抄録
To explain cooling of metal poured in a metallic mold, the solution of the equation of heat conduction between molten metal and metallic mold in ideal contact condition is used in general. But in practical casting, the surface of mold is very rough and even coated. Accordingly, molten metal does not contact with mold ideally. It can be considered that actual contact condition has heat resistance between metal and mold when heat flows from metal to mold. In this case, the boundary condition of the equation is as follows, U1(0, t)−U2(0, t)=−RH d⁄(dx) U1(0, t) Using this condition, when metal and mold have infinite length from the surface of contact, we get the following solution. Concerning metal, U1(x, t)=θ1 − k1⁄(μλ1) (θ1−θ2){erfc(−x⁄(2k1√t)) − e−μx⁄(RHk1) + (μ⁄(RH))2t • erfc(μ⁄(RH)√t + −x⁄(2k1√t))} Concerning mold, U2(x, t)=θ2 + k2⁄(μλ2) (θ1−θ2){erfc(x⁄(2k2√t))−eμx⁄(RHk2) + (μ⁄(RH))2t • erfc(μ/RH)√t + x⁄(2k2√t))} t : time after pouring x : distance from the surface of contact, x≦0 for metal, x≧0 for mold U1(x, t) : temperature of metal U2(x, t) : temperature of mold k?? : thermal diffusivility of metal k?? : thermal diffusivility of mold λ1 : thermal conductivity of metal λ2 : thermal conductivity of mold θ1 : pouring tempemperature θ2 : initial tempepature of mold μ=(λ1k2+λ2k1)/λ1λ2 [Written in non-displayable characters.] In this solution, the term involving contact heat resistance RH is the complementary one. When RH decreases, the term tends to zero and the solution agrees with that in ideal contact condition. Therefore, this solution is more general for heat conduction between metal and mold. In this experiment, measurements of contact heat resiststance were carried out in steady state at comparatively low temperature using solid metal instead of molten metal. It became clear that heat resistance changes by thickness of coating, roughness of the surface of mold and the pressure which is applied to metal, and that its value in practical aluminum casting lies approximately between 10 and 100cm2•s• °C/cal.