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Stefan Boltzmann

The document outlines a laboratory experiment aimed at determining the Stefan Boltzmann constant for radiation heat transfer using a small black body and a hemispherical surface. The procedure involves heating water, measuring temperature changes, and calculating the constant based on energy exchange equations. It includes specifications for the apparatus, thermocouple readings, and data collection methods.
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0% found this document useful (0 votes)
26 views4 pages

Stefan Boltzmann

The document outlines a laboratory experiment aimed at determining the Stefan Boltzmann constant for radiation heat transfer using a small black body and a hemispherical surface. The procedure involves heating water, measuring temperature changes, and calculating the constant based on energy exchange equations. It includes specifications for the apparatus, thermocouple readings, and data collection methods.
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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IMPACT COLLEGE OF ENGINEERING AND APPLIED SCIENCES

SAHAKARA NAGAR SOUTH, BENGALURU - 560092


DEPARTMENT OF MECHANICAL ENGINEERING

HEAT TRANSFER LAB


DETERMINATION OF STEFAN BOLTZMANN CONSTANT
OBJECTIVE: To determine the value of Stefan Boltzmann constant for radiation
heat transfer.

PRINCIPLE: The energy exchange between a small black body located at the center
q 1-2
of a hemispherical surface is given by q1-2 = A ( T14 – T24 ) or  =
A( T14 - T24 )
Where A is the surface area of the small body.

The method consists of maintaining the hemispherical surface to a desired


constant high temperature by supplying preheated water at a temperature close to
boiling point on the outside of the hemispherical dome. A small copper disc coated
with lamp black is introduced at the center of the hemisphere and the rate of
temperature rise of the disc is determined graphically. Then by equating the rate of
radiation energy exchange between the hemispherical surface and the disc to the rate
of energy absorption by the disc, the Stefan Boltzmann constant is evaluated.

APPARATUS: The fig shows the cross-sectional view of the apparatus.

Saleha Nadeem B.E., M. Tech (Thermal) Asst. prof., Dept. of ME, ICEAS.
IMPACT COLLEGE OF ENGINEERING AND APPLIED SCIENCES
SAHAKARA NAGAR SOUTH, BENGALURU - 560092
DEPARTMENT OF MECHANICAL ENGINEERING

REF NO DESCRIPTION
1 WATER INLET
2 WATER OUTLET
3 WATER CIRCULATION
4 SPECIMEN-
5 ________ROD
6 _______ ___mm Dia.
7 WATER JACKET
8 COPPER BOWL ___mm Dia.

PROCEDURE:

a) Fill the water in the upper tank.


b) Switch on the immersion heater and heat the water upto 90o C.
c) Remove the disc before pouring the water into the tank.
d) Switch off the heater and open the valve to allow the water into the lower tank.
e) Allow it to reach steady state.
f) Note down the thermocouple temperatures T1, T2, T3, & T4.
g) Insert the disc and immediately note the temperature T4 at every five seconds
interval from zero seconds.
dT
h) Draw the graph of temperature vs time and find
dt
m.C p . ( dT / dt )
i) Calculate `  ’ using the equation :  = 4 4
A ( Ths - Ts )
Where Cp = Specific heat of surface in kJ / kg oK

DATA SHEET
SPECIFICATIONS:

Specimen material : _______


Size of the disc :  __ mm, ___ mm thickness
Base plate :  ____ mm,___ mm thickness (_____)
Heater : 1.5 kW Capacity, immersion type
Copper Bowl :  _____ mm
Digital temperature indicator : 0 – 199.9 oC

Saleha Nadeem B.E., M. Tech (Thermal) Asst. prof., Dept. of ME, ICEAS.
IMPACT COLLEGE OF ENGINEERING AND APPLIED SCIENCES
SAHAKARA NAGAR SOUTH, BENGALURU - 560092
DEPARTMENT OF MECHANICAL ENGINEERING

Thermocouples used : 5 numbers, on hemisphere


Stop watch : Digital type
Overhead tank : SS, approximately 1-liter capacity
Water Jacket :  230 mm, SS
Mass of Specimen, m : 5 gm.
T1, T2, T3, are Surface Temperatures, T4, Specimen temperature before
insertion
T5, Heater Temperature.

TABULATION OF READINGS

TRIAL THERMOCOUPLE READINGS ( OC )


NO.
T1 T2 T3 T4 T5

Variation Of Temperature V/S Time Of The Specimen

TRIAL 1 TRIAL 2
TEM
TEMP TEMP TEMP TIM TIM
TIME TIME P
( OC) ( OC) ( OC) E E
( C)
O

0 0

SPECIMEN CALCULATION:

d 2
Area of the disc, A1 = = m2.
4
Mass of the disc, m = 5  10-3 kg.

Saleha Nadeem B.E., M. Tech (Thermal) Asst. prof., Dept. of ME, ICEAS.
IMPACT COLLEGE OF ENGINEERING AND APPLIED SCIENCES
SAHAKARA NAGAR SOUTH, BENGALURU - 560092
DEPARTMENT OF MECHANICAL ENGINEERING

Specific heat of the disc material (____), CPs = 385 J/Kg K.

T1 + T2 + T3
Temperature of the hemispherical surface = Ths = = oC or K.
3

Average temperature of the disc before insertion, T4 = ts = C.


o

Ts = ts + 273 = K.
dT
Rate of temperature rise of the disc, = ( From graph )
dt
dT
Rate of energy absorption by the disc, mCP x = W.
dt
Rate of radiation energy exchange between the disc and the enclosure,
= A1F12(Ths4 – Ts4) W.
Where  is the Stefan Boltzmann constant, F12 = 1 for a small body in a large
enclosure.
Equating Rate of radiation energy exchange to rate of energy absorption by the
disc, we
dT
Get, A1F12 ( Ths4 – Ts4 ) = mCPs
dt
dT
mC P
 Stefan Boltzmann constant  = dt
4
A1 ( Ths - Ts4 )
=………………….W/m2K4
GRAPH :
Temp v/s Time

RESULT:

The value of the Stefan Boltzmann’s constant is _____________ W/m K4


and the theoretical value is ________________ W/m-K4

Saleha Nadeem B.E., M. Tech (Thermal) Asst. prof., Dept. of ME, ICEAS.

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