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mengfan
Ìú¸Ëľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 7931.9
- ºì»¨: 3
- Ìû×Ó: 639
- ÔÚÏß: 92.8Сʱ
- ³æºÅ: 390430
- ×¢²á: 2007-06-02
- ÐÔ±ð: GG
- רҵ: ½ðÊô½á¹¹²ÄÁÏ
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ratio(½ð±Ò+2):ллӦÖú£¬»¶Ó³£À´£¡£¡ 2010-04-27 18:09
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Finite Length Warburg - Open Circuit Terminus Z = R*ctnh([I*T*w]^P) / (I*T*w)^P Parameters: Wo-R, Wo-T, Wo-P This element is also known as a Generalized Finite Warburg element (GFW). It is an extension of another more common element, the Finite-Length Warburg (FLW). To use the FLW equation, set Wo-P = 0.5 and set its freedom to 'fixed'. The FLW is the solution of the one-dimensional diffusion equation of a particle, which is completely analogous to wave transmission in a finite-length RC transmission line. In the diffusion interpretation Wo-T = L2 / D. (L is the effective diffusion thickness, and D is the effective diffusion coefficient of the particle). The GFW is similar to this, but for it the square root becomes a continuously varying exponent Ws-P such that 0 < Ws-P < 1. This version of the Warburg element is terminates in a open circuit. At very low frequencies, the Z' approaches Wo-R and Z'¡® continues to increase - similar to the behavior of a capacitor. If the data exhibits only the high frequency (45 degree slope) behavior and not the transition to low frequency behavior, either Wo-R or Wo-T must be set as Fixed(X). Alternately, a CPE can be used in this situation. |
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4Â¥2010-04-27 10:12:08
2Â¥2009-07-05 20:06:05
mengfan
Ìú¸Ëľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
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- Ìû×Ó: 639
- ÔÚÏß: 92.8Сʱ
- ³æºÅ: 390430
- ×¢²á: 2007-06-02
- ÐÔ±ð: GG
- רҵ: ½ðÊô½á¹¹²ÄÁÏ

3Â¥2010-04-27 10:11:47
mengfan
Ìú¸Ëľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 2 (Ó×¶ùÔ°)
- ½ð±Ò: 7931.9
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- Ìû×Ó: 639
- ÔÚÏß: 92.8Сʱ
- ³æºÅ: 390430
- ×¢²á: 2007-06-02
- ÐÔ±ð: GG
- רҵ: ½ðÊô½á¹¹²ÄÁÏ
|
Finite Length Warburg - Short Circuit Terminus Z = R*tanh([I*T*w]^P) / (I*T*w)^P Parameters: Ws-R, Ws-T, Ws-P This element is also known as a Generalized Finite Warburg element (GFW). It is an extension of another more common element, the Finite-Length Warburg (FLW). To use the FLW equation, set Ws-P = 0.5 and set its freedom to 'fixed'. The FLW is the solution of the one-dimensional diffusion equation of a particle, which is completely analogous to wave transmission in a finite-length RC transmission line. In the diffusion interpretation Ws-T = L^2 / D. (L is the effective diffusion thickness, and D is the effective diffusion coefficient of the particle). The GFW is similar to this, but for it the square root becomes a continuously varying exponent Ws-P such that 0 < Ws-P < 1. If the data exhibits only the high frequency (45 degree slope) behavior and not the transition to low frequency behavior, either Wo-R or Wo-T must be set as Fixed(X). Alternately, a CPE can be used in this situation. This version of the Warburg element is terminates in a finite resistance. At very low frequencies, Z¡¯ approaches Ws-R and Z¡¯¡® goes to zero |

5Â¥2010-04-27 10:12:28
strawboss
ľ³æ (ÕýʽдÊÖ)
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6Â¥2014-09-01 18:50:46
ĦÌìÂÖ5920
гæ (³õÈëÎÄ̳)
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7Â¥2017-02-13 21:20:23
ÊÅË®aa
ľ³æ (ÖøÃûдÊÖ)
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8Â¥2017-03-27 16:45:41
ÊÅË®aa
ľ³æ (ÖøÃûдÊÖ)
- Ó¦Öú: 1 (Ó×¶ùÔ°)
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9Â¥2017-03-27 16:46:31
jhl2011
гæ (СÓÐÃûÆø)
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10Â¥2017-06-19 10:37:19














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