1. TORQUE
MEASUREMENT
NAME: JAIMIN AJITKUMAR KEMKAR
EN. NO.: 160123119014
SEM. AND BATCH: 4TH D2
SUBJECT: MECHANICAL MEASUREMENT AND METROLOGY (2141901)
GUIDED BY: PROF. NAMAN M. DAVE
2. CONTENTS
β’ INTRODUCTION OF TORQUE
β’ DIFFERENCE BETWEEN TORQUE, ANGULAR VELOCITY AND POWER
β’ METHODS FOR MEASURING TORQUE
3. INTRODUCTION OF TORQUE
οTorque is defined as a twisting force that tends to cause rotation.
or
οTorque is by definition a quantity that represents the tendency of a force to rotate an
object about an axis.
οUnit. ππ
οE.g. the force generated by an internal-combustion engine to turn a vehicle's drive or
shaft.
ο The torque may be computed by measuring
the force πΉ at a known radius π.
π = πΉπ
where, F = force (N)
r = radius from pivot point (r)
4. DIFFERENCE BETWEEN TORQUE,
ANGULAR VELOCITY & POWER
TORQUE ANGULAR VELOCITY POWER
Force that causes twisting
or turning moment.
angular displacement with
respect to time.
Power is the rate at which
work is done.
Crank shaft turning due to
torque.
Rotation of motor shaft.
the rate at which energy is
transferred by a force.
Notation: T Notation: N or π (omega) Notation: P
Unit: Nm Unit: RPM Unit: watts or horse power
5. METHODS FOR MEASURING
TORQUE
οTorque measuring devices are called as dynamometers.
οTorque measurement is usually associated with determination of
mechanical power, either power required to operate a machine or to
find out the power developed by the machine.
π =
2πππ
60
where,
o P = power developed by machine (watt)
o N = rotation of shaft (rpm)
o T = torque (Nm)
6. TYPES OF DYNAMOMETERS
β’ Absorption dynamometers:
β’ CLASSIFICATION:
1) Mechanical brakes
ο Prony brakes
ο Rope brakes
2) Hydraulic or fluid friction brakes
3) Eddy current dynamometer
β’ Driving dynamometers:
ο These are useful in determining performance characteristics of devices such as pumps and compression.
β’ CLASSIFICATION:
1) Torsion and belt dynamometers
2) Epicyclic train dynamometer
3) Strain gauge dynamometer
β’ Transmission dynamometers:
ο These are the passive devices placed at an appropriate location within a machine or in between the machine to
sense the torque at that location.
β’ CLASSIFICATION:
1) Electric cradled dynamometer
8. CONSTRUCTION
ο It consists of two wooden blocks placed around a pulley fixed to the shaft of an engine whose
power is required to be measured.
ο Blocks are clamped by means of bolts and nuts. A helical spring is provided between the nut
and the upper block to adjust the pressure on the pulley to control its speed.
ο The upper block has a long lever attached to it and carries a weight W at its outer end. A
counter weight is placed at the other end of the lever which balances the brake when unloaded.
ο In order to limit the motion of the lever, two stops provided.
WORKING
ο When the brake is to be operated, the long end of lever is loaded with suitable weights W and
nuts are tightened until the engine shaft runs at a constant speed and the lever is in horizontal
position.
ο Under these conditions, the moment due to the weight W must balance the moment of frictional
resistance between the blocks and the pulley.
9. ο LET,
ο W = weight at the outer end of the lever (Newton)
ο L = horizontal distance of the weight W from the center of the pulley (meter)
ο R = radius of the pulley (meter)
ο N = speed of the shaft (rpm)
ο Now, the moment of the frictional resistance or torque of the shaft,
ο π = π Γ πΏ (Nm)
π΅ππππ πππ€ππ =
πΓ2ππ
60
=
(πΓπΏ)Γ2ππ
60
(Watts)
οLIMITATIONS
οwhen the driving torque on the shaft is not uniform, this dynamometer is subjected to serve oscillations.
οAPPLIATIONS
οmeasuring power or torque developed by power source such as engines or electric motors.
10. CONSTRUCTION:
οIt consists of one, two or more ropes wound around the flywheel
or rim of a pulley fixed rigidly to the shaft of the engine.
οThe upper end is kept in position while the lower end of the
ropes is kept in position by applying a dead weight.
οIn order to prevent the slipping of the rope over the flywheel,
wooden blocks are placed at intervals around the circumference
of the flywheel.
WORKING
ο For the operation of the brake, the engine is made to run at a
constant speed.
ο The frictional torque due to rope, must be equal to the torque
being transmitted by the engine.
LET,
β’ W = weight at the end of the rope (N)
β’ S = spring balance reading (N)
β’ N = engine speed (rpm)
β’ D = diameter of the brake wheel (m)
β’ d = diameter of the rope (m)
β’ ( D + d ) = Effective diameter of the brake wheel
11. ο Then,
work/revolution = π‘ππππ’π Γ πππππ π‘π’ππππ πππ πππ£πππ’π‘πππ
= (π β π) Γ
π·+π
2
Γ 2π
= (π β π) Γ (π· β π) Γ π
work done per minuets = π β π π π· + π π
work done/ sec =
πβπ π π·βπ π
60
Brake power =
(πβπ)ππ·π
60Γ1000
(kW) or =
πΓ2ππ
60Γ1000
(ππ)
ADVANTAGE
ο Cheap and easy construction
LIMITATIONS
ο Its not accurate because of change in friction coefficient of the rope with temperature.
APPLICATIONS
ο This type of absorption dynamometer is most commonly used.
12. DRIVING DYNAMOMETERS
β’ Working principle:
These dynamometers measure power or torque and as well provide energy to operate the device to be
tested.
13. WORKING:
β’ it consists of a simple epicyclic train of gears, i.e. a spur gear.
β’ The spur gear is keyed to the engine shaft and rotates in anticlockwise direction.
β’ The annular gear is also keyed to the driving shaft and rotates in clockwise direction.
β’ The pinion or the intermediate gear meshes with both the spur and annular gears. The pinion
revolves freely on a lever.
β’ A weight w is placed at the smaller end of the lever in order to keep it in position.
β’ The tangential effort P exerted by the spur gear on the pinion and the tangential reaction of the
annular gear on the pinion are equal
β’ For equilibrium of the lever, taking moments about the fulcrum F
2π Γ π = π Γ πΏ or π =
πΓπΏ
2π
R = Pitch circle radius of the spur gear in meters, and
N = Speed of the engine shaft in rpm
β’ Torque transmitted,
π = π Γ π
14. β’ Now power π =
πΓ2ππ
60
=
(πΓπ )Γ2ππ
60
(Watts)
WORKING PRINCIPAL:
When power is being transmitted by the belt from one pulley to another, the tangential
effort on the driven pulley is equal to the difference between the tension in the tight and slack sides
of the belt.
ο A belt transmission dynamometer, is called a Froude or Throneycraft transmission dynamometer.
15. CONSTRUCTION:
β’ It consists of a pulley A (called driving pulley) which is rigidly fixed tothe shaft of an engine
whose power is required to be measured.
β’ There is another pulley B (called driven pulley) mounted on another shaft to which the power
from pulley A is transmitted. The pulleys
β’ A and B are connected by means of a continuous belt passing round the two loose pulleys C and
D which are mounted on a T-shaped frame.
β’ The frame is pivoted at E and its movement is controlled by two stops.
WORKING:
β’ Since the tension in the tight side of the belt (T1) is greater than the tension in the slack side of
the belt (T2),so the total force acting on the pulley C (i.e. 2T1) is greater than the total force
acting on the pulley D (i.e. 2T2).
β’ It is thus obvious that the frame causes movement about E in the anticlockwise direction.
β’ In order to balance it, a weight W is applied at a distance L from E on the frame.
β’ Now taking moments about the pivot E, neglecting friction,
2π1 Γ π = 2π2 Γ π + (π Γ πΏ) or π1 β π2 =
(πβπΏ)
2π
16. β’ Work done in one revolution= (π1 β π2)ππ· (Nm)
β’ workdone per minute= (π1 β π2)ππ·π (Nm)
β’ Brake power =
(π1βπ2)ππ·π
60
(Watts)
17. REFERANCES
TEXTS:
ο Mechanical measurement and instrumentation (R.K. RAJPUT)
ο WEB CONTENTS
ο BRITANICA
ο WIKIPEDIA
ο ME MECHANICAL
IMAGES:
ο GOOGLE IMAGIS
ο ME MECHANICAL