E (b.) (c.) A fictitious glass is consistent with data provided below. Table 1. Temperature (°C) 700 900 1100 Viscosity (P-poise) 1.09 x 10¹ Plot the data points from Table 1 in the figure above the table to show that it seems to "fit" the trends shown by the other glasses. Add an approximate trend line. 1.23 x 10 1.00 x 10 Viscosity (n) is the inverse of fluidity (p), where the latter obeys an Arrhenius formula: Therefore, viscosity obeys the following: p = A exp 1 exp(-27) RT n=no expl (Quiscous RT Determine the activation energy for viscous flow (Qviscous) for the fictitious glass. The glass-transition temperature is above the strain point, and this temperature is the lower limit of the supercooled liquid regime. The strain point in general is the temperature at which the viscosity equals 3 x 10¹4 P. What is the temperature of the strain point for our fictitious glass?
E (b.) (c.) A fictitious glass is consistent with data provided below. Table 1. Temperature (°C) 700 900 1100 Viscosity (P-poise) 1.09 x 10¹ Plot the data points from Table 1 in the figure above the table to show that it seems to "fit" the trends shown by the other glasses. Add an approximate trend line. 1.23 x 10 1.00 x 10 Viscosity (n) is the inverse of fluidity (p), where the latter obeys an Arrhenius formula: Therefore, viscosity obeys the following: p = A exp 1 exp(-27) RT n=no expl (Quiscous RT Determine the activation energy for viscous flow (Qviscous) for the fictitious glass. The glass-transition temperature is above the strain point, and this temperature is the lower limit of the supercooled liquid regime. The strain point in general is the temperature at which the viscosity equals 3 x 10¹4 P. What is the temperature of the strain point for our fictitious glass?
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
Section: Chapter Questions
Problem 1.1MA
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
Transcribed Image Text:(a.)
(b.)
(c.)
A fictitious glass is consistent with data provided below.
Table 1
Temperature (°C)
700
900
1100
Viscosity (P-poise)
1.09 x 10¹5
Plot the data points from Table 1 in the figure above the table to show that it
seems to "fit" the trends shown by the other glasses. Add an approximate
trend line.
1.23 x 100
1.00 x 10⁰
Viscosity (n) is the inverse of fluidity (p), where the latter obeys an Arrhenius
formula:
Therefore, viscosity obeys the following:
9 = A exp(-2)
n = no exp
(Quiscous)
RT
Determine the activation energy for viscous flow (Qviscous) for the fictitious
glass.
The glass-transition temperature is above the strain point, and this temperature is
the lower limit of the supercooled liquid regime. The strain point in general is the
temperature at which the viscosity equals 3 x 10¹4 P. What is the temperature
of the strain point for our fictitious glass?

Transcribed Image Text:Viscosity (Pa-s)
400
1016
1014
1012
1010
108
105
104
10²
1
200
800
Borosilicate
glass
Temperature (°F)
1200 1600 2000
96% silica
glass
Working range
Melting point
400 600
Fused
silica
2400 2800 3:200
Strain point
Annealing point
Softening point
Working point
Soda-lime glass
1018
1016
1014
1012
1010
108
106
104
10²
800 1000 1200 1400 1600 1800
Temperature (°C)
Viscosity (P)
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