Semiconductor thermogenerator – Seebeck effect
Principle
In a semi-conductor thermogenerator, the no-load voltage and the short-circuit current are measured as a function of the temperature difference. The internal resistance, the Seebeck coefficient and the efficiency are determined.
Benefits
- Open design allows to fully understand function and applications
- Individual instruments for distinct functions (no “black box”)
- Key products of the experiment setup can also be used for investigating the Peltier effect
Bath for thermostat, makrolon
External circulation set for thermostat Alpha A
Immersion thermostat Alpha A, 230 V
Thermometer -10…+50 °C
Lab thermometer,-10..+110 °C
Rubber tubing, i.d. 6 mm
Tubing connector, ID 6-10mm
Stopwatch, digital, 1/100 s
Heat conductive paste,50 g
Thermogenerator with 2 water baths
Flow-through heat exchanger
Connection box
Resistor 1 Ohm 2%, 2W, G1
Resistor 2 Ohm 5%, 2W, G1
Resistor 5 Ohm 2%, 2W, G1
Resistor 10 Ohm 2%, 2W, G1
Rheostat, 33 Ohm , 3.1A
Voltmeter, 0.3-300 V DC, 10-300 V AC
Ammeter 1/5 A DC
Connecting cord, 32 A, 500 mm, red
Connecting cord, 32 A, 500 mm, blue
Tasks
- To measure no-load voltage U0 and short-circuit current Is at different temperature differences and to determine the Seebeck coefficient.
- To measure current and voltage at a constant temperature difference but with different load resistors, and to determine the internal resistance Ri from the measured values.
- To determine the efficiency of energy conversion, from the quantity of heat consumed and the electrical energy produced per unit time.
What you can learn about
- Seebeck effect (thermoelectric effect)
- Thermoelectric e.m.f.
- Efficiency
- Peltier coefficient
- Thomson coefficient
- Seebeck coefficient
- Direct energy conversion
- Thomson equations