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The Thermo-Electric Effect
PRESENTED BY-SOURABH GUPTA
UID-K11180
BRANCH-MECHANICAL
SUBMITTED TO- MR.ADITYA MISHRA
What is it?
The thermoelectric effect is the
direct conversion of temperature
differences to electric voltage or
vice-versa.
The direction of heat flow can be
controlled by changing polarity of
the voltage source
History
 In the 1820’s Thomas Seebeck (Germany)
discovered that if two metals at different
temperatures were touching you could
create an electric current
 Jean Peltier discovered that the opposite
was also true. By sending a current through
two metals you could create differences in
temperature
Why does this Effect Occur?
Charge Carrier Diffusion and Phonon Drag
Seebeck Effect Peltier Effect
Thermoelectric Module
The Zeroth Law of Thermodynamics
 Pairs of P and N type conductors are both it
contact with a copper plate.
 There will thermo power until the system is
at equilibrium. (All three materials are at
the same temperature)
Semiconductors
 Semiconductors have an electrical
conductivity between materials like copper
and glass
 They possess and interesting property
where its conductivity increases with
added temperature
 P and N type (thermocouples)
semiconductors are created by doping.
Physics Behind It
 Efficiency= e =
𝑒𝑛𝑒𝑟𝑔𝑦 𝑝𝑟𝑜𝑣𝑖𝑑𝑒𝑑
ℎ𝑒𝑎𝑡 𝑒𝑛𝑒𝑟𝑔𝑦 𝑎𝑏𝑠𝑜𝑟𝑏𝑒𝑑
 Voltage = V = (SB-SA)*(T2-T1)
 Thermo Power (V/K) = S = -
∆𝑉
∆𝑇
Thermal Conductivity of Ceramics
Pcond= kA((Th-Tc)/L)
k=1.5
A= 0.03 m2
Th=100°C
Tc=RT (21°C)
L=0.005m
711 W/m/°C
Applications
 Thermoelectric generator
 Cooling Computers
 Drink Coolers
 Recharging Devices
 Space Probes
 Solar Power
 Clothing
 Useful, Quiet, no Moving Parts
 It is less efficient (10%) and more expensive
Test for Understanding
 The USB Coffee cup warmer is an
example of the Seebeck Effect or the
Peltier Effect?
 Before the P and N type Semiconductors
what material were used instead as
thermal couples for thermoelectric
modules?
 What are the advantages of using
thermoelectric generators over, for
example heat engines?
References
Rockwood, Alan L. (1984). "Relationship of thermoelectricity to
electronic entropy". Phys. Rev. A 30 (5): 2843–4. Bibcode
1984PhRvA..30.2843R. doi:10.1103/PhysRevA.30.2843
G. Jeffrey Snyder and Eric S. Toberer "Complex Thermoelectric
Materials" Nature Materials 7, 105-114 (2008).
CRC Handbook of Thermoelectrics, Introduction, Edited by D.M.
Rowe, CRC Press, 1995.
G. Jeffrey Snyder, Tristan Ursell. "Thermoelectric efficiency and
compatibility" Physical Review Letters, Vol 91 p. 148301 (2003)
THANK YOU

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k11180 Sourabh rac ppt

  • 1. Career Point University The Thermo-Electric Effect PRESENTED BY-SOURABH GUPTA UID-K11180 BRANCH-MECHANICAL SUBMITTED TO- MR.ADITYA MISHRA
  • 2. What is it? The thermoelectric effect is the direct conversion of temperature differences to electric voltage or vice-versa. The direction of heat flow can be controlled by changing polarity of the voltage source
  • 3. History  In the 1820’s Thomas Seebeck (Germany) discovered that if two metals at different temperatures were touching you could create an electric current  Jean Peltier discovered that the opposite was also true. By sending a current through two metals you could create differences in temperature
  • 4. Why does this Effect Occur? Charge Carrier Diffusion and Phonon Drag Seebeck Effect Peltier Effect
  • 6. The Zeroth Law of Thermodynamics  Pairs of P and N type conductors are both it contact with a copper plate.  There will thermo power until the system is at equilibrium. (All three materials are at the same temperature)
  • 7. Semiconductors  Semiconductors have an electrical conductivity between materials like copper and glass  They possess and interesting property where its conductivity increases with added temperature  P and N type (thermocouples) semiconductors are created by doping.
  • 8. Physics Behind It  Efficiency= e = 𝑒𝑛𝑒𝑟𝑔𝑦 𝑝𝑟𝑜𝑣𝑖𝑑𝑒𝑑 ℎ𝑒𝑎𝑡 𝑒𝑛𝑒𝑟𝑔𝑦 𝑎𝑏𝑠𝑜𝑟𝑏𝑒𝑑  Voltage = V = (SB-SA)*(T2-T1)  Thermo Power (V/K) = S = - ∆𝑉 ∆𝑇
  • 9. Thermal Conductivity of Ceramics Pcond= kA((Th-Tc)/L) k=1.5 A= 0.03 m2 Th=100°C Tc=RT (21°C) L=0.005m 711 W/m/°C
  • 10. Applications  Thermoelectric generator  Cooling Computers  Drink Coolers  Recharging Devices  Space Probes  Solar Power  Clothing  Useful, Quiet, no Moving Parts  It is less efficient (10%) and more expensive
  • 11. Test for Understanding  The USB Coffee cup warmer is an example of the Seebeck Effect or the Peltier Effect?  Before the P and N type Semiconductors what material were used instead as thermal couples for thermoelectric modules?  What are the advantages of using thermoelectric generators over, for example heat engines?
  • 12. References Rockwood, Alan L. (1984). "Relationship of thermoelectricity to electronic entropy". Phys. Rev. A 30 (5): 2843–4. Bibcode 1984PhRvA..30.2843R. doi:10.1103/PhysRevA.30.2843 G. Jeffrey Snyder and Eric S. Toberer "Complex Thermoelectric Materials" Nature Materials 7, 105-114 (2008). CRC Handbook of Thermoelectrics, Introduction, Edited by D.M. Rowe, CRC Press, 1995. G. Jeffrey Snyder, Tristan Ursell. "Thermoelectric efficiency and compatibility" Physical Review Letters, Vol 91 p. 148301 (2003)

Notes de l'éditeur

  1. Change in electrons
  2. Charge carrier diffusion if electrons move from hot to cold, then a positive immobile nucleus is left at hot side to conserve charge. So this gives rise to a voltage. Phonon Drag: Similar, P has holes while N has excess by running current the incoming electrons distort nearby electrons thus causing a degradation in mobility and thus a lower temperature.
  3. Thermo Couples used to be only two different metals but now you have p and n type Used to be metal not p and n semiconductors 2000 degress Celsius series
  4. P type has a deficiency of charge carriers and n types have an excess
  5. Thermo power is measured across the material