PASCO TD-8555 User manual

STEFAN-BOLTZMAN LAMP
012-02889D
1/93
$1.00
Introduction
The Stefan-Boltzmann Lamp is a high temperature source of
thermal radiation. It can be used with a radiation detector,
such as PASCO's Model TD-8553 Radiation Sensor, to
investigate the Stefan-Boltzmann Law:
Rrad = σT4;
where Rrad is the power per unit area radiated by an object,
and T is its temperature. This law can also be investigated
using a low temperature source such as PASCO's Model
TD-8554 Thermal Radiation Cube. However, the high
temperature of the Stefan-Boltzmann Lamp simplifies the
analysis because the fourth power of the ambient tempera-
ture is negligibly small compared to the fourth power of the
high temperature of the lamp filament.
When properly oriented, the filament of the Stefan-
Boltzmann Lamp provides a good approximation to a point
source of thermal radiation. It therefore works well for
investigations into the inverse square law.
Measuring the Filament Temperature
By adjusting the power into the lamp (13 Volts Maximum,
between 2 and 3 A or approximately 36 Watts), filament
temperatures up to approximately 3,000 °C can be obtained.
The filament temperature is determined by carefully measur-
ing the voltage and current into the lamp. The voltage
divided by the current gives the resistance of the filament.
For small temperature changes, the temperature of the
tungsten filament can be calculated using α, the temperature
coefficient of resistivity for the filament:
Instruction Sheet
for the PASCO
Model TD-8555
T = + Tref
R- Rref
where,
T = Temperature
R = Resistance at temperature T
Tref= Reference temperature (usually room temp.)
Rref= Resistance at temperature Tref
α= Temperature coefficient of resistivity for the
filament
αRref
Recommended Equipment
AC/DC LV Power Supply SF-9584 or equivalent capable of
13 V @ 3 A max.
Banana Connectors:
Connect to Power
Supply – 13 V MAX,
(2 A min, 3 A max)
For large temperature differences, however, αis not constant
and the above equation is not accurate.
For large temperature differences, therefore, determine
the temperature of the tungsten filament as follows:
1. Accurately measure the resistance (Rref) of the tungsten
filament at room temperature (about 300 °K). Accuracy
is important here. A small error in Rref will result in a
large error in your result for the filament temperature.
2. When the filament is hot, measure the voltage and
current into the filament and divide the voltage by the
current to measure the resistance (RT).
3. Divide RTby Rref to obtain the relative resistance
(RT/Rref).
4. Using your measured value for the relative resistivity of
the filament at temperature T, use Table 2 on the
following page, or the associated graph, to determine the
temperature of the filament.
Model TD-8555
STEFAN-BOLTZMANN
LAMP
CAUTION
13 VDC MAX LAMP VOLTAGE
FOR MAXIMUM ACCURACY,
MEASURE VOLTAGE AT BINDING
POSTS.
USE NO. 1196 BULB

012-02889D
2
Limited Warranty
PASCO scientific warrants this product to be free from defects in
materials and workmanship for a period of one year from the date
of shipment to the customer. PASCO will repair or replace, at its
option, any part of the product which is deemed to be defective in
material or workmanship. This warranty does not cover damage to
the product caused by abuse or improper use. Determination of
whether a product failure is the result of a manufacturing defect or
improper use by the customer shall be made solely by PASCO
scientific. Responsibility for the return of equipment for warranty
repair belongs to the customer. Equipment must be properly
packed to prevent damage and shipped postage or freight prepaid.
(Damage caused by improper packing of the equipment for return
shipment will not be covered by the warranty.) Shipping costs for
returning the equipment, after repair, will be paid by PASCO
scientific.
Important: The voltage into the lamp should
NEVER exceed 13 V. Higher voltages will burn
out the filament.
Replacement Bulb: Use GE Lamp No. 1196,
available at most auto parts stores. When replacing
the bulb, solder the leads to minimize resistance.
Note: Complete instructions for the Stefan-
Boltzmann and inverse square law experiments can
be found in the Instruction Manual and Experiment
Guide for the PASCO scientific Thermal Radiation
System (PASCO Part NO. 012-02845).
Resistivity
µΩ cm
Resistivity
µΩ cm
Resistivity
µΩ cm
0 500 1000 1500 2000 2500 3000 3500
Temperature and Resistivity for Tungsten
Temperature versus Resistivity for Tungsten
0
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
R
T
R
300K
20
Temperature (Kelvin)
Relative
Resistivity
1.0
1.43
1.87
2.34
2.85
3.36
3.88
4.41
4.95
300
400
500
600
700
800
900
1000
1100
5.65
8.06
10.56
13.23
16.09
19.00
21.94
24.93
27.94
5.48
6.03
6.58
7.14
7.71
8.28
8.86
9.44
10.03
1200
1300
1400
1500
1600
1700
1800
1900
2000
30.98
34.08
37.19
40.36
43.55
46.78
50.05
53.35
56.67
10.63
11.24
11.84
12.46
13.08
13.72
14.34
14.99
15.63
2100
2200
2300
2400
2500
2600
2700
2800
2900
60.06
63.48
66.91
70.39
73.91
77.49
81.04
84.70
88.33
16.29
16.95
17.62
18.28
18.97
19.66
26.35
3000
3100
3200
3300
3400
3500
3600
103.3
107.2
111.1
115.0
92.04
95.76
99.54
Temp
°K
R/R
300K
Resistivity
µΩ cm Temp
°K
R/R
300K
Temp
°K
R/R
300K
Temp
°K
R/R
300K