scholarly journals Regulation of cGMP levels by guanylate cyclase in truncated frog rod outer segments.

1989 ◽  
Vol 94 (4) ◽  
pp. 649-668 ◽  
Author(s):  
S Kawamura ◽  
M Murakami

Cyclic GMP is the second messenger in phototransduction and regulates the photoreceptor current. In the present work, we tried to understand the regulation mechanism of cytoplasmic cGMP levels in frog photoreceptors by measuring the photoreceptor current using a truncated rod outer segment (tROS) preparation. Since exogenously applied substance diffuses into tROS from the truncated end, we could examine the biochemical reactions relating to the cGMP metabolism by manipulating the cytoplasmic chemical condition. In tROS, exogenously applied GTP produced a dark current whose amplitude was half-maximal at approximately 0.4 mM GTP. The conductance for this current was suppressed by light in a fashion similar to when it is activated by cGMP. In addition, no current was produced in the absence of Mg2+, which is known to be necessary for the guanylate cyclase activity. These results indicate that guanylate cyclase was present in tROS and synthesized cGMP from exogenously applied GTP. The enzyme activity was distributed throughout the rod outer segment. The amount of synthesized cGMP increased as the cytoplasmic Ca2+ concentration of tROS decreased, which indicated the activation of guanylate cyclase at low Ca2+ concentrations. Half-maximal effect of Ca2+ was observed at approximately 100 nM. tROS contained the proteins involved in the phototransduction mechanism and therefore, we could examine the regulation of the light response waveform by Ca2+. At low Ca2+ concentrations, the time course of the light response was speeded up probably because cGMP recovery was facilitated by activation of the cyclase. Then, if the cytoplasmic Ca2+ concentration of a photoreceptor decreases during light stimulation, the Ca2+ decrease may explain the acceleration of the light response during light adaptation. In tROS, however, we did observe an acceleration during repetitive light flashes when the cytoplasmic Ca2+ concentration increased during the stimulation. This result suggests the presence of an additional light-dependent mechanism that is responsible for the acceleration of the light response during light adaptation.

Biochemistry ◽  
2000 ◽  
Vol 39 (41) ◽  
pp. 12522-12533 ◽  
Author(s):  
Teresa Duda ◽  
Venkateswar Venkataraman ◽  
Anna Jankowska ◽  
Christian Lange ◽  
Karl-W. Koch ◽  
...  

1990 ◽  
pp. 139-145
Author(s):  
I. M. Pepe ◽  
I. Panfoli ◽  
C. Cugnoli

2006 ◽  
Vol 28 (1) ◽  
pp. 50-58 ◽  
Author(s):  
A. Jankowska ◽  
B. Burczynska ◽  
T. Duda ◽  
J. B. Warchol ◽  
R. K. Sharma

Biochemistry ◽  
1995 ◽  
Vol 34 (44) ◽  
pp. 14279-14283 ◽  
Author(s):  
Nikolay Pozdnyakov ◽  
Akiko Yoshida ◽  
Nigel G. F. Cooper ◽  
Alexander Margulis ◽  
Teresa Duda ◽  
...  

2003 ◽  
Vol 270 (18) ◽  
pp. 3814-3821 ◽  
Author(s):  
Ji-Young Hwang ◽  
Christian Lange ◽  
Andreas Helten ◽  
Doris Hoppner-Heitmann ◽  
Teresa Duda ◽  
...  

Biochemistry ◽  
1999 ◽  
Vol 38 (42) ◽  
pp. 13912-13919 ◽  
Author(s):  
Teresa Duda ◽  
Anuradha Krishnan ◽  
Venkateswar Venkataraman ◽  
Christian Lange ◽  
Karl-Wilhelm Koch ◽  
...  

1974 ◽  
Vol 64 (2) ◽  
pp. 166-185 ◽  
Author(s):  
Richard Srebro ◽  
Michael Behbehani

Light adaptation in both the ventral photoreceptor and the lateral eye photoreceptor is a complex process consisting of at least two phases. One phase, which we call the rapid phase of adaptation, occurs whenever there is temporal overlap of the discrete waves that compose a light response. The recovery from the rapid phase of adaptation follows an exponential time-course with a time constant of approximately 75 ms at 21°C. The rapid phase of adaptation occurs at light intensities barely above discrete wave threshold as well as at substantially higher light intensities with the same recovery time-course at all intensities. It occurs in voltage-clamped and unclamped photoreceptors. The kinetics of the rapid phase of adaptation is closely correlated to the photocurrent which appears to initiate it after a short delay. The rapid phase of adaptation is probably identical to what is called the "adapting bump" process. At light intensities greater than about 10 times discrete wave threshold another phase of light adaptation occurs. It develops slowly over a period of ½ s or so, and decays even more slowly over a period of several seconds. It is graded with light intensity and occurs in both voltage-clamped and unclamped photoreceptors. We call this the slow phase of light adaptation.


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