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Table 5 Summary of data showing the effect of the number of gj-channels on the length constant (λ) and on overall propagation velocity (θov) in the single linear chain of 100 myocardial cells

From: Cable properties and propagation velocity in a long single chain of simulated myocardial cells

 

No. of gj-channels

N MathType@MTEF@5@5@+=feaafiart1ev1aaatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXatLxBI9gBaebbnrfifHhDYfgasaacH8akY=wiFfYdH8Gipec8Eeeu0xXdbba9frFj0=OqFfea0dXdd9vqai=hGuQ8kuc9pgc9s8qqaq=dirpe0xb9q8qiLsFr0=vr0=vr0dc8meaabaqaciaacaGaaeqabaqabeGadaaakeaadaGcaaqaaiabd6eaobWcbeaaaaa@2DEC@

λ(μm)

θov(cm/sec)

A

300

17.3

150

358

B

1000

31.6

270

874

C

3000

54.8

440

1850

 

Ratios

C/A

10.0

3.17

2.93

5.17

C/B

3.00

1.73

1.63

2.12

B/A

3.33

1.82

1.80

2.44

  1. N = Number of gj-channels.
  2. The data are given for only those 3 cases in which there was an exponential decay of potential as a function of distance.
  3. Note that the ratios for the effects were always substantially higher for θov than for λ. That is, adding gj-channels had a larger effect on θov than on λ.
  4. Also note that λ varies approximately with the square root of the number of gj-channels.