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Steffan's Boltzman Apparatus

The document describes an apparatus used to determine the Stefan Boltzmann constant. The apparatus consists of a copper disc centered in a hemispherical copper enclosure that is heated by circulating water. The temperature change of the disc over time is measured and used to calculate the Stefan Boltzmann constant based on the disc's thermal properties and the enclosure's temperature. The experiment involves heating the enclosure to a steady temperature and recording the disc's temperature increase as it radiatively heats up.

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0% found this document useful (0 votes)
160 views5 pages

Steffan's Boltzman Apparatus

The document describes an apparatus used to determine the Stefan Boltzmann constant. The apparatus consists of a copper disc centered in a hemispherical copper enclosure that is heated by circulating water. The temperature change of the disc over time is measured and used to calculate the Stefan Boltzmann constant based on the disc's thermal properties and the enclosure's temperature. The experiment involves heating the enclosure to a steady temperature and recording the disc's temperature increase as it radiatively heats up.

Uploaded by

Priyank Sharma
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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Download as DOC, PDF, TXT or read online on Scribd
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CHEMICAL ENGINEERING GROUP

STEFAN BOLTZMANN APPARATUS

STEFAN’S BOLTZMANN APPARATUS 1


CHEMICAL ENGINEERING GROUP

STEFAN BOLTZMANN APPARATUS

OBJECTIVE

Study of Radiation heat transfer by black body.

AIM

To determine Stefan Boltzmann constant.

THEORY

All substances at all temperature emit thermal radiation. Thermal radiation is an


electromagnetic wave and does not require any material medium for propagation. Radiation
that is emitted by the surface originates from the thermal energy of matter bounded to the
surface. The rate at which energy is released per unit area is termed as surface emissive
power.

There is an upper limit to the emissive power prescribed by Stefan-Boltzmann law. This law
states that emissive power of a black body is proportional to the fourth power of absolute
temperature of the surface and is given by

E b  σTs4

The constant of proportionally is called the Stefan Boltzmann constant and has the value of
5.67 x 10-8 W/m2 K4. The Stefan Boltzmann law can be derived by integrating the Planck’s
law over the entire spectrum of wavelength from 0 to .

DESCRIPTION OF APPARATUS

The apparatus consists of a copper disc is centered on a flanged copper hemispherical


enclosure fixed on a flat non-conducting base plate. The disc, which is mounted in an
insulating bakelite sleeves is fitted in a hole drilled in the centre of the base plate. The outer
surface of hemisphere is enclosed in a water jacket. Circulating water from a supply tank
passes through the jacket and is used to maintain the hemisphere surface at some desired
temperature. A heater in the supply tank facilitates variation of water temperature.

STEFAN’S BOLTZMANN APPARATUS 2


CHEMICAL ENGINEERING GROUP

The hemisphere temperature is measured using a temperature sensor and the same is
read by a temperature indicator. Another temperature sensor is used to measure the
temperature of disc. The inner surface of hemisphere, base plate forming the enclosure and
the surface of the copper disk are coated using lamp black to approximate a black body.

UTILITIES REQUIRED

Electricity Supply: 1 Phase, 220 V AC, 2 Amps.

EXPERIMENTAL PROCEDURE

1. Note ambient temperature and pressure before commencing measurements.


2. Ensure that there is water in the supply tank before starting main power supply.
Switching the heater on with no water in the tank will lead to overheating and damage
the heater.
3. Ensure that the disk is not in position and detached from base plate at the start of the
experiment.
4. Ensure that the valve on the overflow line is open.
5. Switch on the main power supply to the test set-up and heater.
6. Set the water temperature in the supply tank to some desired temperature.
7. Once the water is the supply tank attains the desired temperature, start flow of water
through the jacket.
8. The hemispherical enclosure and the base plate will attain some uniform temperature
in a short time after the hot water fills the jacket. The jacket is considered completely
filled when water starts to flow from the overflow line provided. The thermal inertia of
hot water is quite adequate to prevent significant cooling in the time required to conduct
the experiment.
9. Close the valve on the overflow line. Allow the enclosure to attain thermal equilibrium.
Note the steady state temperature of the enclosure.
10. Note down the temperature of the disc before inserting in the base plate (at time t = 0)
11. Insert the disk into the base plate and note the temperature change every five seconds
for duration of three minutes.
12. To conclude the experiment, detach the disk first. Switch of the heater in the supply tank.
Allow the water in the hemisphere to cool before draining it off. Consult the lab
instructor before doing this.

STEFAN’S BOLTZMANN APPARATUS 3


CHEMICAL ENGINEERING GROUP

SPECIFICATIONS / KNOWN DATA

Hemispherical enclosure diameter : 200 mm


Base plate diameter : 250 mm
Test disc diameter : 20 mm
Mass of test disc : 5.1 g
Specific heat of the disc : 418 J/kg.K

OBSERVATIONS

1. Temperature of enclosure: _______ºC


2. Temperature of disc (at t = 0): _______ºC

Time / sec Disk temperature / ºC


5
10
15
20
.
.
.
Till 120 or 180 seconds

DATA REDUCTION

Area of the disc (m2)

The cross sectional area AD of the disc is evaluated using

 d2
AD 
4

Stefan Boltzmann constant (W/m2.K4)

The Stefan Boltzmann constant is calculated from

STEFAN’S BOLTZMANN APPARATUS 4


CHEMICAL ENGINEERING GROUP

 dT 
mcP  
 dt  t  0
σ
AD (Th4  TD4 )

where cP denoted the specific heat of the disc material and Td denoted the thermodynamic
temperature of the disk at time t = 0

NOMENCLATURE

AD Area of disc
th Temperature of hemisphere enclosure in Celsius
Th Thermodynamic temperature of hemisphere enclosure
TD Thermodynamic temperature of disc at time t = 0
m Mass of disc
cP specific heat of the disc material
σ Stefan Boltzmann constant

Precautions & Maintenance Instructions:

1. Always use clean water. Ensure that the heater is submerged in water before switching
ON the heater.
2. Always note the temperature of the disc before attaching it to the base plate.
3. Use stabilized A.C. Single Phase supply only.
4. Never switch on mains power supply before ensuring that all the ON/OFF switches
given on the panel are at OFF position.
5. Voltage supply to heater should be constant.
6. Never run the apparatus if power supply is less than 180 V and above than 240 V.
7. Operate selector switch of temperature indicator gently.
8. Always keep the apparatus free from dust.
9. Don’t switch ON the heater before filling the water into the bath.

REFERENCES:

1. Holman, J.P., Heat Transfer, 9th edition, McGraw Hill, NY, 2004
2. Incropera, F. P. and Dewitt, D. P., Heat and Mass transfer, 5th Edition, 2002

STEFAN’S BOLTZMANN APPARATUS 5

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