ASME SA213 · TP316LN.UNS S31653 Foto a egosipụtara

ASME SA213 · TP316LN.UNS S31653 ígwè Austenitic

Nkọwa Dị Mkpirikpi:

TP316LN (UNS S31653) bụ ígwè anaghị agba nchara 316 nke nwere nitrogen, nke nwere obere carbon. Nchikota nke mgbakwunye nitrogen na obere carbon na-eme ka arụmọrụ dị elu, ike ịgbado ọkụ, na iguzogide nchara dị n'etiti granular dịkwuo mma. TP316LN na-enye ike dị egwu na gburugburu ụlọ ọrụ mmepụta ihe nwere chloride, mmiri, kemịkalụ, na nrụgide dị elu.

Ọkwa Tube:TP316LN, AISI 316LN, EN 1.4429, UNS S31653

Ụdị Tube:Enweghị Nsogbu

Ụdị Tube:Mpekere kwụ ọtọ, U gbagọrọ agbagọ, nke a kpụrụ akpụ ruo n'ogologo

Mmecha Elu:Ngwọta e ji ihe na-esi ísì ụtọ mee (AP), Bright Annealed (BA), a kpụchara akpụcha

Ụkpụrụ (ASME/ASTM):ASME SA213, ASTM A213

Ụkpụrụ (EN):EN 10216-5

Zitere anyị ozi-e

Nkọwa Ngwaahịa

Akara Ngwaahịa

TP316LNIgwe anaghị agba nchara tubes, 1.4429 Tubes ígwè anaghị agba nchara

ihe	Nkọwapụta/Nkọwapụta
Igwe anaghị agba nchara tube	ASME SA213, ASTM A213
Nha tube	1/8 ″ OD ruo 5 ″ OD (6.35 mm ruo 127 mm)
Oke ọkpụrụkpụ	0.5 mm – 15 mm
Ụdị	Enweghị Nsogbu
Ụdị	Gbaa gburugburu, U Gbagọrọ
Ogologo	Otu Emeghị Eme, Ugboro Abụọ Emeghị Eme & Ogologo achọrọ / U Gbagọọ
Ọgwụgwụ	Ọgwụgwụ Dị Mfe, Ọgwụgwụ A Gbagọrọ Agọ
Nchedo Ọgwụgwụ	Okpu plastik
Mmecha Mpụga	2B, BA, AP, Emechara ya nke ọma
Ọnọdụ Nnyefe	Ngwọta e tinyere n'ime ya ma gwerie ya, e tinyere n'ime ya nke ọma, e tinyere n'ime ya nke ọma
Nnyocha, Akụkọ Ule	Asambodo Nnwale Ụlọ Ọrụ, EN 10204 3.1, Nnwale Eddy Ugbu a, Nnwale Hydrostatic
Nkwakọ ngwaahịa	E tinyere ya n'ime igbe osisi, ma ọ bụ dịka arịrịọ ndị ahịa si dị
Ihe pụrụ iche	Enwere ike imepụta nha na nkọwapụta ndị ọzọ karịa nke dị n'elu ma ọ bụrụ na achọrọ ya.

TP 316LN. UNS S31653. 1.4429 Ngwakọta Kemịkalụ

Ihe mejupụtara kemịkalụ (na pasentị site na oke)

Ọkwa	C (Kachasị)	Si (Max.)	Mn (Max.)	P (Kachasị)	S (Kachasị)	Cr	Ni	Mo	Ti	N	Ndị ọzọ
316LN	0.035	1.00	2.00	0.045	0.030	16.0 – 18.0	10.0 – 14.0	2.00 – 3.00		0.10 – 0.16
1.4429	0.030	1.00	2.00	0.045	0.015	16.5 – 18.5	11.0 – 14.0	2.50 – 3.00		0.12 – 0.22