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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.
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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.
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.
The copper-gold phase diagram is constructed below.
(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=
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 =
μ (^) oμB
3
= 1.14 Bohr magnetons/atom