Module 3.pptx

42

Transcript of Module 3.pptx

Page 1: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 1/42

Page 2: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 2/42

is a measure of average KINETIC ENERGY of the

particles that makes up a body.

is the ability of one body to transfer thermal energy

to another body.

It is the Degree of HOTNESS of a body.

Page 3: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 3/42

Page 4: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 4/42

Page 5: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 5/42

TEMPERATURE - Measurement Scales

Relative Scales

Fahrenheit (°F)

Celsius (°C)

Absolute Scales

Rankine (°R)

Kelvin (K)

Page 6: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 6/42

100:C 

373:K 

273:K 

255:K 

0:C 

-18:C 

-273:C  0:K 

-460:F  0:R 

0:F 

32:F 

460:R 

492:R 

672:R 212:F  Fahrenheit[°F] = [°C] · 9/5 + 32

Celsius[°C] = ([°F] − 32) x 5/9

Kelvin[K] = [°C] + 273.15

Rankine[°R] = [°F] + 459.67

TEMPERATURE - Measurement Scales

Page 7: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 7/42

Mechanical Methods Filled – in – System thermometers

Bimetallic Strips/ Expansion of materials

Bulb & Capillary Sensor

Electrical Methods

RTD Thermocouple

Thermistor

Pyrometers etc.

TEMPERATURE - Measurement Methods

Page 8: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 8/42

Bimetallic Strip Thermometer

Suppose metal A has a smaller coefficient of thermal expansion than

does metal B. As temperature increases, metal B expands more than

does metal A, causing the bimetallic strip to curl upwards as sketched.

Two dissimilar metals are bonded together into

what is called a bimetallic strip.

Page 9: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 9/42

Bimetallic Thermometer (Expansion of solids)

Effect of unequal expansion of a bimetallic strip

Different metals have difference coefficient.

Configured as spiral or helix for compactness

Can be used with a pointer to make an inexpensive

compact rugged thermometer.

Page 10: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 10/42

Bimetallic Thermometer (Expansion of solids)

Effect of unequal expansion of a bimetallic strip

Page 11: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 11/42

Bimetallic Thermometer (Expansion of solids)

Page 12: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 12/42

One common application of bimetallic strips is in air-conditioningthermostats, where a bimetallic strip is used as the arm of a switch

between electrical contacts. As the room temperature changes, the

bimetallic strip bends as discussed above. When the bimetallic strip

bends far enough, it makes contact with electrical leads which turn the

heat or air conditioning on or off.

Bimetallic Strip as Thermostat

Page 13: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 13/42

Liquid-in-Glass Thermometer 

The most common and well-known thermometer

is the liquid-in-glass thermometer.

As the temperature rises, the liquid expands,

moving up the tube. The scale is calibrated to

read temperature directly. Usually, mercury or

some kind of alcohol is used for the liquid. 

Mercury thermometers can range from -38F to 1110 F

Alcohol thermometers range from -328 F to 1110 F

Other thermometer fill fluids include Benzene & ether

Page 14: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 14/42

Filled-in-System Thermometers 

Similar operation as the

liquid in glass system.

Filled system thermometers,

also called pressure

thermometers.

Page 15: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 15/42

Sensing element is a capillary tube

filled with a liquid or gas which

expands with an increase in

temperature.

This sensing element delivers a

motion of physical change that is

applied to the control element

which either indicates, records, or

by comparing the signal to a setpoint can be used to control the

temperature of a process.

How it works? 

Page 16: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 16/42

Elements

Bulb

Capillary tube

Pressure element

Scale

Page 17: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 17/42

 

Class I (A,B) – Liquid filled (Excluding Mercury)

Class II (A,B,C,D)  – Vapour filled

Class III (A,B)  – Gas filled

Class IV - Deleted

Class V (A,B) – Mercury Filled

Filled-in-System Thermometers - TYPES 

Page 18: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 18/42

Filled-in-System Thermometers - TYPES 

Temperature Range Response

Class I: -125 F to + 600 F Slowest

Class II: -40 to 32 or 32 to 600 F Fastest Class III: -450 F to +1400 Fast

Class V: -40 F to +1200 F Fast

Page 19: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 19/42

The big advantage of the filled system is that

it places the sensor in one place and the

signal processing equipment on another

Page 20: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 20/42

Class I (Liquid Filled) Systems 

Liquid Range (0C)

Ethyl Alcohol -45 to 150

Xylene -40 to 400

Ether (Ethyl) 20 to 90

Toulene -80 to 250

Page 21: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 21/42

Sensing bulb partially filled with volatile

fluid.

Common fluids include: methyl chloride,

ether, butane, hexane, propane,toluene, sulfur dioxide, water etc.

Based upon the principle that in a

system containing only a liquid and its

vapor, at a given temperature, a given

pressure will exist in the system,

regardless of system volume.

Actual temperature measurement

occurs at interface between liquid and

vapor.

Class II (Vapour Filled) Systems 

Page 22: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 22/42

May exhibit erratic operation when temperature

being measured swings above and below ambient

temperature.

Offers good reliability, inherently accurate, non-uniform scales (non-linear).

Class II (Vapour Filled) Systems … 

Page 23: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 23/42

Utilizes perfect gas law PV = nRT

Constant volume thermometers.

When temperature raised at constant volume pressureraises to operate Bourden gauge.

Helium approximates perfect gas, but tends to leak and isnot often used

Nitrogen usually is used

Compensation generally not necessary if a large bulb is

used.

Class III (Gas Filled) Systems 

Page 24: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 24/42

1. Ambient Temperature Effect

2. Head or Elevation Effect

3. Barometric Effect

4. Immersion Effect

5. Radiation Effect

Filled-in-System Thermometers

ERRORS 

Page 25: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 25/42

The change in ambient temperature causes volume

changes in the capillary and the pressure spring cases

error in measurement.

Its value is given by tE = (Vctc+Vptp)/Vb

where c = capillary; p = pressure spring; b = bulb;

E = error; t=change in temperature; V=Volume

1. Ambient Temperature Effect 

Page 26: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 26/42

If the thermometer bulb is placed at a different height with

respect to the pressure spring, elevation error arises.

For the bulb at higher position, pressure reading is also high.

The error in % span,

2. Head/Elevation Error 

h = height difference;

ρ=fluid density

Kb&kf  = bulb & fluid stiffnesses

% Es = 100hρ(kb+kf )Vb/∆ 

= 100hρ(kb+kf )/(Rδ)

Page 27: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 27/42

Due to atmospheric pressure changes, changes the

effective differential pressure at the pressure spring.

For a pressure change ∆p in the system and a

barometric pressure change of ∆pB, error in percentage

of the span of ts, 

tb= 100 ∆pB ts/∆p 

3. Barometric Effect 

Page 28: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 28/42

If the bulb is not properly or fully immersed in the

process and the head of the bulb is properly insulated,

heat from the bulb is lost due to conduction throughthe extension neck and thermal well causing error.

the error is roughly proportional to the unexposed area

of the bulb. 

4. Immersion Effect 

Page 29: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 29/42

Occurs due to the temperature difference between the

bulb and the other solid bodies around it. 

5. Radiation Error 

Page 30: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 30/42

CASE COMPENSATION

FULL COMPENSATION (CASE+CAPILLARY COMPENSATION) 

COMPENSATION TECHNIQUES

Page 31: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 31/42

CASE COMPENSATION

Inserting a bimetal strip between the free end of Bourden Gauge

and the pointer.

The deflection of the bimetal strip due to ambient temperature

is in such a way that it compensates the deflection of the

Bourden Gauge due to ambient temperature effect.

Page 32: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 32/42

FULL COMPENSATION

Page 33: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 33/42

FULL COMPENSATION… 

A dummy system excluding bulb is arranged by side.

The dummy system provides a rotation exactly equal in

magnitude but opposite in direction compared to the ambient

temperature effect on the measurement system.

Page 34: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 34/42

Advantages

Self Contained. They do not require auxiliary power source.

They are simple, rugged, lasting and have minimum

possibility of being damaged during shipping andinstallation.

Inexpensive due to simple design.

Sensitivity and Speed of response fairly good.

They can be designed to deliver significant power to drive

indicating or controlling mechanisms, including valves.

The capillary allows considerable separation between the

point of measurement and the point of indication.

Filled-in-System Thermometers 

Page 35: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 35/42

Disadvantages

In the case of system failure entire units need to be replaced.

Many applications may not allow large bulb volume within the

measured medium. Performance characteristics vary for different liquids, so care

should be taken for particular application.

The maximum temperature is limited compared to electrical

systems. The separation of the sensing and indicating elements is

limited compared to electrical systems.

Electronic sensors are more preferred due to flexibility,

distant measurement, cost etc.

Filled-in-System Thermometers 

Page 36: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 36/42

Electrical MethodsElectrical Temperature Transducers

Page 37: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 37/42

Thermistor, a word formed by combining thermal with

resistor, is a temperature-sensitive resistor fabricated from

semiconducting materials.

The resistance of thermistors decreases proportionally withincreases in temperature.

The operating range can be -200°C to + 1000°C

Page 38: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 38/42

The thermistors can be in the shape of a rod, bead or

disc.

Manufactured from oxides of nickel, manganese, iron,

cobalt, magnesium, titanium and other metals.

Page 39: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 39/42

The word that best describes the thermistors is

“sensitive” 

Page 40: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 40/42

Advantages:

Small sizes and fast response

Low cost

Suitability for narrow spans

Disadvantages:

More susceptible to permanent decalibration at high

temperatures.

Use is limited to a few hundred degrees Celsius.

Respond quickly to temperature changes, thus,

especially susceptible to self-heating errors.

Very fragile

Page 41: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 41/42

RTD (Resistance Temperature Detector) is a temperature

sensitive resistor.

It is a positive temperature coefficient device, which

means that the resistance increases with temperature.

The resistive property of the metal is called its

resistivity.

The industry standard is the platinum wire RTD

(Pt100) whose base resistance is exactly 100.00

ohms at 0.0 °C.

Page 42: Module 3.pptx

7/27/2019 Module 3.pptx

http://slidepdf.com/reader/full/module-3pptx 42/42

linear temperature sensors.

Resistance Vs temperature characteristics are stable andreproducible.

linear positive temperature coefficient (-200 to 800°C).

very accurate and suitable for use as a secondarystandard.