
PMC:7594251 / 61658-62283
Annnotations
LitCovid-PD-CLO
Id | Subject | Object | Predicate | Lexical cue |
---|---|---|---|---|
T450 | 4-10 | http://purl.obolibrary.org/obo/SO_0000418 | denotes | signal |
T451 | 122-124 | http://purl.obolibrary.org/obo/CLO_0003414 | denotes | g2 |
T452 | 204-210 | http://purl.obolibrary.org/obo/SO_0000418 | denotes | signal |
T453 | 483-489 | http://purl.obolibrary.org/obo/SO_0000418 | denotes | signal |
LitCovid-PD-CHEBI
Id | Subject | Object | Predicate | Lexical cue | chebi_id |
---|---|---|---|---|---|
T33217 | 38-47 | Chemical | denotes | molecules | http://purl.obolibrary.org/obo/CHEBI_25367 |
T4015 | 331-338 | Chemical | denotes | nucleus | http://purl.obolibrary.org/obo/CHEBI_33252 |
LitCovid-sentences
Id | Subject | Object | Predicate | Lexical cue |
---|---|---|---|---|
T427 | 0-436 | Sentence | denotes | The signal intensity of the diffusing molecules depends on three factors, as described by Equation (3) [294]:(5) I=I0e−Dγ2g2δ2 where I is the observed intensity, I0 the reference intensity (unattenuated signal intensity), D is, of course, the diffusion coefficient referred to earlier, γ is the gyromagnetic ratio of the observed nucleus, g is the strength of the gradient, δ the length of the gradient, and ∆ the diffusion time [294]. |
T428 | 437-625 | Sentence | denotes | From Equation (3), it is easy to see that the signal intensity decreases exponentially with time, so it is vital to optimize the values of g, δ, and ∆ for diffusion NMR measurements [294]. |