i v e p a r t i a l me l t i n g o f i n d i v i d u a l mi n e r a l s , t y p i c a l l y f e l d s p a r s . I n c r e a s i n g d e s t r u c t i o n o f o r i g i n a l t e x t u r e s . • > 6 0 G P a t o 1 0 0 G P a - C omp l e t e me l t i n g o f a l l mi n e r a l s t o f o rm a s u p e r h e a t e d r o c k me l t . • > 1 0 0 G P a - C omp l e t e r o c k v a p o r i s a t i o n . No p r e s e r v e d ma t e r i a l s f o rme d a t t h i s s t a g e . ( v a p o r i z a t i o n a n d s u b s e q u e n t c o n d e n s a t i o n t o g l a s s y ma t e r i a l h a v e b e e n i d e n t i f i e d s o f a r )
  • 11. Shatter Cones Carbonate Phosphate Impact Melt Diaplectic Glass 2 sets of decorated PDFs Quartz multiple sets of PDFs
  • 12. REFERENCES • Traces of Catastrophe – NASA • www.mit.edu – MIT open course Impact Craters • www.en.Wikipedia.org • www.images.google.com • www.flickr.com • www.tumblr.com