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SEEBecK EFFECT
      &
PETLIER EFFECT




        PRESENTED BY:
        VISHAL CHATURANI
        BSc(Engg.) MECHANICAL
        ROLL NO.- 114089
           S No.-105
Thermoelectric Phenomena
Electrically conductive materials exhibit
  three types of
thermoelectric phenomena:
• the Seebeck effect,
• the Peltier effect, and
• the Thomson effect.
SEEBECK EFFECT


 Differential
Thermocouple


   Vab
α=
   ΔT
SEEBECK EFFECT
• The Seebeck effect is the conversion
  of temperature differences directly into electricity
• It is named after German physicist Thomas Johann
  Seebeck
• in 1821 he discovered that a compass needle would be
  deflected by a closed loop formed by two metals joined in
  two places, with a temperature difference between the
  junctions.
• This was because the metals responded differently to the
  temperature difference, creating a
  current loop and a magnetic field.
• Seebeck did not recognize there was an electric
  current involved, so he called the phenomenon the
  thermomagnetic effect. Danish physicist Hans
  Christian Ørsted rectified the mistake and coined the
  term "thermoelectricity".
Cause of seebeck effect

• As we know that no of free electrons per unit volume
  and their average velocity varies from one metal to
  another .
• At the junction of two dissimilar metals, electrons
  migrate in one direction across the junction.
• It sets up an opposing electric field .
• As a result a fixed potential difference is developed .
• This effect is called Seebeck effect.
• The combination of two metals in such a
  manner is called thermocouple
• The e.m.f generated in a thermocouple is
  known as thermo e.m.f
• The current which flows along the closed
  circuit is called thermo electric current
Cause (Contd.)

• Since a migration of charges creates an electric
  potential, the buildup of charged carriers onto the
  cold side eventually ceases at some maximum
  value since the electric field is at equilibrium.
• An increase in the temperature difference
  resumes a buildup of charge carriers on the cold
  side, leading to an increase in the thermoelectric
  voltage, and vice versa.
 The voltage created by this effect is on the order of
  several micro volts per Kelvin difference.
 One such combination, copper-constantan, has a
  Seebeck coefficient of 41 microvolt per Kelvin at
  room temperature.
 S is positive when the direction of electric current is
  same as the direction of thermal current
Thermoelectric series
• For a given temperature range, the thermo e.m.f induced
  is different for different metal combinations.
• Seebeck arranged 35 metals in a series in such away
  when any two form a thermocouple:-
• Current will flow through the cold junction from the one
  that occurs first in series to the other that occurs later in
  series
• Between 0oC & 1000C the thermoelectric series is:

     Antimony, Fe, Cd, Zn, Ag, Au, Rb,Mo,Cr,Sn,Pb,Hg,M
     n,Cu,Pt,Cob,
Variation of thermoelectric E.M.F. with
                 temperature
• Tn =neutral temperature(constant for a
  given thermocouple)
• Ti =inversion temperature(beyond which
  e.m.f. starts increasing in opp. direction)
• Ti – Tn = Tn – T0
                  Thermo e.m.f.
1.   Law of intermediate metal: if the junction of the
     thermocouple is opened and a third metal is
     inserted, the e.m.f. for the couple AB remains the
     same i.e. without introducing C provided both the
     junction of the third metal C are at the same
     temperature.

                       B                     A
                                  c
2.Law of intermediate or successive
   temperatures : the e.m.f for a thermo-
   couple between temperatures t1 and t2 is
   equal to the sum of e.m.fs (seebeck) for any
   number of successive steps into which the
   given range of temperatures may be divided.
   Thus

      eᶿ1ᶿn =eᶿ1ᶿ2 + eᶿ2ᶿ3 + eᶿ3ᶿ4 +…..eᶿn-1ᶿn
Experimental demonstration of
                 seebeck effect
In this experiment , two rods of bismuth & antimony
   are arranged in the form of cross “X”
• Firstly, closed key “K1”.
• Current starts flowing, making the
   junction hot.
 Temperature difference is obtained.
 Open K1 and close K2.
 Deflection is shown by galvanometer ,
   thus confirming the seebeck effect
Peltier Effect
                                 Electric Current




 Difference in      Material A
                                                       Heat
                                                    Absorbed or
 εF between                                          Expelled
Materials A and B   Material B
Peltier effect
• In 1834, a French watchmaker and part time
  physicist, Jean Peltier found that an electrical
  current would produce a temperature gradient at
  the junction of two dissimilar metals
•
•                       when the current direction was
  r                     reversed, the cold junction
  w                     would get hot while the hot
  junction w            would get cold.
Cause of peltier effect
When a current flows across the junction of two
metals, it gives rise to an absorption or liberation of
heat, depending on the direction of the current. i.e.
Applying a current (e- carriers) transports heat from
the warmer junction to the cooler junction.
As an example of the Peltier effect,
consider the circuit shown here.
Under these conditions, it is
observed, as indicated in the
diagram,    that   the    right-hand
junction is heated. It shows, in
other words, that electrical energy
is being transformed into heat
energy. Meanwhile, heat energy is
transformed into electrical energy
at the left junction, thereby
causing it to be cooled. When the
current   is   reversed,    heat   is
absorbed at the right junction and
produced at the left one.
• The rate of evolution of or absorption of heat is
  proportional to the current &thus the peltier effect
  is reversible.
• If direction of current is changed then the peltier
  effect is also reversed.
• The energy absorbed or evolved at one of the
  junctions of the two dissimilar metals when one
  ampere of current flows for one second is called
  Peltier coefficient ,denoted by ∏
   In this experiment, two rods of bismuth and
    antimony are joined as shown.
   A differential air
    thermometer is
    placed with its two
    bulbs at
    junctions A and B.
   When no current flows through the thermocouple
    , the junctions A & B are at same temperature.
    Also Hg(mercury) pellet in the thermometer lies
    symmetrically at the centre.
   When large current is passed through the
    thermocouple , then there will be:
    ◦ Evolution of heat at junction A.
    ◦ Absorption of heat at junction B.
    ◦ Hg pellet moves to one direction
   If direction of current is changed the pellet moves
    in the opp. Direction indicating that now A has
    become cold and B has become hot.
Applications

 Seebeck effect
• The Seebeck effect is used in the thermoelectric
  generator, which functions like a heat engine
• These have a use in power plants for converting waste
  heat into additional power (a form of energy recycling).
• in automobiles as automotive thermoelectric
  generators (ATGs) for increasing fuel efficiency.
• Space probes often use radioisotope thermoelectric
  generators with the same mechanism but using
  radioisotopes to generate the required heat difference.
Peltier effect
• The Peltier effect can be used to
  create a refrigerator which is
  compact and has no circulating
  fluid or moving parts
• such refrigerators are useful in
  applications where their
  advantages out weigh the
  disadvantage of their very low
  efficiency.
Applications
Water/Beer Cooler                      Cryogenic IR Night Vision

                            Si bench



                       TE




                                            Electronic Cooling
Cooled
Car Seat

                    Laser/OE Cooling




                                              25
Temperature measurement

• Thermocouples and thermopiles are devices
  that use the Seebeck effect to measure the
  temperature difference between two objects,
  one connected to a voltmeter and the other to
  the probe.
• The temperature of the voltmeter, and hence
  that of the material being measured by the
  probe.
THANK
   YOU

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Seebeck effect & peltier effect

  • 1. SEEBecK EFFECT & PETLIER EFFECT PRESENTED BY: VISHAL CHATURANI BSc(Engg.) MECHANICAL ROLL NO.- 114089 S No.-105
  • 2. Thermoelectric Phenomena Electrically conductive materials exhibit three types of thermoelectric phenomena: • the Seebeck effect, • the Peltier effect, and • the Thomson effect.
  • 3.
  • 5. SEEBECK EFFECT • The Seebeck effect is the conversion of temperature differences directly into electricity • It is named after German physicist Thomas Johann Seebeck • in 1821 he discovered that a compass needle would be deflected by a closed loop formed by two metals joined in two places, with a temperature difference between the junctions. • This was because the metals responded differently to the temperature difference, creating a current loop and a magnetic field.
  • 6. • Seebeck did not recognize there was an electric current involved, so he called the phenomenon the thermomagnetic effect. Danish physicist Hans Christian Ørsted rectified the mistake and coined the term "thermoelectricity".
  • 7. Cause of seebeck effect • As we know that no of free electrons per unit volume and their average velocity varies from one metal to another . • At the junction of two dissimilar metals, electrons migrate in one direction across the junction. • It sets up an opposing electric field . • As a result a fixed potential difference is developed .
  • 8. • This effect is called Seebeck effect. • The combination of two metals in such a manner is called thermocouple • The e.m.f generated in a thermocouple is known as thermo e.m.f • The current which flows along the closed circuit is called thermo electric current
  • 9. Cause (Contd.) • Since a migration of charges creates an electric potential, the buildup of charged carriers onto the cold side eventually ceases at some maximum value since the electric field is at equilibrium. • An increase in the temperature difference resumes a buildup of charge carriers on the cold side, leading to an increase in the thermoelectric voltage, and vice versa.
  • 10.  The voltage created by this effect is on the order of several micro volts per Kelvin difference.  One such combination, copper-constantan, has a Seebeck coefficient of 41 microvolt per Kelvin at room temperature.  S is positive when the direction of electric current is same as the direction of thermal current
  • 11. Thermoelectric series • For a given temperature range, the thermo e.m.f induced is different for different metal combinations. • Seebeck arranged 35 metals in a series in such away when any two form a thermocouple:- • Current will flow through the cold junction from the one that occurs first in series to the other that occurs later in series • Between 0oC & 1000C the thermoelectric series is: Antimony, Fe, Cd, Zn, Ag, Au, Rb,Mo,Cr,Sn,Pb,Hg,M n,Cu,Pt,Cob,
  • 12. Variation of thermoelectric E.M.F. with temperature • Tn =neutral temperature(constant for a given thermocouple) • Ti =inversion temperature(beyond which e.m.f. starts increasing in opp. direction) • Ti – Tn = Tn – T0 Thermo e.m.f.
  • 13. 1. Law of intermediate metal: if the junction of the thermocouple is opened and a third metal is inserted, the e.m.f. for the couple AB remains the same i.e. without introducing C provided both the junction of the third metal C are at the same temperature. B A c
  • 14. 2.Law of intermediate or successive temperatures : the e.m.f for a thermo- couple between temperatures t1 and t2 is equal to the sum of e.m.fs (seebeck) for any number of successive steps into which the given range of temperatures may be divided. Thus eᶿ1ᶿn =eᶿ1ᶿ2 + eᶿ2ᶿ3 + eᶿ3ᶿ4 +…..eᶿn-1ᶿn
  • 15. Experimental demonstration of seebeck effect In this experiment , two rods of bismuth & antimony are arranged in the form of cross “X” • Firstly, closed key “K1”. • Current starts flowing, making the junction hot.  Temperature difference is obtained.  Open K1 and close K2.  Deflection is shown by galvanometer , thus confirming the seebeck effect
  • 16. Peltier Effect Electric Current Difference in Material A Heat Absorbed or εF between Expelled Materials A and B Material B
  • 17. Peltier effect • In 1834, a French watchmaker and part time physicist, Jean Peltier found that an electrical current would produce a temperature gradient at the junction of two dissimilar metals • • when the current direction was r reversed, the cold junction w would get hot while the hot junction w would get cold.
  • 18. Cause of peltier effect When a current flows across the junction of two metals, it gives rise to an absorption or liberation of heat, depending on the direction of the current. i.e. Applying a current (e- carriers) transports heat from the warmer junction to the cooler junction.
  • 19. As an example of the Peltier effect, consider the circuit shown here. Under these conditions, it is observed, as indicated in the diagram, that the right-hand junction is heated. It shows, in other words, that electrical energy is being transformed into heat energy. Meanwhile, heat energy is transformed into electrical energy at the left junction, thereby causing it to be cooled. When the current is reversed, heat is absorbed at the right junction and produced at the left one.
  • 20. • The rate of evolution of or absorption of heat is proportional to the current &thus the peltier effect is reversible. • If direction of current is changed then the peltier effect is also reversed. • The energy absorbed or evolved at one of the junctions of the two dissimilar metals when one ampere of current flows for one second is called Peltier coefficient ,denoted by ∏
  • 21. In this experiment, two rods of bismuth and antimony are joined as shown.  A differential air thermometer is placed with its two bulbs at junctions A and B.
  • 22. When no current flows through the thermocouple , the junctions A & B are at same temperature.  Also Hg(mercury) pellet in the thermometer lies symmetrically at the centre.  When large current is passed through the thermocouple , then there will be: ◦ Evolution of heat at junction A. ◦ Absorption of heat at junction B. ◦ Hg pellet moves to one direction  If direction of current is changed the pellet moves in the opp. Direction indicating that now A has become cold and B has become hot.
  • 23. Applications Seebeck effect • The Seebeck effect is used in the thermoelectric generator, which functions like a heat engine • These have a use in power plants for converting waste heat into additional power (a form of energy recycling). • in automobiles as automotive thermoelectric generators (ATGs) for increasing fuel efficiency. • Space probes often use radioisotope thermoelectric generators with the same mechanism but using radioisotopes to generate the required heat difference.
  • 24. Peltier effect • The Peltier effect can be used to create a refrigerator which is compact and has no circulating fluid or moving parts • such refrigerators are useful in applications where their advantages out weigh the disadvantage of their very low efficiency.
  • 25. Applications Water/Beer Cooler Cryogenic IR Night Vision Si bench TE Electronic Cooling Cooled Car Seat Laser/OE Cooling 25
  • 26. Temperature measurement • Thermocouples and thermopiles are devices that use the Seebeck effect to measure the temperature difference between two objects, one connected to a voltmeter and the other to the probe. • The temperature of the voltmeter, and hence that of the material being measured by the probe.
  • 27. THANK YOU

Editor's Notes

  1. when two metal wires of different materials were joined to form an electrical circuit and a direct electrical current was made to flow through the circuit, one junction would become cold and the other junction would become hot.indicated in the diagram, that the right-hand junction is heated. It shows, in other words, that electrical energy is being transformed into heat energy. Meanwhile, heat energy is transformed into electrical energy at the left junction, thereby causing it to be cooled.
  2. . If the current happens to flow in the same direction as the current that is produced by the Seebeck Effect at the hot junction (T2), heat will be absorbed, whereas at the cold junction (T1) heat will be liberated.
  3. The effect should not be confused with joules heating effect
  4. 1. , but is less bulky, has no moving parts, and is typically more expensive and less efficient.
  5. can be measured separately using cold junction compensation techniques.