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Page "Pitot tube" ¶ 10
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Note and above
Note that the scripts mentioned above are not considered proper alphabets, as they all lack characters representing vowels.
Note that the above formula is only applicable to classical ideal gases and not Bose – Einstein or Fermi gases.
Note that the RGB color may be premultiplied, hence saving the additional multiplication before RGB in the equation above.
Note: the fasces depicted have no axes, possibly because in the Roman Republic, the blade was always removed from the bundle whenever the fasces were carried inside the city, in order to symbolize the rights of citizens against arbitrary state power ( see above ).
Note: The above definition of group velocity is only useful for wavepackets, which is a pulse that is localized in both real space and frequency space.
Note: Some of the following kings are already listed above as German Kings
Note: Some of the following dukes are already listed above as German Kings
Note that the " Zero Frame " dot is placed above the first character due to the smaller size of 16mm.
Note the curved streamlines above and below the foil, and the overall downward deflection of the air.
Note the narrower streamtubes above and the wider streamtubes below the foil.
Note that from the perspective of the smaller-mass object — from the moon, in the preceding example — a spacecraft might appear to orbit in an irregular path about the or point, but from the perspective above the orbital plane, it becomes clear that both the smaller mass and the spacecraft are orbiting the larger mass ( or more precisely, all of the objects are in orbit around the barycenter of the system ); they simply have overlapping orbital paths.
Note that the example net given above on the neighborhood system of a point x does indeed converge to x according to this definition.
( Note: In the above calculation, the square-root, must be positive.
Note that the n-th generation can be found by just taking the n-th power of W substituting it in place of W in the above formula.
( Note that in SQL the heading is not always a set of column definitions as described above, because it is possible for a column to have no name and also for two or more columns to have the same name.
Note that the probability of risk occurrence is difficult to estimate, since the past data on frequencies are not readily available, as mentioned above.
Note that this is the same as above.
( Note that the choice of signs for above follows the space-like convention (−+++).
Note that we require the domains of G < sub > 2 </ sub >, G < sub > 3 </ sub > to be broad enough to make the above properties meaningful.
Note the similarity of the above formula to the ideal gas law and also that osmotic pressure is not dependent on particle charge.
## If not, send F + 1 backwards in time on channel c. Note that this results in a paradox, as the number received in step 3 above is not the same as that sent in this step.
( Note that r is the orbital radius, the distance from the centre of the Earth, not the height above the Equator.
Note that every signaling system can be characterized along each of the above axes of classification.
Note that the above only becomes an issue if the user wishes to ( or has to ) continue to send e-mail remotely, using the same SMTP server which they were previously accessing locally.

Note and equation
Note that by reversing the equation, we can swap < math > < </ math > and, for example:
Note that in this equation, both force and displacement are vector quantities.
Note that, with the opposite sign convention ( used in Physics ), this is the potential generated by a point particle, for an inverse-square law force, arising in the solution of Poisson equation.
Note that in, the equation holds, and therefore
Note how the equation above reduces to that of the univariate normal distribution if is a matrix ( i. e. a real number ).
( Note that the same equation applies for recoil energy losses in x-rays, but the photon energy is much less, resulting in a lower energy loss, which is why gas-phase resonance could be observed with x-rays.
Note that this equation only holds when the density operator is taken to be in the Schrödinger picture, even though this equation seems at first look to emulate the Heisenberg equation of motion in the Heisenberg picture, with a crucial sign difference:
Note that the above equation is flawed — as the temperature approaches zero, the entropy approaches negative infinity, in contradiction to the third law of thermodynamics.
Note that this equation reduces to that of the volume of a sphere when all three elliptic radii are equal, and to that of an oblate or prolate spheroid when two of them are equal.
Note that the integrand above ( uv ) differs from the previous equation.
Note that the above construction of the Galois group for a fifth degree polynomial only applies to the general polynomial, specific polynomials of the fifth degree may have different Galois groups with quite different properties, e. g. has a splitting field generated by a primitive 5th root of unity, and hence its Galois group is abelian and the equation itself solvable by radicals.
Note that this equation indicates that when expectations of future inflation ( or, more correctly, the future price level ) are totally accurate, the last term drops out, so that actual output equals the so-called " natural " level of real GDP.
Note in the second equation that if instead of planck masses the electron mass were used, the equation would no longer be unitary and instead equal a gravitational coupling constant, analogous to how the equation of the fine-structure constant operates with respect to the elementary charge and the Planck charge.
Note that the above equation describes the Earth's gravitational potential, not the geoid itself, at location the co-ordinate being the geocentric radius, i. e., distance from the Earth's centre.
Note: In the following examples the multiplier is the right-hand-side equation without the first component.
Treating free charges separately from bound charges, Ampère's equation including Maxwell's correction in terms of the H-field is ( the H-field is used because it includes the magnetization currents, so J < sub > M </ sub > does not appear explicitly, see H-field and also Note ):
Note that the right-hand side of the equation is also the price of buying a forward contract on the stock with delivery price K. Thus one way to read the equation is that a portfolio that is long a call and short a put is the same as being long a forward.
Note that in any given coordinate patch, ( 1 ) defines an ordinary differential equation, with the initial condition given by ( 2 ).

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