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Solutions to ECE331 Homework #8: Phase Diagrams and Magnetic Susceptibility, Assignments of Electrical and Electronics Engineering

Solutions to homework #8 of ece331, which covers topics such as phase diagrams and magnetic susceptibility. It includes calculations for pressure at melting and sublimation points, mass fractions of phases in alloys, and magnetic susceptibility of a metal alloy.

What you will learn

  • What is the composition of the liquid phase formed when heating a lead-tin alloy of composition 30 wt% Sn-70 wt% Pb?
  • What is the mass fraction of eutectic ββββ in an 80 wt% Sn-20 wt% Pb alloy?
  • What is the pressure at which melting occurs for a specimen of ice I at -10°C?

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2021/2022

Uploaded on 02/03/2022

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ECE331 Homework #8 Solution
(Due Friday, March 10, 2006)
1. Callister, 9.13
This problem asks us to consider a specimen of ice I which is at -10°C and 1 atm pressure.
(a) In order to determine the pressure at which melting occurs at this temperature, we move
vertically at this temperature until we cross the Ice I-Liquid phase boundar y of Figure 9.33.
This occurs at approximately 570 atm; thus the pressure of the specim en must be raised from
1 to 570 atm.
(b) In order to determine the pressure at which sublimation occurs at this temperature, we
move vertically downward from 1 atm until we cross the Ice I-Vapor phase boundary of Figure
9.33. This intersection occurs at approximately 0.0023 atm.
2. Callister, 9.20
Upon heating a lead-tin alloy of composition 30 wt% Sn-70 wt% Pb from 150°C and utilizing
Figure 9.7:
(a) the first liquid forms at the temperature at which a vertical line at this composition
intersects the eutectic isotherm--i.e., at 183°C;
(b) the composition of this liquid phase corresponds to the intersection with the (α
αα
α + L)-L
phase boundary, of a tie line constructed across the α
αα
α + L phase region just above this
eutectic isotherm--i.e., CL = 61.9 wt% Sn;
(c) complete melting of the alloy occurs at the intersection of this same vertical line at 30 wt%
Sn with the (α
αα
α + L)-L phase boundary--i.e., at about 260°C;
(d) the composition of the last solid remaining prior to complete melting corresponds to the
intersection with α
αα
α-(α
αα
α + L) phase boundary, of the tie line constructed across the α
αα
α + L phase
region at 260°C--i.e., Cα
αα
α is about 13 wt% Sn.
3. Callister, 9.23
The copper-gold phase diagram is constructed below.
pf3
pf4

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ECE331 Homework #8 Solution

(Due Friday, March 10, 2006)

1. Callister, 9.

This problem asks us to consider a specimen of ice I which is at -10°C and 1 atm pressure. (a) In order to determine the pressure at which melting occurs at this temperature, we move vertically at this temperature until we cross the Ice I-Liquid phase boundary of Figure 9.33. This occurs at approximately 570 atm; thus the pressure of the specimen must be raised from 1 to 570 atm. (b) In order to determine the pressure at which sublimation occurs at this temperature, we move vertically downward from 1 atm until we cross the Ice I-Vapor phase boundary of Figure 9.33. This intersection occurs at approximately 0.0023 atm.

2. Callister, 9.

Upon heating a lead-tin alloy of composition 30 wt% Sn-70 wt% Pb from 150°C and utilizing Figure 9.7: (a) the first liquid forms at the temperature at which a vertical line at this composition intersects the eutectic isotherm--i.e., at 183°C; (b) the composition of this liquid phase corresponds to the intersection with the (αααα + L )- L phase boundary, of a tie line constructed across the αααα + L phase region just above this eutectic isotherm--i.e., CL = 61.9 wt% Sn; (c) complete melting of the alloy occurs at the intersection of this same vertical line at 30 wt% Sn with the (αααα + L )- L phase boundary--i.e., at about 260°C; (d) the composition of the last solid remaining prior to complete melting corresponds to the intersection with αααα-(αααα + L ) phase boundary, of the tie line constructed across the αααα + L phase region at 260°C--i.e., C αααα is about 13 wt% Sn.

3. Callister, 9.

The copper-gold phase diagram is constructed below.

4. Callister, 9.

(a) This portion of the problem asks that we determine the mass fractions of αααα and (^) ββββ phases for an 80 wt% Sn-20 wt% Pb alloy (at 180°C). In order to do this it is necessary to employ the lever rule using a tie line that extends entirely across the αααα + ββββ phase field (Figure 9.7), as follows:

Wα =

Cβ − Co Cβ − Cα^ =^

Wβ = Co − Cα Cβ − Cα^ =^

(b) Now it is necessary to determine the mass fractions of primary ββββ and eutectic microconstituents for this same alloy. This requires us to utilize the lever rule and a tie line that extends from the maximum solubility of Pb in the ββββ phase at 180°C (i.e., 97.8 wt% Sn) to the eutectic composition (61.9 wt% Sn). Thus

Wβ' = C (^) o − Ceutectic Cβ − Ceutectic =

We =

Cβ − Co Cβ − Ceutectic=

7. Callister, 20.

We are to determine the number of Bohr magnetons per atom of a hypothetical metal that has a simple cubic crystal structure, an atomic radius of 0.125 nm, and a saturation flux density of 0.85 tesla. It becomes necessary to employ Equations (20.8) and (20.11) as follows:

Ms = B (^) s μo =

nBμB VC

For the simple cubic crystal structure VC = (2 r )^3 , where r is the atomic radius. Substituting this relationship into the above equation and solving for nB yields

n (^) B =

B s (8r 3 )

μ (^) oμB

(0.85 tesla)(8) 0.125 x 10( −^9 m)

3

(1.257 x 10 −^6 H/ m)(9.27 x 10 −^24 A - m^2 / BM)

= 1.14 Bohr magnetons/atom