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COLLISION
Collison
Head on
Collision
Elastic
Collision
Inelastic
Collision
Oblique
Collision
Perfectly
Inelastic
Collision
Partially
Inelastic
Collision
HEAD ON
COLLISIONS
HEAD ON
COLLISION
• It is the collision in the
straight line.
• Elastic Collision
• Its is the collision in which
bodies regain their original
shape after collision.
• Inelastic Collision
• I. Perfectly Inelastic
Collision : It's is the
collision in which
bodies moves
• together as a single body
after collision.
• II. Partially Inelastic
Collision : It's is the
collision in which
bodies moves
• independently, but there
shape gets deformed.
COEFFICIENT OF RESTITUTION
• When two objects collide head-on, their velocity of separation
after impact is in constant ratio to their velocity of approach
before impact.
• E = velocity of separation
velocity of approach
0≤e≤1 velocity of separation = e (velocity of approach)
• The constant e is called as the coefficient of restitution.
ELASTIC
COLLISION
IN
1DIMENSION
Calculation of velocities after collision
INELASTIC COLLISION IN ONE
DIMENSION
COLLISION IN TWO
DIMENSION/OBLIQUE
COLLISION
COLLISION IN
TWO DIMENSION
DERIVATION
SPECIAL
CASE
• when two particles of same
mass undergo perfectly elastic
collision in two dimension I.e
m1=m2
• θ+ ϕ = 90°
• hence we conclude that in a
perfectly elastic collision in
two dimension between two
particles of same mass the two
particles move along mutually
perpendicular directions after
the collision
• IN THIS CASE, THE FIRST
OBJECT, MASS , INITIALLY
MOVES ALONG THE -AXIS
WITH SPEED . ON THE OTHER
HAND, THE SECOND OBJECT,
MASS , INITIALLY MOVES AT
AN ANGLE TO THE -AXIS WITH
SPEED . AFTER THE COLLISION,
THE TWO OBJECTS
STICK TOGETHER AND MOVE OFF
AT AN ANGLE TO THE -AXIS
WITH SPEED .
MOMENTUM CONSERVATION
ALONG THE -AXIS YIELDS
• M1.VI1 + M2.VI2 COS ѲI=
(M1+M2)VF COS Ѳ F
• LIKEWISE, MOMENTUM
CONSERVATION ALONG THE -
AXIS GIVES
• M2.VI2 SIN ѲI= (M1+M2)VF
SIN Ѳ F
• KNOWING M1,M2, U1, U2
AND Ѳ WE CAN CALCULATE
FINAL VELOCITY V AND ITS
DIRECTION
QUESTION:
Q 1 - B A L L M O V I N G W I T H A S P E E D O F 9 M P E R
S E C O N D S T R I K E S A N D I D E N T I C A L B A L L A T R E S T
S U C H T H A T A F T E R T H E C O L L I S I O N T H E D I R E C T I O N
O F E A C H B O W L M A K E S A N A N G L E O F 3 0 D E G R E E
W I T H T H E O R I G I N A L L I N E O F T H E M O T I O N F I N D
T H E S P E E D O F T H E T W O B A L L S A F T E R C O L L I S I O N

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Collision (work, energy and power)

  • 4. HEAD ON COLLISION • It is the collision in the straight line. • Elastic Collision • Its is the collision in which bodies regain their original shape after collision.
  • 5. • Inelastic Collision • I. Perfectly Inelastic Collision : It's is the collision in which bodies moves • together as a single body after collision. • II. Partially Inelastic Collision : It's is the collision in which bodies moves • independently, but there shape gets deformed.
  • 6. COEFFICIENT OF RESTITUTION • When two objects collide head-on, their velocity of separation after impact is in constant ratio to their velocity of approach before impact. • E = velocity of separation velocity of approach 0≤e≤1 velocity of separation = e (velocity of approach) • The constant e is called as the coefficient of restitution.
  • 8. Calculation of velocities after collision
  • 9. INELASTIC COLLISION IN ONE DIMENSION
  • 10.
  • 12.
  • 14. SPECIAL CASE • when two particles of same mass undergo perfectly elastic collision in two dimension I.e m1=m2 • θ+ ϕ = 90° • hence we conclude that in a perfectly elastic collision in two dimension between two particles of same mass the two particles move along mutually perpendicular directions after the collision
  • 15. • IN THIS CASE, THE FIRST OBJECT, MASS , INITIALLY MOVES ALONG THE -AXIS WITH SPEED . ON THE OTHER HAND, THE SECOND OBJECT, MASS , INITIALLY MOVES AT AN ANGLE TO THE -AXIS WITH SPEED . AFTER THE COLLISION, THE TWO OBJECTS STICK TOGETHER AND MOVE OFF AT AN ANGLE TO THE -AXIS WITH SPEED . MOMENTUM CONSERVATION ALONG THE -AXIS YIELDS • M1.VI1 + M2.VI2 COS ѲI= (M1+M2)VF COS Ѳ F • LIKEWISE, MOMENTUM CONSERVATION ALONG THE - AXIS GIVES • M2.VI2 SIN ѲI= (M1+M2)VF SIN Ѳ F • KNOWING M1,M2, U1, U2 AND Ѳ WE CAN CALCULATE FINAL VELOCITY V AND ITS DIRECTION
  • 16. QUESTION: Q 1 - B A L L M O V I N G W I T H A S P E E D O F 9 M P E R S E C O N D S T R I K E S A N D I D E N T I C A L B A L L A T R E S T S U C H T H A T A F T E R T H E C O L L I S I O N T H E D I R E C T I O N O F E A C H B O W L M A K E S A N A N G L E O F 3 0 D E G R E E W I T H T H E O R I G I N A L L I N E O F T H E M O T I O N F I N D T H E S P E E D O F T H E T W O B A L L S A F T E R C O L L I S I O N