For a bonding MO with σ-symmetry, the orbital can be labeled σ < sub > g </ sub >, and for an antibonding MO with σ-symmetry the orbital can be labeled σ < sub > u </ sub >, because inversion through the center of symmetry for Figure 4 ( b ) would produce a sign change.

* February 15 – Laurence Owen, American Figure Skater ( b. 1944 )

Figure 1 ( b ) illustrates this transition with the corresponding spectroscopic notation.

Figure 1 ( b ): The Bode plot for a first-order ( one-pole ) lowpass filter ; the straight-line approximations are labeled " Bode pole "; phase is 90 ° lower than for Figure 1 ( a ) because the phase contribution of the numerator is 0 ° at all frequencies.

In Figure 1 ( b ), the Bode plots are shown for the one-pole lowpass filter function:

Also shown in Figure 1 ( a ) and 1 ( b ) are the straight-line approximations to the Bode plots that are used in hand analysis, and described later.

The Bode plot is shown in Figure 1 ( b ) above, and construction of the straight-line approximation is discussed next.

In Figure 1, a, b, and c are the lengths of the three sides of the triangle, and α, β, and γ are the angles opposite those three respective sides.

Figure ( b ) above is an example of a perfect matching.

Figure 1: An edge-dislocation ( b = Burgers vector )

* 1967 "( Do I Figure ) In Your Life " ( Dello ) b / w " Throw My Love Away " ( Cane )-Deram

Chlorophyll b replaces a methyl group at the C-3 position on the ring ( Green Box in Figure ) with an aldehyde group.

Figures 1. b ) and 1. c ) show examples of aperture masks used in front of the secondary at the Keck telescope by Peter Tuthill and collaborators ; Figure 1. b ) is a non-redundant mask while Figure 1. c ) is partially redundant.

Figure 1 Schematic graphs of three different kinds of Field-Effect Transistor ( FET ): ( a ) the metal-insulator-semiconductor FET ( MISFET ); ( b ) the metal-semiconductor FET ( MESFET ); ( c ) the thin-film transistor ( TFT ).

Figure 5: Photon detections as a function of time for a ) antibunching ( e. g. light emitted from a single atom ), b ) random ( e. g. a coherent state, laser beam ), and c ) bunching ( chaotic light ).

Figure 1: The Wigner quasiprobability distribution for a ) the vacuum b ) An n = 1 Fock state ( e. g. a single photon ) c ) An n = 5 Fock state.

File: Small_angle_compair_odd. svg |< b > Figure 1 .</ b > A comparison of the basic odd trigonometric functions to θ.

File: Small_angle_compare_even. svg |< b > Figure 2 .</ b > A comparison of cos ( θ ) to 1-θ < sup > 2 </ sup >/ 2.

Figure 3 shows the data on a silicone fluid, labeled 12,500 cps which gave a high positive normal pressure.

The Skeletal Age curve in the lower portion of Figure 2 shows that slowing may have occurred for her during the prepubescent period.

The photograph, Figure 1 of the completed frieze, shows how, having been separated from his fellows in useless isolation for eighty years, he has now been given a hand, and by juxtaposition ( and the permission of the Committee ), given a new job, to represent the witnesses of the first flight at Kitty Hawk in 1903.

Figure 2, above, shows the aging properties of urethane foams as determined by the percent of change in tensile strength during exposure to ultra-violet light.

Figure 7-3 shows a platform system with the gyro vectors arranged as described above.

Figure ( c ) shows a parallel system in which each processor has a direct access to a shared memory.

Figure 1 shows the cumulative budget ( cost ) for this project as a function of time ( the blue line, labeled PV ).

Figure 2 shows the EV curve ( in green ) along with the PV curve from Figure 1.

Figure 3 shows the same EV curve ( green ) with the actual cost data from Figure 1 ( in red ).

Figure 4 shows all three curves together – which is a typical EVM line chart.

Figure 1 also shows the λ-line.

Figure 2 shows the differential force of gravity on a spherical body ( body 1 ) exerted by another body ( body 2 ).

Figure A shows a normal vein with a working valve and normal blood flow.

Figure B shows a varicose vein with a deformed valve, abnormal blood flow, and thin, stretched walls.

Figure 2 shows a Faraday rotator with an input polarizer, and an output analyser.

Figure 3 shows the propagation of light through a polarization independent isolator.

Figure 1 shows the trends which density and temperature follow through the chromosphere.

Figure 2 shows an active electronic implementation of a first-order high-pass filter using an operational amplifier.

Figure 2 shows the typical form of the sharp fluorescent spectral lines obtained in the energy-dispersive method ( see Moseley's law ).

One such famous variation, entitled Figure with Meat ( 1954 ), shows the pope between two halves of a bisected cow.

Figure 3 shows the first fold, and figure 4 the result of the first nine folds, which form a spiral.

Figure 3 shows the sequence of events illustrating the obduction model following continental collision.

For example, arrow 17 in Figure 3 portrays the proximal radial epiphysis for boy 34, whereas the same epiphysis for girl 2 is portrayed by arrow 18 in Figure 4.

Fractals are typically self-similar patterns, where self-similar means they are " the same from near as from far " Fractals may be exactly the same at every scale, or as illustrated in Figure 1, they may be nearly the same at different scales.

::* Quasi self-similarity: approximates the same pattern at different scales ; may contain small copies of the entire fractal in distorted and degenerate forms ; e. g., the Mandelbrot set's satellites are approximations of the entire set, but not exact copies, as shown in Figure 1

A line slightly longer than the note head is drawn parallel to the staff, above or below, spaced at the same distance as the lines within the staff ( see Figure 1 ).

The second Figure 3 does the same for the phase.

Figure 1: The amplitude of a single frequency wave as a function of time t ( red ) and a copy of the same wave delayed by τ ( green ).

Figure 2: The amplitude of a wave whose phase drifts significantly in time τ < sub > c </ sub > as a function of time t ( red ) and a copy of the same wave delayed by 2τ < sub > c </ sub >( green ).

Figure 3: The amplitude of a wavepacket whose amplitude changes significantly in time τ < sub > c </ sub > ( red ) and a copy of the same wave delayed by 2τ < sub > c </ sub >( green ) plotted as a function of time t. At any particular time the red and green waves are uncorrelated ; one oscillates while the other is constant and so there will be no interference at this delay.

Thus, the triggering scheme is the same as an SCR and the equivalent circuit is outlined in Figure 4.

So, in the end, the structure which is crossed by the major portion of the current is the same as Quadrant I operation (" 3 " in Figure 5 ).

Now to increase the labour keeping the production the same the organization has to decrease capital. In Figure 1 B is the point where capital decreases to K2, while labour increases to L2.

Suppose a particle moves at a uniform rate along a line from A to B ( Figure 2 ) in a given time ( say, one second ), while in the same time, the line AB moves uniformly from its position at AB to a position at DC, remaining parallel to its original orientation throughout.

As the level of consumption remains the same, the income – consumption curve for perfect complements is the diagonal line passing through the origin as shown in Figure 5 on the left.

A MOSFET version of Figure 3 is shown in Figure 4 where MOSFETs M < sub > 3 </ sub > and M < sub > 4 </ sub > operate in Ohmic mode to play the same role as emitter resistors R < sub > E </ sub > in Figure 3, and MOSFETs M < sub > 1 </ sub > and M < sub > 2 </ sub > operate in active mode in the same roles as mirror transistors Q < sub > 1 </ sub > and Q < sub > 2 </ sub > in Figure 3.