| ²é¿´: 576 | »Ø¸´: 2 | ||||
| µ±Ç°Ö÷ÌâÒѾ´æµµ¡£ | ||||
mqjiangľ³æ (ÖøÃûдÊÖ)
Amorphous Solids
|
[½»Á÷]
¡¾Ô´´¡¿¹ØÓÚ½ðÊô²£Á§ÖмôÇдøÊ§ÎȵÄÎïÀíÆðÔ´
|
|||
|
¿éÌå½ðÊô²£Á§ÓÉÓÚÆä¶ÀÌØµÄ΢¹Û½á¹¹£¨Ô×ÓÅÅÁг¤³ÌÎÞÐò¡¢¶Ì³ÌÓÐÐò£¬ÎÞ¾§½ç¡¢Î»´íµÈ´«Í³ÒâÒåµÄ½á¹¹È±ÏÝ£©£¬¸³ÓèÕâÀà²ÄÁÏһϵÁÐÓÅÒìµÄÎïÀí¡¢Á¦Ñ§¡¢»¯Ñ§µÈÐÔÄÜ¡£µ«ÊÇ£¬ÔÚÍÆ½ø½ðÊô²£Á§µÄʵ¼ÊÓ¦Óùý³ÌÖУ¬×î´óµÄÒ»¸öÆ¿¾±ÊÇËüÔÚÊÒÎÂϼ«²îµÄÀÉìÑÓÐÔ£¬ÆäÔÒòÊǽðÊô²£Á§ÔÚÊÒÎÂϵÄËÜÐÔ±äÐθ߶Ⱦֲ¿»¯£¬¼«Ò×ÐγÉÄÉÃ׳߶ȵļôÇдø¡£Òò´Ë£¬¶ÔÓÚ½ðÊô²£Á§ÖмôÇдøÏà¹ØµÄÑо¿¾ÍÏÔµÃÓÈÎªÖØÒª¡£ ¹ØÓÚ½ðÊô²£Á§ÖмôÇдøµÄÐγɻúÀí»òÕßÎïÀíÆðÔ´£¬ËäÈ»¾¹ý¼¸Ê®Äê´óÁ¿µÄ̽Ë÷£¬Ä¿Ç°ÆäÇåÎúµÄÎïÀíͼÏñÈÔÈ»²»Çå³þ¡£Ò»°ãÈÏΪ£¬½ðÊô²£Á§ÖÐijЩ²»¾ùÔÈ´¦µÄÕ³¶È½µµÍ²¢½ø¶øµ¼ÖÂËÜÐÔ±äÐÎÄÜÁ¦¼±¾çϽµÊÇÐγɾֲ¿»¯¼ôÇдøµÄÖ÷Òª»úÖÆ¡£µ«ÊÇ£¬¶ÔÓÚÕâÖÖÕ³¶È½µµÍµÄÔÒòÒ»Ö±ÒÔÀ´´æÔÚ×ÅÁ½ÖÖ½ØÈ»²»Í¬µÄ¹Ûµã£º×ÔÓÉÌå»ýÈí»¯ºÍ¾øÈÈÈí»¯¡£ËäÈ»£¬Á½ÖÖ¹Ûµã¸÷×Ô¶¼ÓÐʵÑéÖ¤¾Ý£¬µ«ÊÇÓÐЩÏÖÏóËüÃǵ¥¶ÀÈÔÈ»ÎÞ·¨ºÏÀí½âÊÍ¡£ ÎÒÃÇ¿ÎÌâ×éÔÚÇ°ÃæÍ¨¹ýһϵÁеÄʵÑ顾Liu et al., MCP 2005; JNS 2005; JMR 2006¡¿ºÍÀíÂÛ·ÖÎö¡¾Dai et al., APL 87, 141916 ( 2005); Dai and Bai, IJIE 35, 704 (2008)¡¿£¬³õ²½½Òʾ½ðÊô²£Á§ÖмôÇдøÐγÉÊÇÒ»ÖÖÈÈÁ¦ñîºÏµÄʧÎȹý³Ì£¬²¢²»ÊÇijһÒòËØ£¨×ÔÓÉÌå»ýÈí»¯»òÕßÈÈÈí»¯£©µ¥¶À×÷ÓõĽá¹û¡£ÓÈÆäÊÇÔÚ¸ßÓ¦Á¦ºÍ¸ßÓ¦±äÂÊÌõ¼þÏ£¬Ó¦Á¦Çý¶¯µÄ×ÔÓÉÌå»ý²úÉúºÍ¹¦ÈÈת±äµ¼ÖµÄÎÂÉý¶¼ÓпÉÄÜ·¢Éú£¬²¢ÇÒ»¥ÏàÓ°Ïì¡£ÕâÁ½¸ö¹ý³ÌÌìÈ»ñîºÏÔÚÒ»Æð¡£×î½ü·¢Õ¹µÄһЩÈÈÁ¦ñîºÏÄ£ÐÍÄܹ»ºÜºÃµØÃèÊö½ðÊô²£Á§µÄ£¨·Ç£©¾ùÔÈËÜÐÔ±äÐÎÐÐΪ£¬µ«ÊǶÔÓÚÔÚÕâÖÖñîºÏ¹ý³ÌÖУ¬×ÔÓÉÌå»ýºÍÈȵÄÏ໥×÷ÓÃÒÔ¼°ËÊǼôÇдøµÄÆðÔ´µÈ¹Ø¼üÎÊÌâûÓиø³öÃ÷È·µÄ´ð°¸£¬ÈÔÈ»ÐèÒª½øÒ»²½µÄÑо¿¡£ ÎÒÃÇÕâ¸ö¹¤×÷¾ÍÊÇÕë¶ÔÉÏÊöÕâ¸öÎÊÌâ½øÐÐϵͳ¶øÉîÈëµÄÀíÂÛ·ÖÎö£¬ÖØµã¹Ø×¢ÔÚ¼ôÇдøÐγɹý³ÌÖУ¬ÈȺÍ×ÔÓÉÌå»ýµÄÏ໥×÷ÓÃͼÏñ£»×ÔÓÉÌå»ý¾Û¼¯¡¢ÎÂÉý¡¢ÌåÕͶÔÓÚ¼ôÇдøÊ§ÎȵÄÓ°Ïì¡£Ïà¹Ø¹¤×÷ÒѾ·¢±íÔÚ¹ÌÌåÁ¦Ñ§ÁìÓò×îÓÐÓ°ÏìÁ¦µÄÔÓÖ¾ J. Mech. Phys. Solids (2009),doi:10.1016/j.jmps.2009.04.008 On the origin of shear banding instability in metallic glasses M.Q. Jiang, and L.H. Dai, State Key Laboratory of Nonlinear Mechanics, Institute of Mechanics, Chinese Academy of Sciences, Beijing 100190, PR China Received 20 October 2008; revised 13 April 2009; accepted 21 April 2009. Available online 4 May 2009. Abstract To uncover the physical origin of shear-banding instability in metallic glass (MG), a theoretical description of thermo-mechanical deformation of MG undergoing one-dimensional simple shearing is presented. The coupled thermo-mechanical model takes into account the momentum balance, the energy balance and the dynamics of free volume. The interplay between free-volume production and temperature increase being two potential causes for shear-banding instability is examined on the basis of the homogeneous solution. It is found that the free-volume production facilitates the sudden increase in the temperature before instability and vice versa. A rigorous linear perturbation analysis is used to examine the inhomogeneous deformation, during which the onset criteria and the internal length and time scales for three types of instabilities, namely free-volume softening, thermal softening and coupling softening, are clearly revealed. The shear-banding instability originating from sole free-volume softening takes place easier and faster than that due to sole thermal softening, and dominates in the coupling softening. Furthermore, the coupled thermo-mechanical shear-band analysis does show that an initial slight distribution of local free volume can incur significant strain localization, producing a shear band. During such a localization process, the local free-volume creation occurs indeed prior to the increase in local temperature, indicating that the former is the cause of shear localization, whereas the latter is its consequence. Finally, extension of the above model to include the shear-induced dilatation shows that such dilatation facilitates the shear instability in metallic glasses. Keywords: Metallic glasses; Free volume; Temperature increase; Shear-banding instability; Dilatation È«ÎÄÏÂÔØµØÖ·£ºhttp://www.sciencenet.cn/m/user_content.aspx?id=235805 [ Last edited by hslining on 2009-9-12 at 09:00 ] |
» ÊÕ¼±¾ÌûµÄÌÔÌûר¼ÍƼö
ÎÄÏ×ÊÕ¼¯ |
» ²ÂÄãϲ»¶
Çóµ÷¼Á
ÒѾÓÐ6È˻ظ´
275Çóµ÷¼Á
ÒѾÓÐ4È˻ظ´
318Çóµ÷¼Á
ÒѾÓÐ6È˻ظ´
305·ÖÇóµ÷¼Á£¨Ê³Æ·¹¤³Ì£©
ÒѾÓÐ5È˻ظ´
Çóµ÷¼ÁԺУÐÅÏ¢
ÒѾÓÐ5È˻ظ´
Ò»Ö¾Ô¸070300Õã´ó»¯Ñ§358·Ö£¬Çóµ÷¼Á£¡
ÒѾÓÐ3È˻ظ´
Ò»Ö¾Ô¸¶«»ª´óѧ»¯Ñ§070300£¬Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
Ò»Ö¾Ô¸±±¾©»¯¹¤´óѧ070300 ѧ˶336Çóµ÷¼Á
ÒѾÓÐ6È˻ظ´
¿¼Ñе÷¼Á
ÒѾÓÐ3È˻ظ´
» ±¾Ö÷ÌâÏà¹ØÉ̼ÒÍÆ¼ö: (ÎÒÒ²ÒªÔÚÕâÀïÍÆ¹ã)

ffwu
ͳæ (³õÈëÎÄ̳)
- Ó¦Öú: 0 (Ó×¶ùÔ°)
- ½ð±Ò: 78.8
- Ìû×Ó: 28
- ÔÚÏß: 26.2Сʱ
- ³æºÅ: 690062
- ×¢²á: 2009-01-08
- ÐÔ±ð: GG
- רҵ: ²ÄÁÏ¿ÆÑ§Ó빤³Ì/·Ç¾§
¹§Ï²
¡ï
Сľ³æ(½ð±Ò+0.5):¸ø¸öºì°ü£¬Ð»Ð»»ØÌû½»Á÷
Сľ³æ(½ð±Ò+0.5):¸ø¸öºì°ü£¬Ð»Ð»»ØÌû½»Á÷
| ¹§Ï²£¬ JMPSÊDZÈActa»¹Òª¸ßºÜ¶àµÄÒ»¸öÅ£ÔÓÖ¾ |
2Â¥2009-06-03 22:13:03
mqjiang
ľ³æ (ÖøÃûдÊÖ)
Amorphous Solids
- Ó¦Öú: 12 (СѧÉú)
- ½ð±Ò: 4702.5
- É¢½ð: 662
- ºì»¨: 5
- Ìû×Ó: 1265
- ÔÚÏß: 192.8Сʱ
- ³æºÅ: 681623
- ×¢²á: 2008-12-25
- ÐÔ±ð: GG
- רҵ: ¹ÌÌåÁ¦Ñ§

3Â¥2009-06-04 08:56:40













»Ø¸´´ËÂ¥

