BASICS OF HYDRAULICS BASICS OF HYDRAULICS 1) DEFINITIONS 1.1) HYDRAULICS 1.2) CLASSIFICATION 1.2.1) HYDROSTATICS BAS
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BASICS OF HYDRAULICS
BASICS OF HYDRAULICS 1)
DEFINITIONS 1.1) HYDRAULICS 1.2) CLASSIFICATION 1.2.1) HYDROSTATICS
BASIC DEFINITIONS & FORMULAE
1.2.2) HYDRODYNAMICS 1.3) FORCE , PRESSURE , AREA 1.4) PASCAL’S LAW 2)
MULTIPLICATION OF FORCES 2.1) BRAMAH’S PRESS 2.2) LAW OF CONSERVATION OF ENERGY
3)
HYDRAULIC POWER TRANSMISSION 3.1) LINEAR ACTUATOR 3.2) ROTARY ACTUATOR
USES OF HYDRAULIC S
BASICS OF HYDRAULICS 4)
ADVANTAGES OF HYDRAULICS 4.1) SPEED CONTROL 4.2) DIRECTION CONTROL 4.3) FORCE CONTROL 4.4) OVERLOAD PROTECTION 4.5) COMPACTNESS
5)
HOW PRESSURE IS CREATED
ADVANTAGES OF HYDRAULICS
PRACTICAL DETAILS IN HYDRAULIC S
HYDRAULICS HYDRO
AULUS
( meaning Water ) ( meaning Pipe ) HYDRAULICS : Work done by fluids in pipes.
H y d r a u lic s is C la s s if e d a s H Y D R O S T A T IC S
H Y D R O D Y N A M IC S
HYDROSTATICS HYDROSTATICS FORCE F1
Eg.:F1 = 1 Kg A1 = 1 Cm2 P = F1 = 1 Kg A1 1 Cm2
AREA A1
= 1 Kg / Cm2 ( Same Pressure P) A2 = 10 Cm2 F2 = P x A2 = 1
x 10
= 10 Kg
FORCE F2
AREA A2
HYDRODYNAMICS LIQUID AT HIGH VELOCITY NOZZLE
TURBINE
PRESSURE •
IN ORDER TO DETERMINE THE TOTAL FORCE EXERTED ON A SURFACE WE NEED TO KNOW THE PRESSURE OR FORCE PER UNIT AREA.
•
PRESSURE = FORCE AREA
P
=
FORCE IN KILOGRAMS ( Kg ) AREA IN SQ. CM ( Cm2 ) PRESSURE IN KILOGRAM / SQ.CM (Kg / Cm2 )
F A
•
FORCE = PRESSURE x AREA
•
THE ATMOSPHERIC AIR EXERTS UNIFORM PRESSURE ALL ROUND. THIS PRESSURE IS APPROX. 1 Kg / Cm2 AND P IS DENOTED AS 1 BAR ( BAROMETER )
F A
PASCAL’S LAW PRESSURE APPLIED ON A CONFINED FLUID IS TRANSMITTED UNDIMINISHED IN ALL DIRECTIONS AND ACTS WITH EQUAL FORCE ON EQUAL AREAS AND AT RIGHT ANGLES TO THEM. •
PRESSURE APPLIED ON A
•
FRENCH SCIENTIST PASCAL DISCOVERED THIS LAW IN THE 17th CENTURY.
•
RELATES TO USE OF CONFINED FLUID IN TRANSMITTING POWER MODIFYING MOTION MULTIPLYING FORCE.
CONFINED FLUID IS TRANSMITTED UNDIMINISHED IN ALL DIRECTIONS ACTS WITH EQUAL FORCE ON EQUAL AREAS AND AT RIGHT ANGLES TO THEM
PASCAL’S LAW
FORCE F1 SMALL AREA A1
P = F1 A1
PRESSURE P
F2 = P x A 2
LARGE AREA FORCE F2
A2
BRAMAH’S PRESS
HYDRAULIC LEVERAGE
10 kg
10 Kg ON A 1Cm2 AREA
1Cm2
INPUT
100 kg
PRESSURE DEVELOPED THROUGHOUT IS 10 Kg / Cm2
10 Cm2
THE FORCES ARE PROPORTIONAL TO THE PISTON AREAS 100 Kg 10 Kg = 10 Cm2 1 Cm2
OUTPUT
MECHANICAL LEVERAGE 10 Kg
100 Kg
A LOAD OF 10 Kg HERE 1 0
THIS PRESSURE SUPPORTS A WT OF 100 Kg IF AREA IS 10 Cm2
1
WILL BALANCE A LOAD OF 100 Kg HERE
LAW OF CONSERVATION OF ENERGY MOVING THE SMALL PISTON 10 Cm DISPLACES 1 Cm2 x 10 Cm = 10 Cm3 OF LIQUID
10 Cm
1Cm2
100 kg 10 Cm2
1 Cm
Q=Axh
10 kg
10 Cm OF LIQUID WILL MOVE LARGER PISTON ONLY 1Cm. 10 Cm2 x 1 Cm = 10 Cm3
WORK DONE = FORCE x DISTANCE MOVED
W=Fxd
W=Fxd
W=Fxd
= 10 Kg x 10 Cm
= 100 Kg x 1 Cm
= 100 Kg-Cm
= 100 Kg-Cm
ENERGY CAN NEITHER BE CREATED NOR DESTROYED. WHAT IS GAINED BY FORCE IS SACRIFICED IN THE DISTANCE MOVED.
HYDRAULIC POWER TRANSMISSION LINEAR ACTUATOR PUMP
LOAD
PISTON & ROD TO RESERVOIR
ROTARY ACTUATOR PUMP
HYDRO MOTOR
ADVANTAGES OF HYDRAULICS SPEED CONTROL MAXIMUM SPEED (No speed control ) 10 lpm Q = Ax V PUMP
THIS VOL. IS 10 Lts.
PISTON MOVES “X” Cm IN 1 min.
Q Flow (Cm3/min) A Area ( Cm2 ) V Velocity (Cm/ min ) (Speed control )
FLOW CONTROL VALVE
10 lpm PUMP
5 lpm
RELIEF VALVE ACTUATOR GETS ONLY 5 LPM AND TRAVELS “X/2” Cm IN ONE MIN.
ADVANTAGES OF HYDRAULICS HYDRAULIC DRIVES ARE REVERSIBLE DIRECTION CONTROL PUMP
RELIEF VALVE
DIRECTIONA L
THE CYLINDER ROD EXTENDS
VALVE
PUMP
RELIEF VALVE
DIRECTIONAL VALVE
THE CYLINDER ROD RETRACTS
ADVANTAGES OF HYDRAULICS
OVER LOAD PROTECTION RELIEF VALVE PROTECTS THE SYSTEM BY MAINTAINING THE SYSTEM SET PRESSURE.
ANY INCREASE IN PRESSURE IN SYSTEM IS RELEAVED TO TANK . ( MOMENTARILY DIVERTING FLOW TO THE TANK. )
THUS OVERLOAD PROTECTION IS ACHIEVED.
PRESSURE HEAD PUMP INLET LOCATIONS OIL LEVEL ABOVE PUMP CHARGES INLET
PRESSURE HERE IS 0.85 x 100 gm / Cm2 = 0.085 Kg / Cm2
100 Cm
PUMP
OIL LEVEL BELOW PUMP REQUIRES VACUUM TO “LIFT “ OIL
100 Cm
INLET
OUTLET
INLET
OUTLET
PUMP
THERE MUST BE A VACUUM EQUIVALENT TO 0.085 Kg / Cm2 TO LIFT THE OIL PUMP MECHANISM CREATES THE LOWER PRESSURE CONDITION.
HOW PRESSURE IS DEVELOPED NO PRESSURE
NO RESTRICTION
PUMP RELIEF VALVE
Set at 100 Kg/Cm2
PRESSURE BUILDS UP
WITH RESTRICTION
PUMP RELIEF VALVE
Set at 100 Kg/Cm2
PRESSURE BUILDS UPTO RELIEF VALVE SETTING (100 Kg / Cm2)
CLOSING
PUMP RELIEF VALVE
Set at 100 Kg/Cm2
PARALLEL FLOW PATHS THE OIL CAN CHOOSE 3 PATHS
10 A PUMP
B
C
OIL TAKES THE PATH OF LEAST RESISTANCE
20
PUMP
10 BAR OPENS VALVE A 20 BAR OPENS VALVE B
30 BAR OPENS VALVE C IF FLOW IS BLOCKED BEYOND “ A”
OIL WILL FLOW THRO “B” WHEN PRESSURE REACHES 20 BAR
SERIES RESISTANCE ADD PRESSURE A 10 BAR
0
P1 = 0
P2 = ( P1 + 10 )
B
10
=
0 + 10
= 10 BAR
20 BAR P3 = ( P2 + 20 )
C
30
= 10 + 20 = 30 BAR
30 BAR
P = ( P3 + 30 ) PUMP
60
= 30 + 30 = 60 BAR
PRINCIPLES OF FLOW HOW FLOW IS MEASURED ? VELOCITY FLOW ( FLOW RATE ) FLOW RATE AND SPEED FLOW AND PRESSURE DROP LAMINAR AND TURBULENT FLOW BERNOULLI’S PRINCIPLE FLOW IS THE ACTION IN THE HYDRAULIC SYSTEM THAT GIVES THE ACTUATOR ITS MOTION. PRESSURE GIVES THE ACTUATOR ITS FORCE , BUT FLOW IS ESSENTIAL TO CAUSE MOVEMENT. FLOW IN THE HYDRAULIC SYSTEM IS CREATED BY THE PUMP PRESSURE INDICATES WORK LOAD.
VELOCITY : IS THE AVERAGE SPEED OF THE FLUID’S PARTICLES PAST A GIVEN POINT OR THE AVERAGE DISTANCE THE PARTICLES TRAVEL PER UNIT OF TIME. Unit :m/Sec or m / min ( Metres / Sec or Metres/min )
FLOW RATE : IS THE VOLUME OF FLUID PASSING A POINT IN A GIVEN TIME. Unit: Cm3 / min or l / min ( cc / minute or litres / min )
SPEED OF AN ACTUATOR DEPENDES ON THE ACTUATOR SIZE AND RATE OF FLOW INTO IT. Q = Ax V FLOW IN Cm3 / min : AREA IN Cm 2
:
VELOCITY IN Cm / min
FLOW AND PRESSURE DROP MAX. PRESSURE HERE BECAUSE OF THE HEAD OF THE FLUID
SUCEEDINGLY LOWER LEVEL OF LIQUID SHOWS PRESSURE IS REDUCED AT POINTS DOWNSTREAM FROM SOURCE.
PRESSURE GRADIENT
FRICTION IN PIPE DROPS PRESSURE
PRESSURE IS ZERO HERE AS THE FLUID FLOWS OUT UNRESTRICTED
DUE TO EFFECT OF FRICTION RECOMMENDED VELOCITY RANGES ARE : 1.) PUMP INLET LINE
0.6 ~ 1.2 metres / Second
2.) WORKING LINE ( PR. LINES) :
2~6
metres / Second
NOR DOES A GRADUAL CHANGE IN DIRECTION.
LAMINAR FLOW
LOW VELOCITY FLOW IN A STRAIGHT PIPE IS STREAMLINED. THE FLUID PARTICLES MOVE PARALLEL TO FLOW DIRECTION.
TURBULENT FLOW
THE FLOW MAY START OUT STREAMLINED.
AN ABRUPT CHANGE IN CROSSSECTION MAKES IT TURBULENT.
SO DOES AN ABRUPT CHANGE IN DIRECTION.
NON PARALLEL PATHS OF PARTICLES INCREASE RESISTANCE TO FLOW.