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Fuzzy sets and shapes and ranges of membership function for ALTITUDE input variable.

Fuzzy sets and shapes and ranges of membership function for MODE output variable.

Fuzzy Sets Q for some failures.

Fuzzy sets, shapes and ranges of membership function for SPEED input variable.

Fuzzy Truth Restrictions t, upon the Perfect Design for the Alternative Design Elutions.

Fuzzy upper bound of the FRF between the upper and lower ring of the structure.

Fuzzy Variables for a Choice between Alternative Structures.

Fuzzy Variables for Environmental Impact Example.

Fuzzy variables for failure assessment. Thus if xij w y. T j

Fuzzy weighted, region adaptive Gaussian mask

FV - 19 shows how a pore size distribution may be obtained from a melting curve and extent of undercooling, the cumulative pore volume can be obtained as a function of the pore radius.

FV - 32. Potential as a function of the distance for various ionic strengths.

Fv Fm ratios in control 0 and iron deficient plants during the recovery by darkness after 10 minutes under 1500 pmol m- s . Squared symbols correspond to 12 h dark adapted samples

FV height left and force images right of electrospun fiber of PVA on SAM of octadecanethiol. The data was acquired with unmodified AFM tips in air. The gray scale denotes

FV images of oxyfluorinated iPP

Fv of tomato leaf discs at decreasing temperature.

FVactions of developed silver-bromide grains after deposition of size-selected silver clusters

FVE distribution curve in terms of probe or FVE volume . Fitting results

FVeak wave recorded on the 24th November, 1981 at the Gorm Field in the Danish

FVeak wave simulated by the high-order spectrum method.

FVee energy profiles in acetonitrile as functions of the reaction coordinate. Solid lines

FVequency-shift factor as caused by the entanglement effect versus the weight fraction of component two, W2. The arrow indicates the predicted Wc value from Eq. .

FVetting cycles for the shot peened dry material.

FVH diagram, showing the concept of adiabatic following. The Bloch vector, , precesses in a narrow cone about the rotating frame torque vector, S . As the detuning. A, changes from negative to positive, the field vector, fi, becomes inverted. If the change in is adiabatic the Bloch vector follows the

FVH diagram, showing the eoneept of adiabatie following. The Bloeh veetor, f, preeesses m a narrow eone about the rotating frame torque veetor, i2. As the detuning. A, ehanges from negative to positive, the field veetor, J , beeomes inverted. If the ehange m j is adiabatie the Bloeh veetor follows the



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