Wm. Atkins et al., TIME-RESOLVED FLUORESCENCE AND COMPUTATIONAL STUDIES OF ADENYLYLATED GLUTAMINE-SYNTHETASE - ANALYSIS OF INTERSUBUNIT INTERACTIONS, Protein science, 2(5), 1993, pp. 800-813
Adenylylation of Tyr-397 of each subunit of Escherichia coli glutamine
synthetase (GS) down-regulates enzymatic activity in vivo. The overal
l structure of the enzyme consists of 12 subunits arranged as two hexa
mers, face to face. Research reported in this paper addresses the ques
tion of whether the covalently attached adenylyl group interacts with
neighboring amino acid residues to produce the regulatory phenomenon.
Wild-type GS has two Trp residues (positions 57 and 158) and the adeny
lylation site lies within 7-8 angstrom of the Trp-57 loop in the adjac
ent subunit of the same hexameric ring; Trp-158 is about 35 k from the
site of adenylylation. Fluorescence lifetimes and quantum yields have
been determined for two fluorophores with wild-type and mutant GS. On
e fluorophore is epsilon-AMP adenylylated GS (at Tyr-397), and the oth
er fluorophore is the intrinsic protein residue Trp-57. These experime
nts were conducted in order to detect possible intersubunit interactio
ns between adenylyl groups and the neighboring Trp-57 to search for a
role for the Trp-57 loop in the regulation of GS. The fluorescence due
to epsilon-AMP of two adenylylated enzymes, wild-type GS and the W158
F mutant, exhibits heterogeneous decay kinetics; the data adequately f
it to a double exponential decay model with recovered average lifetime
values of 18.2 and 2.1 ns, respectively. The pre-exponential factors
range from 0.66 to 0.73 for the long lifetime component, at five emiss
ion wavelengths. The W57L-epsilon-AMP enzyme yields longer average lif
etime values of 19.5 and 2.4 ns, and the pre-exponential factors range
from 0.82 to 0.85 for the long lifetime component. An additional resi
due in the Trp-57 loop, Lys-58, has been altered and the K58C mutant e
nzyme has been adenylylated with epsilon-AMP on Tyr-397. Lys-58 is nea
r the ATP binding site and may represent a link by which the adenylyl
group controls the activity of GS. The fluorescence of epsilon-AMP-ade
nylylated K58C mutant GS is best described by a triple exponential dec
ay with average recovered lifetime values of 19.9, 4.6, and 0.58 ns, w
ith the largest fraction being the median lifetime component. Relative
quantum yields of epsilon-AMP-Tyr-397 were measured in order to deter
mine if static quenching occurs from adenine-indole stacking in the wi
ld-type GS. The relative quantum yield of the epsilon-AMP-adenylylated
W57L mutant is larger than the wild-type protein by the amount predic
ted from the difference in lifetime values: thus, no static quenching
is evident. Intrinsic tryptophan fluorescence was also studied in the
presence and absence of covalently attached adenylyl groups. The fluor
escence decay parameters of Trp-57 are not significantly affected by t
he presence of epsilon-AMP or AMP attached to Tyr-397. Enzymatic activ
ity of the mutant proteins was also studied. The Mg-activated enzymes
are nearly completely inhibited upon adenylylation, and regulation is
not affected by mutation at Trp-57 or Lys-58. These results indicate t
hat the Trp-57 loop dynamically interacts with the adenylyl group, but
a ''ring stacked'' complex is not formed and is not a structural feat
ure of the regulatory mechanism. This conclusion was further corrobora
ted by computational minimization and molecular dynamics studies of GS
with an AMP moiety built onto Tyr-397. Relative energies were sampled
at various points as the Tr-57 ring and urine ring of AMP were target
ed toward one another, the endpoint being a 3-angstrom parallel and st
acked conformation. Dynamics simulations were performed with the paral
lel, stacked conformation, as well as an extended conformation, as the
starting point. All studies indicate that the stacked indole-purine c
onformation is not favorable; however, a potential hydrogen bonding in
teraction between the amine nitrogen of the tryptophan and the ring ox
ygen of ribose is implied by dynamics simulations for certain conforma
tions of the loop.