Business information for Fly Guys about Excel Spreadsheet and Access Assignment

Business information for Fly Guys about Excel Spreadsheet and Access Database - Assignment Example In contrast, the Excel spreadsheets would keep displaying messages about a locked file and this might intimidate the passengers in addition to contributing to time wastage. Thus, Access database application is a better alternative as pertains to the support of the booking operations. Second, Access database uses structured query languages (SQL) to manipulate records. An even more striking aspect of this future is that the end-user can tailor the queries to suit the business needs. For example, it is possible generating reports based on criteria such as passengers involved in half journeys, passengers involved in full journeys and passengers who are most loyal to Fly Guys. On the other hand, Excel spreadsheets lack such fascinating features. Implicit in this is the point that a business which embraces Excel as an information management tool is likely to be restricted with regards to generating reports that can support business goals. So, MS Access database is better placed to meet the custom report generation needs at Fly Guys. Another reason why Fly Guys would need to focus on MS Access to address the custom report needs is its scalability and flexibility. In brief, Access can scale well and communicate seamlessly with nearly all other 21st century relational databases via open database connectivity (ODBC) connections. The only prerequisite for this capability is for the involved database administrator to have a thorough knowledge of the Fly Guys-owned MS Access database file. As Beskeen (2010) puts it, MS Access is a better option when it comes to information storage. In general, the application’s capabilities come in handy when a need arises to store information for a more elaborated time. This aspect suits the operation at Fly Guys because the records handled will inevitably rise.

Philosophy Token vs. Dualism or New Theory Essay

Philosophy Token vs. Dualism or New Theory - Essay Example In recognition of the mental states in relation to the brain, the Token Theory of mind upholds the analogy of realizations and supposes that the individual thought is identical with the individual brain state in which it corresponds. This philosophy reasoned that if mental states is a cacophony of thought processes then most likely it is identical to the internal state of the brain. In simplified terms; it is interaction of mind and body and the interaction of physical processes in the brain and parts of the body via the nervous system and there is nothing more than physical in the way it functions. Smart (1956) said that the mental state's 'desire for a cup of coffee' would thus be nothing more than the "firing of certain neurons in certain brain regions". The mental phenomenon is then equated with the processes of the brain and is actually considered as the fundamental features of the brain. A heavy challenge under this theory would fall under the category of need. The explanation seems to relay the idea that humans regardless of affiliation feel hunger and hunger is identical to a certain brain state. Each mental state is said to be identical to an individual brain state without any categorization. ... Dualism meanwhile is a complex model that divides the human beings into two substances of matter and mind and separates the mind from the body. In Plato and Aristotle both maintained, for different reasons, "that a man's 'intelligence' (as a faculty of the mind or soul) could not be identified with, or explained in terms of his physical body". In a non-physical form, dualism exists to identify the mind as the control factor in movements along with other components. Dualism however explains the property of the physical (skin, bones and the entire system of the human body) in response to the mental (thoughts and feelings). For example, in simple dualism: a needle puncturing your finger is a physical trauma and causes you to perceive pain; as a physical response one either withdraws the hand or voice out a verbal reaction to pain. In other words there is direct physical interaction between the mind and the body. In more complex dualistic setting and explanation: when one sees a car, the input is placed on the senses and sends out signals through the senses which interpret the experience in the brain whereby a mental image is produced. Scientifically this could be acceptable, but the simplest is always the best answer when trying to find the most natural relation to a human's mind. Despite a certain initial clarity, the token identity theory is still faced with a heavy challenge in the form of the Putnam's(1967) multiple realizations. If this is a difference however, then pain cannot be identical to a certain brain state and thus the identity theory is empirically unfounded for her. It dwells on the neurological aspect of the mind and the

James Madison's 51st Federalist Paper Essay Example | Topics and Well Written Essays - 2000 words

James Madison's 51st Federalist Paper - Essay Example However, the framers identified certain realistic problems in making all offices elective. Especially, the judicial branch would face problems because the typical person does not have knowledge about what qualifications judges ought to have. Judges must have great capability, but also not have any political pressures. While federal judges are selected for life, their philosophy will not be inclined via the president who appoints them or the senators whose permission the president will take. All the arguments were generated due to his past life as he was in aristocratic family in Port Conway so his thinking was also very refined. His personal background did not have anything do with any kind of discrimination of race, class and gender. The background which affected his thinking was his education, refined family background and experience which he gained from Thomas Jefferson Madison's writings are filled with figurative and fancy language. In today's terms, a faction is a special interest group. They are a lot of groups of citizens who make a try to advance their thoughts or economic interests at the cost of other citizens or by methods that conflict with the public good. To be in command of a minority faction, there are two alternatives. One alternative could be to eliminate whatever is the reason behind the rise of the faction. Nevertheless, this is impractical. Thus, a second proposal was prepared. In this proposal Madison states that in order to have power over factions one does not need to its causes, but control its effectiveness. James Madison's Federalist, No. 51, is a transparent expression of views and guiding principle for a new government. He was a strong devotee and member of the Federalists whose key beliefs supported the Constitution. They also thought that the Articles of Confederation required rewriting so that it would be possible for the new central government to control the power of the states. Madison begins possibly the most well-known of the Federalist papers, Federalist No.51, by stating that one of the strongest arguments in favor of the Constitution is the fact that it establishes a government capable of controlling the violence and damage caused by factions. Madison believes that the factions are groups who get together to defend and support their special economic interests as well as political opinions. Even though these factions are different from each other, they often work in opposition to the public interests, and violate the rights of others. Equally supporters as well as opponents of the plan are troubled by the political instability which is caused by opponent factions. The state governments have not been successful in resolving this issue; in fact the state of affairs is so challenging that people are disappointed with all politicians and hold government the reasonable for their troubles. As a result, a kind of popular government that can deal effectively with this crisis has a lot to suggest it. Given the temperament of man, factions are predictable. As long as every man has diverse opinions, have unequal wealth, and have different amount of property, they will carry on socializing with people who more like them. Both severe and small reasons account for the creation of factions however the most vital foundation of faction is the unequally distributed property. Men

Comparing and contrating selena gomez and miley cyrus Essay Example for Free

Comparing and contrating selena gomez and miley cyrus Essay Hey, pop culture consumers and the world at large, the New York Times wants you to know that there is a distinct difference between Miley Cyrus and Selena Gomez. In a recent piece by Jon Caramanica, the Times breaks down the professional and personal trajectory between the two rising starlets, comparing their similar beginnings and their increasingly divergent paths. In it, he writes, Of late, Miley Cyrus, 20, and Selena Gomez, who turned 21 on Monday, have each been pushing back in different ways — Ms. Gomez with her role in the film Spring Breakers, and Ms. Cyrus with her sometimes erratic, sometimes free-spirited tabloid life. He then goes to argue the closer that Miley Cyrus artistic output mirrors her personal life, the better she becomes. The word choices used to describe the two pop princesses demonstrate a clear delineation between Cyrus and Gomez. Cyruss process includes feeling out new forms of rebellion, including the touristic appropriation of black culture, while Gomezs is particularly milquetoast. Her newest album, according to Caramanica, is breathy, wide-ranging, largely toothless. Caramanica is right to turn to these two young actresses/idols/musicians as a barometer of the pop cultural world, because they are certainly exemplary of the state of pop culture (and, of course, tabloid culture, as well). Both fulfill reasonable, identifiable, relatable roles for young women. Miley, the rambunctious rebel who is using her music to jettison her identity forward; Selena, a biracial young woman who is poised, graceful, and a friend any young girl would want to have; and even, to extend the comparisons of other young stars — Demi Lovato as the impassioned, slightly tortured diva, and Vanessa Hudgens as the laid-back West Coast bohemian who has eschewed music for film. Yet, for all of their seeming differences, Caramanica neglects to point out the most fascinating thing these two share: their similarities. Miley and Selena are both fervent anti-bullying advocates, loyally devoted to their fans, and welcome all types of listeners. Both of them want the population at large to believe that they are good people, even though they make bad choices — and they encourage their devotees to be kind to one anothereven when they make bad choices, too. Young girls respond to both Miley and Selena because the specific personality traits (which are, according to Caramanica, rebellious and safe, respectively) they sell to us are appealing. Where Miley harnesses an inner rebel, Selena embraces a wholesome good time in a pure, unself-conscious way (unlike, say, Taylor Swift, whose self-effacing hand-wringing is what makes her so popular with adults). Yet, it is their open accessibility and honestness, along with their all-inclusive message, that keeps a younger generation hungry. And having todays former Disney stars feel out their own way while also espousing tolerance and respect — no matter how calculated that way may be — is so much better than being subjected to a child star who insincerely sells the virginal act. The music, it appears, is secondary. (NY Times)

Generation of Extreme Ultraviolet Radiation

Generation of Extreme Ultraviolet Radiation Generation of Extreme Ultraviolet Radiation from Intense Laser-Plasma Interactions using Two-Colour Harmonics BRIEF HISTORY Over the past few decades breakthroughs in the production of intense laser fields have meant that multi-terawatt and even petawatt systems are now standard in laboratories**. This has been achieved through reduction of the pulse duration, originally from nanosecond pulses down to femtosecond and recently reaching attosecond levels (1as =10-18s)**. This coupled with important improvements to systems, such as the chirped pulse amplification technique (CPA)**, has allowed laser pulses to be amplified to higher peak powers than ever before and used in laser-matter interactions. The resulting scientific drive from developments such as these pushed achievable laser intensities from 109W/cm2 to the 1014W/cm2, at which the interaction between these high intensity lasers and dense electron-free gas was studied**. Only recently thanks to advances in both laser performance and computer simulation tools has study on laser-plasma interactions in the generation of HHG made progress, providing the possibility to generate sources of incoherent electromagnetic radiation of short wavelength and pulse durations**. As further study was carried out on the interaction of light with relativistic free electrons in plasma, it has reached a point now in which generation of high-harmonics of the fundamental laser, soft and hard x-rays, and shorter pulse duration (1as) lasers of intensities reaching 1018W/cm2 are now possible**. Due to this the generation of high-order-harmonics from high-intensity laser interactions has been a major area of attoscience research within the last decade. HHG PRODUCTION High harmonic generation (HHG) refers to the process in which a high intensity laser pulse is focused onto a target, classically a noble gas, in which strong nonlinear interactions result in the generation of very high harmonics of the optical frequency of the pulse**. This will occur for intensities of 1014W/cm2 and above, where typically only a small amount of this energy is converted into the higher harmonics. From these high-harmonics, spatially and temporally coherent attosecond pulses of extreme ultraviolet light can be generated, which can then be used as a reliable source of highly tuneable short wavelength radiation in many different applications e.g. x-ray spectroscopy**. In the case of high intensity laser-gas interactions this is achieved by tailoring the intensity of the laser pulse so that its electric field amplitude is similar to the electric field in the target atoms**. From this the lasers electric field is able to remove electrons from the atoms through tunnel ionisation, at which point the electrons are accelerated in the field and, with certain conditions controlled, are made to collide with the newly created ion upon recombination. The resulting collision generates the emission of high energy photons**, as shown in fig 1. Fig. 1: HHG three step model. This is known as the three step model; electron is detached from atom through tunnel ionisation, then accelerated within the field away from atom, then accelerated back towards atom where it collides and recombines, from this collision all the energy lost appears as emitted HHG ultraviolet photons. HHG from laser-gas interactions have been used extensively to generate attosecond pulses but is limited in flux and photon energy by low conversion efficiencies between the driving laser energy and the attosecond pulses, this can be attributed to two key factors; loss of phase matching between the driving laser to the generated extreme ultraviolet (XUV) radiation as its propagated through the gas over a relatively large distance, and a restriction on the intensity of the driving laser due to the ionisation threshold of the target gas, this saturation intensity is roughly 1016W/cm2**. Meaning laser intensities above this threshold limit will over-ionise the gas leaving no neutral atoms left to generate the XUV harmonics. The use of laser-solid interaction offers the opportunity of reaching much higher attosecond pulse intensities and generation efficiencies beyond the capabilities of gas based HHG**. The method of generating high-harmonics in laser-solid interactions is fundamentally different than that of laser-gas interactions. Interaction of intense ultrashort laser pulses (of pulse duration around a few femtoseconds) on an optically polished solid surface results in the target surface being completely ionised, generating a dense plasma which will act as a mirror, called a plasma mirror**. The reflection of these high intensity laser pulses will be affected by a wave motion set-up in the electrons within the plasma surface causing it to distort the reflected laser field, resulting in the production of upshifted light pulses and the generation of high-order harmonics**. Due to the coherent nature of this process, these generated harmonics are phase-locked and emerge as attosecond pulse. Fig. 2 Laser pulse moving towards overdense plasma. A key property of this plasma is its electron density, this determines whether the laser is reflected, absorbed or not allowed to pass through. This is known as the density gradient scale length, as the laser pulse interacts with the target and forms a plasma it creates a profile that extends out into the vacuum, forming a plasma density profile. This is a critical factor in HHG and consists of two regions: Overdense scale length, Lod If the electron density is equal to the critical density of the target or above, extending up to the maximum target density, the laser pulse is unable to penetrate through the target and is so reflected or absorbed. Underdense scale length, Lud If the electron density is below this critical density the laser will penetrate through, with some absorption. Fig. 3 Plasma density profile, Lud is underdense region, Lod is overdense region. The critical density is determined from: Where is the angular frequency of the laser. As stated before the target surface is highly ionised by the leading edge of the laser pulse, known as the pre-pulse, therefore becoming rapidly over-dense and creating a plasma mirror of sufficient electron density, ne>nc**. HHG within plasma requires laser intensities >1015W/cm2 for 800nm field**, which is usually stated in terms of a normalised vector potential of a ­0, where: In which; e and m are electron charge and electron mass respectively. c is speed of light in vacuum. E is the amplitude of the lasers electric field. I is the lasers intensity. à Ã¢â‚¬ °l is the laser frequency and ÃŽÂ »l is the laser wavelength. Therefore HHG in plasma requires at least an a0à ¢Ã¢â‚¬ °Ã‚ ¥0.03. Recently is was discovered** that there are two mechanisms that lead to HHG from solid density plasma surfaces; Relativistic oscillating mirror (ROM) Coherent wake emission (CWE) These two process result in different distortions to the reflected laser field and therefore a completely different harmonic spectra produced. CWE Coherent wake emission is a process of three steps; Electrons on the surface of the plasma are drawn into the vacuum by the laser field and accelerated back into the dense plasma once they have gained energy from the driving laser field. When propagating within the dense plasma these fast electrons form ultrashort bunches, creating plasma oscillations in their wake. Within the non-uniform region of the plasma (produced from the density gradient between the plasma-vacuum boundary) the electron oscillations will radiate energy in the form of light of various local plasma frequencies found within this gradient. This process will occur once for every laser cycle therefore the spectrum of the emitted light will consist of harmonics of the laser frequency, in which CWE harmonic spectra have a cutoff at the maximum plasma frequency à Ã¢â‚¬ °Ã‚ ­Ã‚ ­pmax **. This mechanism is predominant at moderately relativistic intensities of a0à ¢Ã¢â‚¬ °Ã‚ ¤1, and short but finite plasma gradient lengths of **. Coherent wake emission has only recently been identified as a factor in HHG in laser-solid interactions but it is known that it along with ROM contributes to the generation of high-harmonic orders below à Ã¢â‚¬ °Ã‚ ­Ã‚ ­pmax and the strength of their respective influence below this threshold is determined by laser intensity**. ROM The other mechanism involved in the generation of high-harmonics from laser-plasma interactions is the relativistic oscillating mirror process, this dominates for relativistic normalised vector potentials of a0>>1, although recent studies have shown that ROM harmonics can be observed even at lower intensities when the plasma gradient length is about **. ROM process occurs when surface electrons in the plasma are oscillated collectively by the high intensity incident laser field to relativistic speeds, the plasma will reflect what it observes as a laser pulse of frequency à Ã¢â‚¬ °+. This à Ã¢â‚¬ °+ frequency is a higher upshifted frequency of the fundamental pulse due to a Doppler effect produced from the relative motion of the laser field to the moving reflection point on the oscillating plasma surface. The actual reflected laser pulse will have a frequency of à Ã¢â‚¬ °++ due to a second Doppler upshift effect as it moves towards an observer/target. This is known as Einsteins relativistic Doppler effect, in which the reflected pulse frequency is upshifted by a factor of 4ÃŽÂ ³2**. Fig 4. Schematic of a relativistic oscillating critical density plasma interaction. From past research it has been found that from this mechanism a power-law decay scaling of I(n)ROMn-8/3 is dominant (where n is the harmonic order) in the harmonic spectrum for harmonic orders above the CWE cut-off point, nCWE,** this is the harmonic order related to the maximum plasma frequency of the target, à Ã¢â‚¬ °pmax, mentioned previously. Where: nCWE = nà Ã¢â‚¬ °max = à Ã¢â‚¬ °pmax/à Ã¢â‚¬ °l = In which; à Ã¢â‚¬ °l is the frequency of the laser, is the maximum electron density of the target, Nc is the critical density shown previously. From this process initial femtosecond pulses can be used to create attosecond pulses. When coupled to a relativistic oscillating mirror it adds an oscillatory extension to Einsteins relativistic Doppler effect, so due to the periodic motion of the mirror to the laser field and the double Doppler upshifts this results in the production of extreme ultraviolet (XUV) harmonics**. These ultra-short pulses have been the focus of much scientific research recently as they offer a promising way to resolve in the time domain the ultrafast dynamics of electrons within materials**. Although the relativistic oscillating mirror process is more suited as a macroscopic model for the effective reflection point of the laser field. It assumes that the surface electrons bunch together as the target is ionised and move out into the vacuum to form the plasma where they remain in the overdense region ensuring that the laser field is completely reflected. More recently studies have discovered there is another mechanism in the relativistic regime that can contribute to the harmonic spectrum via a different process entirely. CSE This other process is known as Coherent synchrotron emission (CSE)** and is needed to explain observations that do not fit the previous two models, in which dense electron nanobunches are created at the plasma-vacuum boundary where they produce coherent XUV radiation through coherent synchrotron emission. This is a microscopic model of HHG in laser-solid interactions. It models the electrons in the plasma moving, in dense bunches, under the influence of the incident laser field and subsequent fields produced from the movement of charges within the plasma. These nanobunches are periodically formed and coherently accelerated through an instantaneously synchrotron-like orbit during each laser cycle, for oblique laser incidences. As certain conditions, such as ultrashort plasma density scale length, are met these bunches emit bursts of sub-femtosecond intense high-frequency radiation. This radiation has properties dependent on the electron trajectories and it has been shown that it can b e modelled as synchrotron radiation**, therefore the coherent XUV emissions are distinctly different from that produced in ROM from relativistic Doppler upshifts. In reality actual electron dynamics may be a mix of CSE and ROM, but due to the complex nature of the changing fields within a plasma it makes it impossible to analytically model with accuracy. Therefore requiring the use of computer simulations to deal with the electron trajectories and their respective radiation emissions. PREVIOUS EXPERIMENTS Based on the work of Edwards et al, 2014, in which the study of attosecond XUV pulse generation from relativistic driven overdense plasma targets with two-colour incident light was performed they used 1D, three velocity, particle-in-cell (PIC) code simulations, which treat oblique incidence with boosted frames, to show how pulse intensity can be improved. They converted a small amount (~5%) of the fundamental laser field energy to an additional laser operating at the second harmonic of the fundamental frequency, to significantly enhance the intensity of the generated attosecond pulses by multiple orders of magnitude. This was based on previous work in which mixing of the fundamental driving laser frequency with the second harmonic was performed on laser-gas interactions to increase the attosecond pulse intensity and isolation (K. J. Schafer et al, 1992). Edwards demonstrated that a significant improvement was also possible through this mixing method in laser-solid interactions following the Similarity theory (proposed by Gordienko and Pukhov,**), that suggests the behaviour of laser-plasma interactions follow a similarity parameter of: 1/S = a0/N à Ã¢â‚¬ °l Where S = ne/a0nc, is a similarity parameter and N = ne/nc which is the ratio of electron density of the plasma to its critical density. Therefore from this it would appear that by doubling à Ã¢â‚¬ °l while using the same laser field amplitude the reflected attosecond pulse intensity would also be increase by a factor of two. One of the main limiting parameters in these experiments is the achievable value of a0, while the largest solid material value of N (lithium at ÃŽÂ »=800nm) is 75, so this type of frequency doubling appears to be a promising pathway to optimising attosecond pulse intensity, although a drawback of this is the negative effect it has on the isolation of the reflected pulses. Therefore they stated that a two-colour method, of partially converting a portion of the fundamental laser field energy to the second harmonic, would be a more attractive alternative. Through this process the advantages of using a higher incident frequency, by increasing the gradient of the electric field at certain points within the pulse generation cycle, without the related decrease in pulse isolation and loss of energy associated to simple frequency doubling can be exploited. In their study they used a normal-incidence beam on a step-like plasma density profile using a mix of the first and second harmonic with a phase difference of to produce harmonics with a higher intensity than either incident field individually. They demonstrate substantial gains after the addition of a small amount of the second harmonic to achieve attosecond pulse enhancement of factors >10. As well as a 10-fold enhancement when using density gradients of 0.05ÃŽÂ » and 0.15ÃŽÂ » with conversions of the fundamental to the second harmonic of 5%-10% at an angle of incidence of à Ã‚ ´=30o. Therefore Edwards was able to go on and state that the relative phase of the two incident harmonics were a critical factor in the improvement in attosecond pulse intensity. This is due to the difference in the driving electric field waveform and corresponding resultant electron motion as is varied. Where they linked the strongest attosecond pulse intensities with sharp transitions in the driving electric field that are aided by the addition of the second harmonic at optimum phases, while phases that break the driving field transition reduce the attosecond intensities to levels sometimes substantially below what could be achieved pre-mixing of the harmonics. Therefore when harmonics are combined without thought to their phases they do not always improve the attosecond strength. Further detail into the trajectories of dense electron bunches, which emit synchrotron like radiation (CSE) was given to help explain this effect, where supressed pulse electrons were shown to follow a longer and slower motion before being accelerated and subsequently emitting, resulting in longer elongated trajectories. Whereas electrons that contribute to the improvement of the attosecond pulse strength are shown to experience a larger field before and during emission. This meant their velocity and acceleration components were larger than the suppressed electrons, giving them more energy as it is driven back into the plasma. Overall they state that the larger the electric field experienced by the electrons increases the intensity of the reflected attosecond pulse, due to the number of electrons travelling in a dense bunch increasing as this larger field that the electrons near the surface experience compresses them into higher density bunches. Another study performed by Yeung et al, 2016, focused on controlling the attosecond motion of strongly driven electrons at the boundary between the pre-formed plasma and the vacuum. They demonstrated experimentally that by precisely adding an additional laser field, at the second harmonic of the fundamental driving frequency, attosecond control over the trajectories of the dense electron bunches involved in intense laser-plasma interactions can be achieved. From this considerable improvements in the high-harmonic generation intensity was observed, which confirms the theoretical work by Edwards in two-colour fields reviewed previously while developing upon this to further factors. Experimentally they showed that attosecond control over the phase relationship of the two driving fields is necessary to optimise the reflected attosecond pulse intensity. While also using PIC simulations to determine the optimal and worst phase relationships, in which a phase of was found to optimise the emission. Microscopic focus determined that during each cycle the emission of the attosecond pulse begins as a primary electron bunch which is compressed and then quickly accelerated away from the surface up to relativistic velocities, from here it emits before it disperses and returns back to the plasma. Secondary bunches are also present but these were found not to have a significant effect harmonic spectrum for orders >20. These bunches were found to emit when their velocities where at their max, which confirmed that the two-colour field phase matched the emitted XUV to the acceleration produced from the fundamental laser field. While at the poorest phase relationship, which Yeung found to be , a plateau in the driving laser field is created which impedes the acceleration of the electrons from the surface, therefore reducing the density of the electron bunch produced that can emit. They concluded from the data provided by the simulations that control of the relative phase of the two colour driving fields has a significant effect the electron bunch dynamics. While from the experimental data their collected it was demonstrated that the HHG produced from the two-colour field was increased substantially when no laser pre-pulse was involved, or equivalently when the plasma has shorter density scale length. Confirming the work of Edwards et al, 2014, that two-colour fields generate significantly more higher-harmonic orders than that of a fundamental field alone, even when only a small percentage (5%-10%) of the fundamental laser energy is converted to the second harmonic. INTRODUCTION TO TWO-COLOUR HARMONICS - ABSTRACT BRIEF SUMMARY OF EXPERIMENT, RESULTS AND CONCLUSION 1x INTRODUCTION BRIEF HISTORY .5x HHG PRODUCTION .5x CWE 1x ROM 2x (inc. plasma theory e.g. scale length) CSE 1x COMPARISON WITH GAS EXPERIMENTS 1x PAST EXPERIMENTS LEADING UP TO THIS ONE 2x INTRODUCTION INTO SPECIFICS OF THIS EXPERIMENT 1x METHOD PIC CODES EXPLAINED 2x EPOCH DETAILS 1x LASER DETAILS 1x PROCESS OF ANALYSIS .5x CREATION OF GRAPHS .5x RESULTS GRAPHS COMPARE CONTRAST IMPLICATIONS CONCLUSION FURUTRE RESEARCH 1x IMPROVEMENTS 1x         

More Than Meets The Eye Essays -- Literary Analysis, Shakespeare

Throughout history, individuals have notoriously been subject to higher powers.   This form of ownership of an individual exemplifies itself in slavery, indentured servitude, and even in the governmental systems that hold reign over the general population.   The ability of one person to rule over another arises from both moral and physical inequalities.   Jean-Jacques Rousseau, a prominent Genevan philosopher, attempts to uncover the origin of inequality.   In The Second Discourse, Rousseau systematically dissects the movement of humans away from their natural state and attempts to explain how inequality is derived.   Shakespeare’s The Tempest tells the tale of a usurped Duke, Prospero, who suffers a life of exile on a mystical island.   Overthrown by his own brother Antonio, Prospero seeks revenge.   In a series of carefully planned events, Prospero strands a group of European lords on his isle, one of whom is Antonio.  Ã‚   Using his knowledge of magic, Prosp ero succeeds at obtaining control over his kingdom of Milan.   On the surface, The Tempest appears unrelated to the work by Rousseau.   However, quite the contrary is true. The Tempest is inundated with many similar philosophical ideas discussed in The Second Discourse.   When comparing The Tempest and The Second Discourse, the themes of inequality versus equality, nature versus nurture, and savage man versus civilized man prevail.   As described in The Tempest, it is clear to identify that inequality exists amongst the island’s inhabitants. Shakespeare illustrates this inequality with reference to the character Prospero. After being dethroned as the Duke of Milan, Prospero and his daughter Miranda are exiled from the country and set to sea on a raft. With the aide of supplies and magic ... ...for food and shelter. Whether barbaric or civilized, the actions of both Caliban and Prospero combine in a most interesting manner.   Ã‚  Ã‚   The Tempest and The Second Discourse are inundated with the themes of inequality versus equality, nature versus nurture, and savage man versus civil man.   Jean-Jacques Rousseau, a prominent philosopher of his time and author of The Second Discourse, attempts to pinpoint the origin of inequality.   In doing so, he interestingly analyzes the differences between civilized man and natural man.   William Shakespeare, a prolific writer during the Elizabethan Era and author of The Tempest, draws attention to issues facing mankind.   While at first glance these two literary pieces appear to be unrelated, after analysis, they offer many similarities.   What is most central is that both pieces offer insight into authority, power, and equality. More Than Meets The Eye Essays -- Literary Analysis, Shakespeare Throughout history, individuals have notoriously been subject to higher powers.   This form of ownership of an individual exemplifies itself in slavery, indentured servitude, and even in the governmental systems that hold reign over the general population.   The ability of one person to rule over another arises from both moral and physical inequalities.   Jean-Jacques Rousseau, a prominent Genevan philosopher, attempts to uncover the origin of inequality.   In The Second Discourse, Rousseau systematically dissects the movement of humans away from their natural state and attempts to explain how inequality is derived.   Shakespeare’s The Tempest tells the tale of a usurped Duke, Prospero, who suffers a life of exile on a mystical island.   Overthrown by his own brother Antonio, Prospero seeks revenge.   In a series of carefully planned events, Prospero strands a group of European lords on his isle, one of whom is Antonio.  Ã‚   Using his knowledge of magic, Prosp ero succeeds at obtaining control over his kingdom of Milan.   On the surface, The Tempest appears unrelated to the work by Rousseau.   However, quite the contrary is true. The Tempest is inundated with many similar philosophical ideas discussed in The Second Discourse.   When comparing The Tempest and The Second Discourse, the themes of inequality versus equality, nature versus nurture, and savage man versus civilized man prevail.   As described in The Tempest, it is clear to identify that inequality exists amongst the island’s inhabitants. Shakespeare illustrates this inequality with reference to the character Prospero. After being dethroned as the Duke of Milan, Prospero and his daughter Miranda are exiled from the country and set to sea on a raft. With the aide of supplies and magic ... ...for food and shelter. Whether barbaric or civilized, the actions of both Caliban and Prospero combine in a most interesting manner.   Ã‚  Ã‚   The Tempest and The Second Discourse are inundated with the themes of inequality versus equality, nature versus nurture, and savage man versus civil man.   Jean-Jacques Rousseau, a prominent philosopher of his time and author of The Second Discourse, attempts to pinpoint the origin of inequality.   In doing so, he interestingly analyzes the differences between civilized man and natural man.   William Shakespeare, a prolific writer during the Elizabethan Era and author of The Tempest, draws attention to issues facing mankind.   While at first glance these two literary pieces appear to be unrelated, after analysis, they offer many similarities.   What is most central is that both pieces offer insight into authority, power, and equality.

3g networks

â€Å"Knock , Knock. Who's There? It's the Papparzzi† In 1960 Federico Fellini directed a film intitled â€Å"La Dole Vlta†. In the film actor Walter Santesso plays a news photographer named ‘Paparazzo'. Little did any of them know the term ‘paparazzo' would be a staple in households and news lines everywhere. In today's times the paparazzi are considered to be rutheless photographers who will do anything to get a snapshot of a celebrity or athelete. Whether it be them leaving practice or a movie set, going out to clubs at night, grocery shopping, or even walking their kids to school.Some say paparazzi are down right (excuse my french) assholes. Standing in line at the supermarket or walking down the streets in some cities, we see magazines or tabloids that have celebrites faces plastered on them in sometimes disapproving situations. We never wonder how the pictures got taken or what lengths it took to get such an amazing or sometimes horrid shot. In June of 2005, then 18 year old Lindsay Lohan's car was hit by photographer Galo Cesar Ramirez who was trying to follow her. In an interview she said â€Å"A line needs to be drawn in terms of getting violent. † She then Joined other celebs includingCameron Diaz and Justin Timberlake in trying to prevent the â€Å"pap† from invading their personal space. In several instances the paparazzi claim the First Amendment, which prohibits the making of any law abridging the freedom of speech, infringing on the freedom of the press, or interfering with the right to peaceably assemble. It is very hard for a celebrity to not seem like a hyprocrite when asking for the paparazzi to leave them alone. When leaving your â€Å"normal† life behind to partake in the lavish yet dangerous life of being famous, there are some things that comes with the erritory.