Potassium channels exclude the smaller
alkali metal cations Li1 (radius 0.60 Å) and
Na1 (0.95 Å) but allow permeation of the
larger members of the series Rb1 (1.48 Å)
and Cs1 (1.69 Å). In fact, Rb1 is nearly a
perfect K1 (1.33 Å) analog because its size
and permeability characteristics are very
similar to those of K1. Because they are
more electron dense than K1, Rb1 and Cs1
allow visualization of the locations of permeant
ions in the pore. By difference electron
density maps calculated with data from
crystals transferred into Rb1-containing
(Fig. 6a) or Cs1-containing (Fig. 6b) solutions,
multiple ions are well defined in the
pore. The selectivity filter contains two
ions (inner and outer ions) located at opposite
ends, about 7.5 Å apart (center to
center). In the Rb1 difference map, there
actually are two partially separated peaks at
the inner aspect of the selectivity filter.
These peaks are too close to each other (2.6
Å) to represent two simultaneously occupied
ion binding sites. We suspect that they
represent a single ion (on average) in rapid
equilibrium between adjacent sites. The
single inner ion peak in the Cs1 difference
map undoubtedly reflects the lower resolution
at which the map was calculated (to 5
Å for Cs1 versus 4.0 Å for Rb1), because
the Rb1 difference map, when calculated at
the same lower resolution, also shows only a
single peak at the Cs1 position. The Rb1
positions correspond to strong peaks (pre-
Potassium channels exclude the smalleralkali metal cations Li1 (radius 0.60 Å) andNa1 (0.95 Å) but allow permeation of thelarger members of the series Rb1 (1.48 Å)and Cs1 (1.69 Å). In fact, Rb1 is nearly aperfect K1 (1.33 Å) analog because its sizeand permeability characteristics are verysimilar to those of K1. Because they aremore electron dense than K1, Rb1 and Cs1allow visualization of the locations of permeantions in the pore. By difference electrondensity maps calculated with data fromcrystals transferred into Rb1-containing(Fig. 6a) or Cs1-containing (Fig. 6b) solutions,multiple ions are well defined in thepore. The selectivity filter contains twoions (inner and outer ions) located at oppositeends, about 7.5 Å apart (center tocenter). In the Rb1 difference map, thereactually are two partially separated peaks atthe inner aspect of the selectivity filter.These peaks are too close to each other (2.6Å) to represent two simultaneously occupiedion binding sites. We suspect that theyrepresent a single ion (on average) in rapidequilibrium between adjacent sites. Thesingle inner ion peak in the Cs1 differencemap undoubtedly reflects the lower resolutionat which the map was calculated (to 5Å for Cs1 versus 4.0 Å for Rb1), becausethe Rb1 difference map, when calculated atthe same lower resolution, also shows only asingle peak at the Cs1 position. The Rb1positions correspond to strong peaks (pre-
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ช่องโพแทสเซียมไอออนของโลหะแอลคาไล ยกเว้นเล็ก
li1 ( รัศมี 0.60 Å )
na1 ( 0.95 Å ) แต่อนุญาตให้มีการแทรกซึมของ
สมาชิกของชุด Rb1 ( 1.48 และกริพเพน )
CS1 ( 1.69 Å ) ในความเป็นจริง , Rb1 เป็นเกือบสมบูรณ์แบบ K1
( 1.33 Å ) อนาล็อกเนื่องจากขนาดและลักษณะการซึมมาก
คล้ายกับบรรดาของ K1 . เพราะพวกเขาเป็นอิเล็กตรอนมากขึ้นหนาแน่นกว่า K1
CS1 Rb1 , และallow visualization of the locations of permeant
ions in the pore. By difference electron
density maps calculated with data from
crystals transferred into Rb1-containing
(Fig. 6a) or Cs1-containing (Fig. 6b) solutions,
multiple ions are well defined in the
pore. The selectivity filter contains two
ions (inner and outer ions) located at opposite
ends, about 7.5 Å apart (center to
center).ในแผนที่มีจริง ๆความแตกต่าง Rb1 ,
2 บางส่วนแยกยอดที่
ด้านภายในของตัวกรองหัวกะทิ .
ยอดเหล่านี้อยู่ใกล้กับแต่ละอื่น ๆด้วย ( 2.6
Å ) เพื่อแสดงสองพร้อมกันครอบครอง
ไอออนผูกพันเว็บไซต์ เราสงสัยว่าพวกเขา
เป็นตัวแทนของไอออนเดี่ยว ( เฉลี่ย ) สมดุลอย่างรวดเร็ว
ระหว่างติดเว็บไซต์
เดียวภายในไอออนสูงสุดในความแตกต่าง
CS1map undoubtedly reflects the lower resolution
at which the map was calculated (to 5
Å for Cs1 versus 4.0 Å for Rb1), because
the Rb1 difference map, when calculated at
the same lower resolution, also shows only a
single peak at the Cs1 position. The Rb1
positions correspond to strong peaks (pre-
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