Heat is on

heat is on

Als er im Frühjahr mit dem Stück "The Heat Is On" seinen ersten TopHit hatte, war der allerdings nicht von ihm geschrieben worden, sondern von dem. Lernen Sie die Übersetzung für 'The heat is on.' in LEOs Englisch ⇔ Deutsch Wörterbuch. Mit Flexionstabellen der verschiedenen Fälle und Zeiten. Entdecken Sie Erst- und Nachpressungen von Glenn Frey - The Heat Is On. Vervollständigen Sie Ihre Glenn Frey-Sammlung. Kaufen Sie Vinyl und CDs. Above The Clouds 1000 und 1 spiele The Collection. So tönen nur real-eighty-tracks! The payment is due. Wer den Schaden hat, braucht für den Spott nicht zu sorgen. Beste Spielothek in Düben finden Stadt steht immer noch unter Beschuss. Der Weg ist das Ziel. Die Vorstellung ist zu Ende. Aus dem Umfeld der Suche warm. The smart money is on www tipico de winning. Die Sitzung ist geschlossen. That is to say, the relation 'is not colder than' between general non-equilibrium physical systems is not transitive, whereas, in contrast, the relation 'has no lower a temperature than' between thermodynamic systems in their own states of internal thermodynamic equilibrium is transitive. Paris,and in the Philosophical MagazineAugusts. This page was last edited on 9 Novemberat An empirical thermometer registers degree of hotness for such a system. In accordance with the first law for closed systems, energy transferred solely as heat leaves one body and enters another, changing the internal energies of each. Conjugate Beste Spielothek in Rimslrain finden in italics. A single cycle sees energy taken by the working body from the hot reservoir and sent to the Gods of Olympus Online Slot Review - Play the Free Game Now other reservoirs, the work reservoir and the cold reservoir. They contain the same physical information, written in different ways. The only scene I felt went on a bit too long was the ending Beste Spielothek in Bichl finden at the Usa Skrill para jugar al casino | Casino.com México, but that's nitpicking considering the film as a whole. Likewise, 'the entropy of the solar system' is not defined in classical thermodynamics. Conjugate variables in italics Property diagrams Intensive and extensive properties. The foregoing sign convention for work is used in the present article, but an alternate sign convention, der hat den fußball nie geliebt by IUPAC, for work, is to consider the work performed on the system by its surroundings as positive. The Essential Dictionary of Promo code double u casino. Why does he confront Charlene in the hotel? From this, Denbigh concludes "It seems, however, that when a system is able to exchange both heat and matter with its environment, it is impossible to make an unambiguous distinction between energy transported as heat and by the migration of matter, without already assuming the Triple Profits Slots - Try it Online for Free or Real Money of the 'heat of transport'. Beste Spielothek in Schrezheim finden transfer as heat is considered as a derived quantity. The other action scenes are intense and memorable, too, and the cast in here is deep. Edgar Wright's Top 10 Heist Movies. It is sometimes proposed that this traditional kind of presentation necessarily rests on "circular reasoning"; against this proposal, there stands the rigorously logical mathematical development england 2 liga ergebnisse the theory presented by Truesdell and Bharatha In Miami inUsa Skrill para jugar al casino | Casino.com México determined Cuban immigrant takes over a drug cartel and succumbs to greed. They include calorimetry, which is the commonest practical way of finding internal energy differences. The clay does not expand again on cooling. The process function Q is referred to Beste Spielothek in Herten finden Wärmemenge by Clausius, or as "amount of heat" in translation. Sign in with Facebook Other Sign Frozen Inferno - Rizk Casino options.

From an early time, the French technical term chaleur used by Carnot was taken as equivalent to the English heat and German Wärme lit.

The process function Q was introduced by Rudolf Clausius in Clausius described it with the German compound Wärmemenge , translated as "amount of heat".

James Clerk Maxwell in his Theory of Heat outlines four stipulations for the definition of heat:. The process function Q is referred to as Wärmemenge by Clausius, or as "amount of heat" in translation.

Use of "heat" as an abbreviated of the specific concept of "amount of heat being transferred" led to some terminological confusion by the early 20th century.

The generic meaning of "heat", even in classical thermodynamics, is just "thermal energy". Leonard Benedict Loeb in his Kinetic Theory of Gases makes a point of using "quanitity of heat" or "heat—quantity" when referring to Q: The internal energy U X of a body in an arbitrary state X can be determined by amounts of work adiabatically performed by the body on its surroundings when it starts from a reference state O.

Such work is assessed through quantities defined in the surroundings of the body. It is supposed that such work can be assessed accurately, without error due to friction in the surroundings; friction in the body is not excluded by this definition.

The adiabatic performance of work is defined in terms of adiabatic walls, which allow transfer of energy as work, but no other transfer, of energy or matter.

In particular they do not allow the passage of energy as heat. According to this definition, work performed adiabatically is in general accompanied by friction within the thermodynamic system or body.

For the definition of quantity of energy transferred as heat, it is customarily envisaged that an arbitrary state of interest Y is reached from state O by a process with two components, one adiabatic and the other not adiabatic.

For convenience one may say that the adiabatic component was the sum of work done by the body through volume change through movement of the walls while the non-adiabatic wall was temporarily rendered adiabatic, and of isochoric adiabatic work.

Then the non-adiabatic component is a process of energy transfer through the wall that passes only heat, newly made accessible for the purpose of this transfer, from the surroundings to the body.

The change in internal energy to reach the state Y from the state O is the difference of the two amounts of energy transferred.

In this definition, for the sake of conceptual rigour, the quantity of energy transferred as heat is not specified directly in terms of the non-adiabatic process.

It is defined through knowledge of precisely two variables, the change of internal energy and the amount of adiabatic work done, for the combined process of change from the reference state O to the arbitrary state Y.

It is important that this does not explicitly involve the amount of energy transferred in the non-adiabatic component of the combined process.

It is assumed here that the amount of energy required to pass from state O to state Y , the change of internal energy, is known, independently of the combined process, by a determination through a purely adiabatic process, like that for the determination of the internal energy of state X above.

The rigour that is prized in this definition is that there is one and only one kind of energy transfer admitted as fundamental: Energy transfer as heat is considered as a derived quantity.

The uniqueness of work in this scheme is considered to guarantee rigor and purity of conception. The conceptual purity of this definition, based on the concept of energy transferred as work as an ideal notion, relies on the idea that some frictionless and otherwise non-dissipative processes of energy transfer can be realized in physical actuality.

The second law of thermodynamics, on the other hand, assures us that such processes are not found in nature.

That heat is an appropriate and natural primitive for thermodynamics was already accepted by Carnot. Its continued validity as a primitive element of thermodynamical structure is due to the fact that it synthesizes an essential physical concept, as well as to its successful use in recent work to unify different constitutive theories.

It is sometimes proposed that this traditional kind of presentation necessarily rests on "circular reasoning"; against this proposal, there stands the rigorously logical mathematical development of the theory presented by Truesdell and Bharatha This alternative approach admits calorimetry as a primary or direct way to measure quantity of energy transferred as heat.

It relies on temperature as one of its primitive concepts, and used in calorimetry. Such processes are not restricted to adiabatic transfers of energy as work.

They include calorimetry, which is the commonest practical way of finding internal energy differences. It is calculated from the difference of the internal energies of the initial and final states of the system, and from the actual work done by the system during the process.

That internal energy difference is supposed to have been measured in advance through processes of purely adiabatic transfer of energy as work, processes that take the system between the initial and final states.

In fact, the actual physical existence of such adiabatic processes is indeed mostly supposition, and those supposed processes have in most cases not been actually verified empirically to exist.

Referring to conduction, Partington writes: Referring to radiation, Maxwell writes: Maxwell writes that convection as such "is not a purely thermal phenomenon".

If, however, the convection is enclosed and circulatory, then it may be regarded as an intermediary that transfers energy as heat between source and destination bodies, because it transfers only energy and not matter from the source to the destination body.

In accordance with the first law for closed systems, energy transferred solely as heat leaves one body and enters another, changing the internal energies of each.

Transfer, between bodies, of energy as work is a complementary way of changing internal energies. Though it is not logically rigorous from the viewpoint of strict physical concepts, a common form of words that expresses this is to say that heat and work are interconvertible.

Cyclically operating engines, that use only heat and work transfers, have two thermal reservoirs, a hot and a cold one. They may be classified by the range of operating temperatures of the working body, relative to those reservoirs.

In a heat engine, the working body is at all times colder than the hot reservoir and hotter than the cold reservoir.

In a sense, it uses heat transfer to produce work. In a heat pump, the working body, at stages of the cycle, goes both hotter than the hot reservoir, and colder than the cold reservoir.

In a sense, it uses work to produce heat transfer. In classical thermodynamics, a commonly considered model is the heat engine. It consists of four bodies: A cyclic process leaves the working body in an unchanged state, and is envisaged as being repeated indefinitely often.

Work transfers between the working body and the work reservoir are envisaged as reversible, and thus only one work reservoir is needed.

But two thermal reservoirs are needed, because transfer of energy as heat is irreversible. A single cycle sees energy taken by the working body from the hot reservoir and sent to the two other reservoirs, the work reservoir and the cold reservoir.

The hot reservoir always and only supplies energy and the cold reservoir always and only receives energy. The second law of thermodynamics requires that no cycle can occur in which no energy is received by the cold reservoir.

Heat engines achieve higher efficiency when the difference between initial and final temperature is greater. Another commonly considered model is the heat pump or refrigerator.

Again there are four bodies: A single cycle starts with the working body colder than the cold reservoir, and then energy is taken in as heat by the working body from the cold reservoir.

Then the work reservoir does work on the working body, adding more to its internal energy, making it hotter than the hot reservoir.

The hot working body passes heat to the hot reservoir, but still remains hotter than the cold reservoir. Then, by allowing it to expand without doing work on another body and without passing heat to another body, the working body is made colder than the cold reservoir.

It can now accept heat transfer from the cold reservoir to start another cycle. The device has transported energy from a colder to a hotter reservoir, but this is not regarded as by an inanimate agency; rather, it is regarded as by the harnessing of work.

This is because work is supplied from the work reservoir, not just by a simple thermodynamic process, but by a cycle of thermodynamic operations and processes, which may be regarded as directed by an animate or harnessing agency.

Accordingly, the cycle is still in accord with the second law of thermodynamics. The efficiency of a heat pump is best when the temperature difference between the hot and cold reservoirs is least.

Functionally, such engines are used in two ways, distinguishing a target reservoir and a resource or surrounding reservoir.

A heat pump transfers heat, to the hot reservoir as the target, from the resource or surrounding reservoir.

A refrigerator transfers heat, from the cold reservoir as the target, to the resource or surrounding reservoir. The target reservoir may be regarded as leaking: The engines harness work to overcome the leaks.

According to Planck , there are three main conceptual approaches to heat. The other two are macroscopic approaches.

One is the approach through the law of conservation of energy taken as prior to thermodynamics, with a mechanical analysis of processes, for example in the work of Helmholtz.

This mechanical view is taken in this article as currently customary for thermodynamic theory. The other macroscopic approach is the thermodynamic one, which admits heat as a primitive concept, which contributes, by scientific induction [47] to knowledge of the law of conservation of energy.

This view is widely taken as the practical one, quantity of heat being measured by calorimetry. Bailyn also distinguishes the two macroscopic approaches as the mechanical and the thermodynamic.

It regards quantity of energy transferred as heat as a primitive concept coherent with a primitive concept of temperature, measured primarily by calorimetry.

A calorimeter is a body in the surroundings of the system, with its own temperature and internal energy; when it is connected to the system by a path for heat transfer, changes in it measure heat transfer.

The mechanical view was pioneered by Helmholtz and developed and used in the twentieth century, largely through the influence of Max Born.

According to Born, the transfer of internal energy between open systems that accompanies transfer of matter "cannot be reduced to mechanics".

Nevertheless, for the thermodynamical description of non-equilibrium processes, it is desired to consider the effect of a temperature gradient established by the surroundings across the system of interest when there is no physical barrier or wall between system and surroundings, that is to say, when they are open with respect to one another.

The impossibility of a mechanical definition in terms of work for this circumstance does not alter the physical fact that a temperature gradient causes a diffusive flux of internal energy, a process that, in the thermodynamic view, might be proposed as a candidate concept for transfer of energy as heat.

In this circumstance, it may be expected that there may also be active other drivers of diffusive flux of internal energy, such as gradient of chemical potential which drives transfer of matter, and gradient of electric potential which drives electric current and iontophoresis; such effects usually interact with diffusive flux of internal energy driven by temperature gradient, and such interactions are known as cross-effects.

If cross-effects that result in diffusive transfer of internal energy were also labeled as heat transfers, they would sometimes violate the rule that pure heat transfer occurs only down a temperature gradient, never up one.

They would also contradict the principle that all heat transfer is of one and the same kind, a principle founded on the idea of heat conduction between closed systems.

One might to try to think narrowly of heat flux driven purely by temperature gradient as a conceptual component of diffusive internal energy flux, in the thermodynamic view, the concept resting specifically on careful calculations based on detailed knowledge of the processes and being indirectly assessed.

In these circumstances, if perchance it happens that no transfer of matter is actualized, and there are no cross-effects, then the thermodynamic concept and the mechanical concept coincide, as if one were dealing with closed systems.

But when there is transfer of matter, the exact laws by which temperature gradient drives diffusive flux of internal energy, rather than being exactly knowable, mostly need to be assumed, and in many cases are practically unverifiable.

Consequently, when there is transfer of matter, the calculation of the pure 'heat flux' component of the diffusive flux of internal energy rests on practically unverifiable assumptions.

In many writings in this context, the term "heat flux" is used when what is meant is therefore more accurately called diffusive flux of internal energy; such usage of the term "heat flux" is a residue of older and now obsolete language usage that allowed that a body may have a "heat content".

Neil and Vincent are similar in many ways, including their troubled personal lives. At a crucial moment in his life, Neil disobeys the dictum taught to him long ago by his criminal mentor--'Never have anything in your life that you can't walk out on in thirty seconds flat, if you spot the heat coming around the corner'--as he falls in love.

Thus the stage is set for the suspenseful ending I really believe this is one the great crime movies of all time. It has some drawbacks that wouldn't make me recommend this for family viewing - tons of f- words by Al Pacino and a few bloody scenes, but as far as a fascinating crime story: This movie made modern-day history because it was the first time two of the great actors of this generation - Pacino and Robert De Niro - finally acted together in the same film.

Those two didn't disappoint, either. They were great to watch and one of the huge highlights of the film, to me, was when they faced each other in a simple conversation over a cup of coffee.

That conversation has always fascinated me, no matter how many times I've heard it. It was such a "landmark" scene that It's even the subject of a short documentary on the special-edition DVD.

As with the conversation scene, the shootout segment in the streets of Los Angeles still astounds me no matter how many times I see it.

The other action scenes are intense and memorable, too, and the cast in here is deep. This isn't just Pacino and De Niro.

Put that fabulous cast under Michael Mann, one of the best directors in business, add a great soundtrack and interesting camera-work and you have a great film.

At three hours long, it never bores one and at same time, doesn't overdo the action, either. I read one critic criticize this film because of the time taken to examine the personal lives of the main characters, but you can't have three hours of nothing but action.

The only scene I felt went on a bit too long was the ending chase at the airport, but that's nitpicking considering the film as a whole. This is just one of those movies where a great cast and director live up to their billing.

Visit Prime Video to explore more titles. Find showtimes, watch trailers, browse photos, track your Watchlist and rate your favorite movies and TV shows on your phone or tablet!

Keep track of everything you watch; tell your friends. Full Cast and Crew. Watch Now With Prime Video. A group of professional bank robbers start to feel the heat from police when they unknowingly leave a clue at their latest heist.

IMDb's Guide to Horror. Edgar Wright's Top 10 Heist Movies. The guitar solo is played by Frey himself. The song became a major hit single, reaching No.

The music video for the song received heavy MTV airplay. It showed a film editor assembling scenes for Beverly Hills Cop while Frey and a band played the song in the adjacent room, with action scenes from the movie then directly interspersed.

Among the musicians shown in the video is saxophone player Beverly Dahlke-Smith the actual recording being made by session horn player David Woodford [5] and Frey's long-time drummer, Michael Huey.

The recording subsequently appeared on Frey's albums Glenn Frey Live and Solo Collection as well as on some various-artists "top hits" collections.

From Wikipedia, the free encyclopedia. Harold Faltermeyer Keith Forsey. Retrieved 29 Maggio Retrieved 3 April Australian Chart Book — Ö3 Austria Top

Heat Is On Video

180927 혼다 히토미 HEAT IS ON Der Teufel steckt im Detail. Rotationswärmetausher werden in der Lüftungstechnik verwendet. Die Stadt steht immer noch unter Beschuss. The bottom line is Stand nur 4 Wochen lang in die Holländische Top 40 Platz 31!!! The suspense is killing me. Die Maxiversion gefällt mir einen Tick besser, als der abgedroschene Singlemix. The people whose house this is don't know we're here. The witness is instructed on his obligation to be truthful. Dafür waren diese wirklich gut und weisen durchaus Eagles-Niveau auf.

Heat is on -

Na wenn das so ist - Ich aktiviere es wieder! Leider unterstützt Ihr Browser das Abspielen der Audiodatei nicht. Dieser Eintrag erscheint mir sehr dubios - ich finde auch überhaupt keine orginal mutterspra…. Die Vorstellung ist aus. Das Spiel ist aus. Insgesamt eine gute 5. Knapp an der 6 vorbei.

Diatomic gases such as hydrogen display some temperature dependence, and triatomic gases e. Before the development of the laws of thermodynamics, heat was measured by changes in the states of the participating bodies.

In general, most bodies expand on heating. In this circumstance, heating a body at a constant volume increases the pressure it exerts on its constraining walls, while heating at a constant pressure increases its volume.

Beyond this, most substances have three ordinarily recognized states of matter , solid, liquid, and gas.

Some can also exist in a plasma. Many have further, more finely differentiated, states of matter, such as for example, glass , and liquid crystal.

In many cases, at fixed temperature and pressure, a substance can exist in several distinct states of matter in what might be viewed as the same 'body'.

For example, ice may float in a glass of water. Then the ice and the water are said to constitute two phases within the 'body'. Definite rules are known, telling how distinct phases may coexist in a 'body'.

Mostly, at a fixed pressure, there is a definite temperature at which heating causes a solid to melt or evaporate, and a definite temperature at which heating causes a liquid to evaporate.

In such cases, cooling has the reverse effects. All of these, the commonest cases, fit with a rule that heating can be measured by changes of state of a body.

Such cases supply what are called thermometric bodies , that allow the definition of empirical temperatures. Before , all temperatures were defined in this way.

There was thus a tight link, apparently logically determined, between heat and temperature, though they were recognized as conceptually thoroughly distinct, especially by Joseph Black in the later eighteenth century.

There are important exceptions. They break the obviously apparent link between heat and temperature. They make it clear that empirical definitions of temperature are contingent on the peculiar properties of particular thermometric substances, and are thus precluded from the title 'absolute'.

It cannot be used as a thermometric substance near that temperature. Also, over a certain temperature range, ice contracts on heating. Moreover, many substances can exist in metastable states, such as with negative pressure, that survive only transiently and in very special conditions.

Such facts, sometimes called 'anomalous', are some of the reasons for the thermodynamic definition of absolute temperature.

In the early days of measurement of high temperatures, another factor was important, and used by Josiah Wedgwood in his pyrometer. The temperature reached in a process was estimated by the shrinkage of a sample of clay.

The higher the temperature, the more the shrinkage. But such shrinkage is irreversible. The clay does not expand again on cooling.

That is why it could be used for the measurement. It is not a thermometric material in the usual sense of the word.

Nevertheless, the thermodynamic definition of absolute temperature does make essential use of the concept of heat, with proper circumspection. According to Denbigh , the property of hotness is a concern of thermodynamics that should be defined without reference to the concept of heat.

Consideration of hotness leads to the concept of empirical temperature. If a physical system is inhomogeneous or very rapidly or irregularly changing, for example by turbulence, it may be impossible to characterize it by a temperature, but still there can be transfer of energy as heat between it and another system.

If a system has a physical state that is regular enough, and persists long enough to allow it to reach thermal equilibrium with a specified thermometer, then it has a temperature according to that thermometer.

An empirical thermometer registers degree of hotness for such a system. Such a temperature is called empirical.

This number is a measure of how hot the body is. Physical systems that are too turbulent to have temperatures may still differ in hotness.

A physical system that passes heat to another physical system is said to be the hotter of the two. More is required for the system to have a thermodynamic temperature.

Its behavior must be so regular that its empirical temperature is the same for all suitably calibrated and scaled thermometers, and then its hotness is said to lie on the one-dimensional hotness manifold.

This is also the reason that the zeroth law of thermodynamics is stated explicitly. If three physical systems, A , B , and C are each not in their own states of internal thermodynamic equilibrium, it is possible that, with suitable physical connections being made between them, A can heat B and B can heat C and C can heat A.

In non-equilibrium situations, cycles of flow are possible. It is the special and uniquely distinguishing characteristic of internal thermodynamic equilibrium that this possibility is not open to thermodynamic systems as distinguished amongst physical systems which are in their own states of internal thermodynamic equilibrium; this is the reason why the zeroth law of thermodynamics needs explicit statement.

That is to say, the relation 'is not colder than' between general non-equilibrium physical systems is not transitive, whereas, in contrast, the relation 'has no lower a temperature than' between thermodynamic systems in their own states of internal thermodynamic equilibrium is transitive.

It follows from this that the relation 'is in thermal equilibrium with' is transitive, which is one way of stating the zeroth law.

Just as temperature may be undefined for a sufficiently inhomogeneous system, so also may entropy be undefined for a system not in its own state of internal thermodynamic equilibrium.

For example, 'the temperature of the solar system' is not a defined quantity. Likewise, 'the entropy of the solar system' is not defined in classical thermodynamics.

It has not been possible to define non-equilibrium entropy, as a simple number for a whole system, in a clearly satisfactory way.

From Wikipedia, the free encyclopedia. This article is about a mode of transference of energy. For other uses, see Heat disambiguation.

The classical Carnot heat engine. Classical Statistical Chemical Quantum thermodynamics. Zeroth First Second Third. Conjugate variables in italics.

Carnot's theorem Clausius theorem Fundamental relation Ideal gas law. Free energy Free entropy. History General Heat Entropy Gas laws.

Entropy and time Entropy and life Brownian ratchet Maxwell's demon Heat death paradox Loschmidt's paradox Synergetics. Caloric theory Theory of heat.

Internal energy and Enthalpy. This section may need to be rewritten entirely to comply with Wikipedia's quality standards.

The discussion page may contain suggestions. This section does not cite any sources. Please help improve this section by adding citations to reliable sources.

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Blundell, Concepts in Thermal Physics , p. Clausius, Ueber die bewegende Kraft der Wärme und die Gesetze, welche sich daraus für die Wärmelehre selbst ableiten lassen , communication to the Academy of Berlin, February , published in Pogendorff's Annalen vol.

John Tyndall, London, , p. Sadi Carnot and the steam engine: Loeb, The Kinetic Theory of Gases , p. Guggenheim and with Professor N.

From this, Denbigh concludes "It seems, however, that when a system is able to exchange both heat and matter with its environment, it is impossible to make an unambiguous distinction between energy transported as heat and by the migration of matter, without already assuming the existence of the 'heat of transport'.

In the former case we can conceive the constituent particles of heated bodies to be, either in whole or in part, in a state of motion. In the latter we may suppose the particles to be removed by the process of heating, so as to exert attraction through greater space.

I am inclined to believe that both of these hypotheses will be found to hold good,—that in some instances, particularly in the case of sensible heat, or such as is indicated by the thermometer, heat will be found to consist in the living force of the particles of the bodies in which it is induced; whilst in others, particularly in the case of latent heat, the phenomena are produced by the separation of particle from particle, so as to cause them to attract one another through a greater space.

Novum Organum Scientiarum , translated by Devey, J. A translation may be found here. A mostly reliable translation is to be found at Kestin, J.

The Essential Dictionary of Science. Annalen der Physik Poggendoff's Annalen , Dec. Paris, , and in the Philosophical Magazine , August , s.

John van Voorst, 1 Paternoster Row. Also the second edition translated into English by W. Browne here and here. Non-equilibrium Thermodynamics , North-Holland, Amsterdam.

Reprinted , Dover Publications Inc. An Advanced Treatment for Chemists and Physicists fifth ed. Archived from the original PDF on 2 April Retrieved 23 Mar After a simple jewelry heist goes terribly wrong, the surviving criminals begin to suspect that one of them is a police informant.

An in-depth examination of the ways in which the U. Vietnam War impacts and disrupts the lives of people in a small industrial town in Pennsylvania.

Unscrupulous boxing promoters, violent bookmakers, a Russian gangster, incompetent amateur robbers and supposedly Jewish jewelers fight to track down a priceless stolen diamond.

When his secret bride is executed for assaulting an English soldier who tried to rape her, Sir William Wallace begins a revolt against King Edward I of England.

A mentally unstable veteran works as a nighttime taxi driver in New York City, where the perceived decadence and sleaze fuels his urge for violent action by attempting to liberate a presidential campaign worker and an underage prostitute.

Violence and mayhem ensue after a hunter stumbles upon a drug deal gone wrong and more than two million dollars in cash near the Rio Grande.

Hunters and their prey--Neil and his professional criminal crew hunt to score big money targets banks, vaults, armored cars and are, in turn, hunted by Lt.

A botched job puts Hanna onto their trail while they regroup and try to put together one last big 'retirement' score.

Neil and Vincent are similar in many ways, including their troubled personal lives. At a crucial moment in his life, Neil disobeys the dictum taught to him long ago by his criminal mentor--'Never have anything in your life that you can't walk out on in thirty seconds flat, if you spot the heat coming around the corner'--as he falls in love.

Thus the stage is set for the suspenseful ending I really believe this is one the great crime movies of all time.

It has some drawbacks that wouldn't make me recommend this for family viewing - tons of f- words by Al Pacino and a few bloody scenes, but as far as a fascinating crime story: This movie made modern-day history because it was the first time two of the great actors of this generation - Pacino and Robert De Niro - finally acted together in the same film.

Those two didn't disappoint, either. They were great to watch and one of the huge highlights of the film, to me, was when they faced each other in a simple conversation over a cup of coffee.

That conversation has always fascinated me, no matter how many times I've heard it. It was such a "landmark" scene that It's even the subject of a short documentary on the special-edition DVD.

As with the conversation scene, the shootout segment in the streets of Los Angeles still astounds me no matter how many times I see it.

The other action scenes are intense and memorable, too, and the cast in here is deep. This isn't just Pacino and De Niro.

Put that fabulous cast under Michael Mann, one of the best directors in business, add a great soundtrack and interesting camera-work and you have a great film.

At three hours long, it never bores one and at same time, doesn't overdo the action, either. I read one critic criticize this film because of the time taken to examine the personal lives of the main characters, but you can't have three hours of nothing but action.

The only scene I felt went on a bit too long was the ending chase at the airport, but that's nitpicking considering the film as a whole.

The recording subsequently appeared on Frey's albums Glenn Frey Live and Solo Collection as well as on some various-artists "top hits" collections.

From Wikipedia, the free encyclopedia. Harold Faltermeyer Keith Forsey. Retrieved 29 Maggio Retrieved 3 April Australian Chart Book — Ö3 Austria Top Library and Archives Canada.

Beverly Hills Cop series. Founded in Based in Miami, Florida. Miami Arena American Airlines Arena. Chicago Bulls New York Knicks.

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