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Murray would read the safety spinning down into the tackle box, an imaginary area near the line of scrimmage, and direct the run away from that safety and the superior number of defensive players to that side of the field.
A popular method to obtain this second-order motion is to (1) create a region filled with black and white random dots (little squares), (2) consider an imaginary rectangular area within that region, (3) change all its black dots into white ones, and all its white dots into black ones, (4) laterally displace the imaginary area, and (5) repeat steps 3 and 4 several times.
At a doorway, the fatal funnel is the area on either side of the door, as deep as the door is tall and just as wide.[3] So standing to the side of a door does not count (obviously the fatal funnel is an imaginary area — an area which the intruder might not be respecting, so just because you are out of the fatal funnel doesn't mean you can't get shot).
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To test for recognition behavior, we made video recordings of the focal crayfish in the central arena which was divided for scoring using boundary markers, into three equal, imaginary areas: a central zone and two end zones (Fig. 1b).
Since the latter is proportional to the square of the radius, r, the former appeared to Lambert to be the area of an imaginary sphere with radius ir, where i = √(−1).
Since the latter is proportional to the square of the radius, r, the former appeared to Lambert to be the area of an imaginary sphere with radius ir, where i = Square root of√−1.
It may sound more like an imaginary Brooklyn area dreamt up by Kings County realtors than the A's manager, but BoMel has his ballclub firing on all cylinders in what has become one of the toughest neighborhoods in baseball.
But this imaginary field is just that, imaginary.
The diameter of an imaginary circle, the area of which is identical to this maximum horizontal area, was defined as the diameter of the colony.
The diameter (A) of a colony was defined as the diameter of an imaginary circle, the area of which is identical to that of the maximum cross section of the colony.
Total wind energy flowing through an imaginary surface with area A during the time t is: E = \frac{1}{2}mv^2 = \frac{1}{2}(Avt\rho)v^2 = \frac{1}{2}At\rho v^3, where ρ is the density of air; v is the wind speed; Avt is the volume of air passing through A (which is considered perpendicular to the direction of the wind); Avtρ is therefore the mass m passing through "A".
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