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Conference, Proceedings

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aerospace engineering, cryogenic engineering (liquefied natural gas tankers) etc. The third one<br />

is alloy FeNi39 commonly used in thermostatic bimetals production (up to 400 0 C).<br />

Temperature [ o C]<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

α<br />

α + γ (heating)<br />

Tc = ~250 o C<br />

Tc = ~195 o C<br />

Tc = ~30 o C<br />

α + γ (cooling)<br />

Tc = ~560 o C<br />

Tc = ~460 o C<br />

0<br />

-100<br />

0 20 29 35 39 48 60 80 100<br />

Nickel content wt. [%]<br />

γ<br />

magnetic<br />

change<br />

Figure 1:. Fe‐Ni Binary Alloy Phase Diagram with a prediction change of the Curie Point [2] as well as<br />

with marked : compositions of FeNi48, and FeNi60 studied alloys; compositions of FeNi29, FeNi35<br />

and FeNi39 invar alloys which have been investigated and described in [7]<br />

This paper presents the results of the thermal diffusivity investigation of the two two‐<br />

component FeNi48 and FeNi60 alloys at the identical temperature range (300 ÷ 900 K).<br />

The first alloy is used in metal to glass seals, especially with soft glasses and for metal to<br />

ceramic sealing applications (UV bulbs). The second alloy is applied in coated electrode<br />

with a core wire of FeNi60, especially suited for welding of spheroidal cast iron. The<br />

weld deposit is free from porosity and has the highest resistance to cracking.<br />

2. Method of the measurement<br />

The theoretical temperature distribution θ (x,t) = T(x,t) – T0 in the sample, where at time t = 0 the<br />

surface layer (0< x ≤ g) absorbs radiation energy of the surface density Q , is obtained by solving<br />

the Fourier equation, under the boundary conditions as it is shown in Figure 2. In this case the<br />

general solution [5] is written as :<br />

2<br />

l<br />

n<br />

l<br />

t nπx<br />

nπx′<br />

θ x t = x dx<br />

e<br />

x dx′<br />

l ∫ θ ′ ′ + ∑ θ ′<br />

l n l ∫<br />

l<br />

∞ −<br />

1<br />

2 τ<br />

( , ) ( , 0)<br />

cos ( , 0)<br />

cos<br />

0<br />

= 1<br />

0<br />

(1)<br />

2 2<br />

where τ = l / π a ‐ is the characteristic time.<br />

217

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