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Real Ghost seen on CCTV in PUB!

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Real Ghost seen on CCTV in PUB!

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security job.

i don’t know where they are from.

There are two ghosts on this tape. The first one seems to appear on the right side of the frame. Then a girl’s face comes up on the left hand side of the screen. Freaky!

Richard “Richie” Mirando, known as Seen UA, born 1961 in The Bronx, New York, is one of the most well known graffiti artists in the world, often referred to as the Godfather of Graffiti, although he did not pioneer the movement.

Seen first started to paint on New York’s subway in 1973. His crew United Artists (or simply UA) quickly gained the reputation for producing full-color throw-ups on whole cars with members such as Pjay, Duster, Sin, and his brother Mad.

Life

For the next 16 years his pieces were running across the city and on all lines, but they were especially prominent on the 2, 5, and 6 lines. He was responsible for dozens of whole-car top-to-bottoms, many of which have become iconic images of the time.

It was during the very early 1980s that Seen started producing work on canvas, shown by galleries and bought by museums and private collectors across the globe. These included not only solo exhibitions but also group shows with artists such as Keith Haring, Andy Warhol, Jean-Michel Basquiat, Dondi, Quik, Blade, and Lee Quinones. Despite the high demand for his work in Europe and constant world travel, Seen continued to hit the New York subway trains until 1989, long after many had admitted defeat at the hands of the MTA. He was also featured prominently in the 1983 PBS documentary Style Wars.

In the late 1980s Seen also turned his talent to tattoo art, opening Tattoo Seen, which quickly became one of the most successful studios in New York. Seen’s recent work includes three-dimensional sculpture, mixed media work with reclaimed or discarded materials (often found in the street), and a series of hand-painted, limited-edition MTA New York subway maps. He continues to exhibit worldwide and produce work with and alongside artists such as Banksy.

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ghosts drag dogs up stairs.

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ghosts drag dogs up stairs.

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In fluid dynamics, drag (sometimes called air resistance or fluid resistance) refers to forces that oppose the relative motion of an object through a fluid (a liquid or gas). Drag forces act in a direction opposite to the oncoming flow velocity.Unlike other resistive forces such as dry friction, which is nearly independent of velocity, drag forces depend on velocity.

For a solid object moving through a fluid, the drag is the component of the net aerodynamic or hydrodynamic force acting opposite to the direction of the movement. The component perpendicular to this direction is considered lift. Therefore drag opposes the motion of the object, and in a powered vehicle it is overcome by thrust.

In astrodynamics, depending on the situation, atmospheric drag can be regarded as an inefficiency requiring expense of additional energy during launch of the space object or as a bonus simplifying return from orbit.

Types of drag

Types of drag are generally divided into the following categories:

parasitic drag, consisting of

form drag,

skin friction,

interference drag,

lift-induced drag, and

wave drag (aerodynamics) or wave resistance (ship hydrodynamics).

The phrase parasitic drag is mainly used in aerodynamics, since for lifting wings drag is in general small compared to lift. For flow around bluff bodies, drag is most often dominating, and then the qualifier “parasitic” is meaningless. Form drag, skin friction and interference drag on bluff bodies are not coined as being elements of parasitic drag, but directly as elements of drag.
Further, lift-induced drag is only relevant when wings or a lifting body are present, and is therefore usually discussed either in the aviation perspective of drag, or in the design of either semi-planing or planing hulls. Wave drag occurs when a solid object is moving through a fluid at or near the speed of sound in that fluid — or in case there is a freely-moving fluid surface with surface waves radiating from the object, e.g. from a ship.

For high velocities — or more precisely, at high Reynolds numbers — the overall drag of an object is characterized by a dimensionless number called the drag coefficient, and is calculated using the drag equation. Assuming a more-or-less constant drag coefficient, drag will vary as the square of velocity. Thus, the resultant power needed to overcome this drag will vary as the cube of velocity. The standard equation for drag is one half the coefficient of drag multiplied by the fluid mass density, the cross sectional area of the specified item, and the square of the velocity.

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