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The Time Delay for A Perceptible Thermal Disturbance in A Slab
Oleh:
Davies, M. G.
Jenis:
Article from Bulletin/Magazine
Dalam koleksi:
Journal of Heat Transfer vol. 121 no. 4 (Nov. 1999)
,
page 1072-1075.
Topik:
thermal conductivity
;
time delay
;
perceptible thermal
;
disturbance
;
slab
Ketersediaan
Perpustakaan Pusat (Semanggi)
Nomor Panggil:
JJ90.1
Non-tandon:
1 (dapat dipinjam: 0)
Tandon:
tidak ada
Lihat Detail Induk
Isi artikel
If a thermal disturbance such as a step change in temperature is applied at each surface of a homogeneous slab of thickness 2L, the effect of cooling at x = +L at first has no effect at x = -L but is clearly evident after a time described by a Fourier number F0 = at / p(c)((p))L(2) of around 0.2. To establish the time of a perceptible change the minimum value of o(i) - (o (1) + (o(2)) is sought, where o(1) is the flux into a semi - infinite solid and o(1) and o(2) are the first and second eigenfunction contributions to the solution for a slab of finite thickness. Cooling throughout the slab is determined virtually by the first eigenfunction alone after F(0 = 0.22. For a fluid-cooled slab these values are larger.
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