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Crank Sliding Link Cylinder
Mechanism
-by Dhaval Shukla (141080119050)
Abhishek Singh (141080119051)
Abhishek Singh (141080119052)
Aman Singh (141080119053)
Azhar Tai (141080119054)
-Mechanical Branch
-2nd Semester
-Engineering Graphics
Crank Sliding Link
Cylinder
Mechanism
Introduction
 A crank is an arm attached at
right angles to a rotating shaft
by which reciprocating
motion is imparted to or
received from the shaft.
 It is used to convert circular
motion into reciprocating
motion, or vice versa. The arm
may be a bent portion of the
shaft, or a separate arm or
disk attached to it.
Introduction
The shaft is rotating
the wheel drum into
reciprocal direction
which is reciprocal
motion produced by
crankshaft
Introduction
The cylinder
moves in two
directions either it
is up or down.
Exactly which
happens in crank
sliding link
cylinder
mechanism.
Function of Working
 Attached to the end of the
crank by a pivot is a rod,
usually called a connecting
rod.
 The end of the rod attached
to the crank moves in a
circular motion, while the
other end is usually
constrained to move in
a linear sliding motion.
Function of Working
 Almost
all reciprocating
engines use cranks
(with connecting rods)
to transform the back-
and-forth motion of the
pistons into rotary
motion. The cranks are
incorporated into
a crankshaft.
Use
 The Crank Sliding Link Cylinder Mechanism
is used in the reciprocating motion of the
vehicles which causes into the movement of
the piston inside the cylinder which
compressed after a fuel intake produces
combustion. E.g. Petrol Engine
Calculations
 The displacement of the end of the
connecting rod is approximately
proportional to the cosine of
the angle of rotation of the crank,
when it is measured from top dead
center (TDC).
 So the reciprocating motion created by
a steadily rotating crank and
connecting rod is
approximately simple harmonic
motion:
Calculations
 where x is the distance of the end of the
connecting rod from the crank axle, l is the
length of the connecting rod, r is the length of
the crank, and α is the angle of the crank
measured from top dead center (TDC).
 Technically, the reciprocating motion of the
connecting rod departs
from sinusoidal motion due to the changing
angle of the connecting rod during the cycle,
and is expressed as:
cosx r l 
Calculations
 This difference becomes significant in
high-speed engines.
 The mechanical advantage of a crank, the
ratio between the force on the connecting
rod and the torque on the shaft, varies
throughout the crank's cycle. The
relationship between the two is
approximately:
2 2 2
cos sinx r l r   
Calculations
 where T is the torque and F is the force on
the connecting rod.
 But in reality, the torque is maximum at crank
angle of less than α = 90° from TDC for a
given force on the piston.
 One way to calculate this angle is to find out
when the conrod small end (piston) speed
becomes the fastest in downward direction
given a steady crank rotational velocity.
sinFr 
Calculations
 Piston speed x' is expressed as:
2
2 2
sin cos
' sin
sin
r
x r
l r
 


  

Disadvantage
 When the crank is driven by the
connecting rod, a problem arises
when the crank is at top dead
centre (0°) or bottom dead
centre (180°).
 At these points in the crank's cycle, a
force on the connecting rod causes no
torque on the crank. Therefore if the
crank is stationary and happens to be
at one of these two points, it cannot be
started moving by the connecting rod.
Disadvantage
 For this reason, in steam locomotives,
whose wheels are driven by cranks,
the connecting rods are attached to
the wheels at points separated by
some angle, so that regardless of the
position of the wheels when the
engine starts, at least one connecting
rod will be able to exert torque to start
the train.
Your Suggestions are
Accepted!

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Crank Sliding Link Cylinder Mechanism

  • 1. Crank Sliding Link Cylinder Mechanism -by Dhaval Shukla (141080119050) Abhishek Singh (141080119051) Abhishek Singh (141080119052) Aman Singh (141080119053) Azhar Tai (141080119054) -Mechanical Branch -2nd Semester -Engineering Graphics
  • 3. Introduction  A crank is an arm attached at right angles to a rotating shaft by which reciprocating motion is imparted to or received from the shaft.  It is used to convert circular motion into reciprocating motion, or vice versa. The arm may be a bent portion of the shaft, or a separate arm or disk attached to it.
  • 4. Introduction The shaft is rotating the wheel drum into reciprocal direction which is reciprocal motion produced by crankshaft
  • 5. Introduction The cylinder moves in two directions either it is up or down. Exactly which happens in crank sliding link cylinder mechanism.
  • 6. Function of Working  Attached to the end of the crank by a pivot is a rod, usually called a connecting rod.  The end of the rod attached to the crank moves in a circular motion, while the other end is usually constrained to move in a linear sliding motion.
  • 7. Function of Working  Almost all reciprocating engines use cranks (with connecting rods) to transform the back- and-forth motion of the pistons into rotary motion. The cranks are incorporated into a crankshaft.
  • 8. Use  The Crank Sliding Link Cylinder Mechanism is used in the reciprocating motion of the vehicles which causes into the movement of the piston inside the cylinder which compressed after a fuel intake produces combustion. E.g. Petrol Engine
  • 9. Calculations  The displacement of the end of the connecting rod is approximately proportional to the cosine of the angle of rotation of the crank, when it is measured from top dead center (TDC).  So the reciprocating motion created by a steadily rotating crank and connecting rod is approximately simple harmonic motion:
  • 10. Calculations  where x is the distance of the end of the connecting rod from the crank axle, l is the length of the connecting rod, r is the length of the crank, and α is the angle of the crank measured from top dead center (TDC).  Technically, the reciprocating motion of the connecting rod departs from sinusoidal motion due to the changing angle of the connecting rod during the cycle, and is expressed as: cosx r l 
  • 11. Calculations  This difference becomes significant in high-speed engines.  The mechanical advantage of a crank, the ratio between the force on the connecting rod and the torque on the shaft, varies throughout the crank's cycle. The relationship between the two is approximately: 2 2 2 cos sinx r l r   
  • 12. Calculations  where T is the torque and F is the force on the connecting rod.  But in reality, the torque is maximum at crank angle of less than α = 90° from TDC for a given force on the piston.  One way to calculate this angle is to find out when the conrod small end (piston) speed becomes the fastest in downward direction given a steady crank rotational velocity. sinFr 
  • 13. Calculations  Piston speed x' is expressed as: 2 2 2 sin cos ' sin sin r x r l r        
  • 14. Disadvantage  When the crank is driven by the connecting rod, a problem arises when the crank is at top dead centre (0°) or bottom dead centre (180°).  At these points in the crank's cycle, a force on the connecting rod causes no torque on the crank. Therefore if the crank is stationary and happens to be at one of these two points, it cannot be started moving by the connecting rod.
  • 15. Disadvantage  For this reason, in steam locomotives, whose wheels are driven by cranks, the connecting rods are attached to the wheels at points separated by some angle, so that regardless of the position of the wheels when the engine starts, at least one connecting rod will be able to exert torque to start the train.