Making a Difference through Nursing Essay Example | Topics and Well Written Essays - 3250 words

Making a Difference through Nursing - Essay Example Since hepatitis C was first recognized in 1989, it has gained increasing significance. More than half the number of individuals exposed to HCV develop chronic infection; and among them around 20% to 30% develop liver cirrhosis and/ or hepatocellular carcinoma within twenty to thirty years. Improved diagnostic techniques and possibilities of therapeutic intervention have brought out the role of HCV infection in acute and chronic liver disease (Hentiges & Wands, 1997: 521). This paper proposes to examine the hepatitis C virus (HCV), its pathophysiology and various other dimensions of the infection including the public health implications, the importance of raising public awareness, clinical governance and surveillance. Hepatitis C infection has been found worldwide, especially in the southeast Asian countries, in northern African and Arabian countries, and with highest prevalences in the Ukraine and in the central African countries of Gabon and Cameroon, as well as in Egypt where up to 14.5% of the population is infected with the Hepatitis C virus. Size of the Problem: HCV infection in Hong Kong is associated predominantly with multiple blood transfusions (67% to 87% anti-HCV positive) and intravenous drug abuse (56% anti-HCV positive). However, the source of infection is unidentified in a large number of HCV carriers (Ho & Wu, 1995: 15). The world-wide prevalence of hepatitis C is estimated at 170 million people or 3% of the global population, with a disease spectrum ranging from mild to severe chronic hepatitis, cirrhosis and hepatocellular carcinoma. Most people infected with HCV are unaware of their clinical status, due to which the actual prevalence of the infection may be under-reported. Around 85% of infected persons are chronically infected by the virus, and 70% of the infected develop chronic hepatitis, cirrhosis and hepatocellular carcinoma

Management and Organisation individual report Essay - 2

Management and Organisation individual report - Essay Example These two are derived from the set textbook by Mullins, Essentials of organisational behavior, 3rd Edition. Further, competitive advantage will also be explicated with inputs of strategy and structure on the management process, and lastly, a conclusion will be drawn as the researcher’s overall perception regarding the nature of management and the integration of strategy and structure. Management is the method consists of modelling and supporting of a particular ambience wherein entities are effectively working together in one purpose (Koontz & Weihrich, 2008, p. 5). The management of activities is usually held by a manager or a supervisor to ensure the effectiveness of operations. The management of it is integrated with strategies, following the organisational structure of the organisation. As defined by James Brian Quinn (1980, p. 3), strategy is the model that incorporates an entity’s principal aims, policies, and series of operations into a coherent entirety (quoted in John & Gilles, 1997, p.176). Strategy is usually long term in nature as compared to tactics that are also formulated to achieve a specific goal but in a short period of time. Organisational structure pertains to the formal flow of organisational knowledge, precise sectioning of various business operations, and the model of frameworks to assure the effectiveness and efficiency of business activities across different units (Daft, 2010, p. 90). This includes precise organisational levels, concise departments, and optimum system to achieve the highest degree of efficiency towards job performance. The disposition of management is derived from the notion that what it is inculcated in the minds of the managers that are required to be understood (Stewart, 1984, p. 324). In specific terms, the nature of management can be depicted as the things that managers should do in order to create an effective strategy. Another notion in understanding the disposition of management depicts the certain

Coincidence Counting With NAI Scintillation Detectors

Coincidence Counting With NAI Scintillation Detectors ABSTRACT Coincidence counting is a technique employed in nuclear medicine for PET imaging. This technique utilizes a positron emitting radionuclide that is injected into patients to track biochemical and physiological processes. The positron annihilates with an electron and emit two 0.511MeV gamma rays which are detected simultaneously by two scintillation detectors. In the experiment, two gamma ray sources, 60Co and 22Na were used with a NaI scintillation counter. A single channel analyzer (SCA) was used to count the number of voltage pulses whose height fell within the gate width. The absolute efficiency and intrinsic efficiency was obtained as a function of distance. Real and random coincidences were determined from the spectrum obtained with varying gate width and gate delay for each source. The optimum gate width obtained was 5 µsec for both sources with gate delays of 1.2 µsec and 0.2 µsec for 22Na and 60Co respectively. The real coincidences for 22Na and 60Co were found to be 200 .1  ± 2.3 and 76.5  ± 1.7 respectively. The random coincidences obtained were 25.1  ± 3.4 and 13.4  ± 2.6 for 22Na and 60Co respectively. This was determined by using the LINEST function. The percentage thus of random to real coincidences obtained in this experiment was 12.54  ± 1.85 % and 17.52  ± 3.81 % for 22Na and 60Co respectively. It was deduced that the uncertainty in determining a random coincidence was higher in 60Co than in 22Na. the magnitude of the uncertainty is as a result of fluctuations in the instrumentation. Hence the Na system is more efficient for coincidence counting and so it is useful in the PET system. INTRODUCTION Coincident counting is a radiological measuring technique that is utilised in the nuclear medicine in the PET scan whereby two photons emitted from an event are detected simultaneously by a ring of detectors. Sodium Fluoride (F18-NaF) is the positron-emitting radionuclide employed in PET for bone imaging [1]. Upon decay, the positron are emitted which travels for a short distance and under Compton’s scattering thereby loosing most of its energy. It then undergoes annihilation with an electron and emit two high energy 0.511MeV photons. The 0.511MeV photons are emitted 180 degrees apart and interact with the PET detector rings at opposite sites. [2] The detectors are made up of scintillation crystals coupled with photomultiplier tubes powered by a high voltage which produces a pulse with a height proportional to the gamma-ray energy. A SCA counts the number of voltage pulses whose height falls within a predetermined window of photon energies. Coincidence measurement is utilised when a single detector cannot produce all the information expected, as gamma rays are randomly produced, hence the need to set several detectors. Real coincidences occur when two photons are emitted in coincidence from the same annihilation event and are detected simultaneously within a certain time frame set by the gate width. Random coincidences occur when two photons emitted from different events are detected simultaneously within the time frame of the gate width. [3] The gate width determines the time window within which the simultaneous emission of the gammas are detected. The optimum gate width therefore will ensure that the maximum number of real coincidences are detected to minimise the events of random coincidences. In the ideal situation when the gate width is zero the real coincidences can be observed, and with an increase in gate width the random coincidences can be observed. In the PET scan, this will ensure efficiency of the coincidence system. The need for the gate delay is to enable the second pulse to be detected within the time frame of the gate width and this is usually a minute time frame. It takes into account the minute fluctuations that occur at time of pulses. By alternating the gate delay and gate width, the rate of coincidence can be determined. In this experiment the two sources used were 60Co and 22Na. 60Co emit two gamma rays upon beta decay at energies 1.3325Mev and 1.1732MeV with 60Ni daughter nuclide. The 22Na undergoes a beta decay and electron capture decay with the emission of a 1.275MeV gamma photons and two 0.511Mev upon interactions with the detector material. The positron from the beta decay of 22Na annihilates an electron of the detector and emit the two gammas at 0.511Mev energies at 1800. The coincidence counting system records just a certain portion of events depending on the solid angle as a function of distance. Coincidence counting as a function of distance is maximum in the middle and zero at the edge [4]. The photons can undergo several interactions in the detector before they are detected and that render the detector inefficient and so there is the need for its efficiency to be determined. The efficiency can be classed into two as absolute and intrinsic efficiencies and they are defined as Absolute efficiency ÃŽ µabs = Number of pulses recorded [3] Number of radiation quanta emitted by source Intrinsic efficiency ÃŽ µint = Number of pulses recorded [3] Number of radiation quanta incident on detector These efficiencies are related by ÃŽ µint = ÃŽ µabs * (4à ¯Ã¢â€š ¬Ã¢â‚¬  /à ¢Ã¢â‚¬Å¾Ã‚ ¦) [3] where à ¢Ã¢â‚¬Å¾Ã‚ ¦ is the solid angle of the between source and detector. The solid angle is dependent on the distance between source and detector (d) and the radius of the detector (r) and it is determined by the this equation, à ¢Ã¢â‚¬Å¾Ã‚ ¦ = 2à ¯Ã¢â€š ¬Ã¢â‚¬   1 d [3] √d2 + r2 To determine the efficiency of the coincidence system, the absolute efficiency for real and random coincidences were also determined for both sources based on the equations below. ÃŽ µabs for real coincidences for 22Na = ÃŽ µabs * ÃŽ µint ÃŽ µabs for random coincidences for 22Na = (ÃŽ µabs)2 * Activity * Intensity * Time ÃŽ µabs for real coincidences for 60Co = ÃŽ µabs * ÃŽ µabs ÃŽ µabs for random coincidences for 60Co = (ÃŽ µabs)2 * Activity * Intensity * Time METHOD Two NaI detectors coupled with photomultipliers with high voltages and preamplifiers were used for this experiment. The inputs were connected to spectroscopic and SCA amplifiers. Detector 1 was first corrected for background by counting for 5 minutes. The 22Na gamma ray source was varied with distance and the absolute efficiency of the detector was determined as a result. Detector 2 was introduced and set at a distance of 10cm apart from Detector 1. 22Na was positioned in the middle and the counting was set to 5 minutes. The gate width and gate delay were varied and their spectrum observed. The experiment was repeated for the second gamma ray source, 60Co. The optimum gate delay was determined and varied with the gate width to obtain the optimum gate width. A linear graph of count rate against gate width was obtained that showed the real and random coincidences based on the slope gradient obtained. The percentage ratio of the random to real coincidences were determined and the uncertainty associated with the experiment was also determined. RESULTS/DISCUSSION The background spectrum was corrected in the count reading for both sources. The background radiation is as a result of scattered radiation associated with the experiment. The absolute efficiency of the detector was determined for both sources as shown in Figure 1 and Figure 2 and Table 1a 1b and Table 2a 2b for 22Na and 60Co respectively. The absolute efficiency was obtained using the formula Absolute efficiency = Sum of count Intensity x Activity Figure 1: Absolute efficiency as a function of the distance between the 22Na source and detector Figure 2: Absolute efficiency as a function of distance between the 60Co source and detector The 22Na revealed a gradual decrease in efficiency with increasing distance, whereas 60Co revealed a rapid drop in efficiency as a function of distance. 60Co revealed lower absolute efficiencies since the measure of the number of pulses obtained by the 60Co was less than the number of photons emitted by the gamma ray source. This could have been due to Compton scattering reducing the number of photons actually detected as a pulse. The 22Na however revealed quite high absolute efficiencies and so can be confirmed that the detector was efficient in detecting the 22Na than the 60Co. The intrinsic efficiency was determined using the equation below. ÃŽ µint = ÃŽ µabs * (4à ¯Ã¢â€š ¬Ã¢â‚¬  /à ¢Ã¢â‚¬Å¾Ã‚ ¦) The solid angle was determined for the detector when the distance between both detectors was varied between 5cm to 20cm and the radius of the detector was measured as 10cm. This is shown in Tables 3 and 4 and Figures 3 and 4 for 22Na and 60Co respectively. Figure 3: Intrinsic efficiency as a function of distance between the 22Na source and detector Figure 4: Intrinsic efficiency as a function of distance between the 60Co source and detector The intrinsic efficiency for 60Co was lower than 22Na. It can be deduced that the number of 60Co photons incident on the detector was more than the number of pulses recorded. Hence signifying that the detector was not efficient in detecting the 60Co. The 22Na however displayed high intrinsic efficiency almost approximating the maximum value for intrinsic efficiency. The intrinsic efficiency were found to be fluctuating with the highest being 0.9898 and 0.3872 with a solid angle of 1.3029 at 13cm distance from detector for 22Na and 60Co respectively. This is as result of the detector’s geometry detecting the photons at different solid angles. The solid angle determines how much of the photons can be detected as a function of distance. The overlap of the error bars signifies the uniformity of the errors. The probability of a 0.511MeV gamma travelling in the direction of the detector and being absorbed by it, will imply that the second 0.511MeV will also travel in the correct direction. Both detectors detecting the two 0.511MeV gammas can be determined to yield the absolute efficiency for real coincidences. This can be deduced from the notion that photons travelling in the right direction will be absorbed in the right direction by both detectors. The results of absolute efficiencies for real and random coincidences for 22Na and 60Co is shown in Table 5 6 and Figure 5, 6, 7 8. The efficiencies for both sources decreased with distance and it was lower for 60Co. The absolute efficiency for random coincidences was however for both sources than the absolute efficiency for real coincidences. It can thus be inferred that the absolute efficiencies for real coincidences for both 22Na and 60Co yields less probability of detection of real coincidence with 60Co as compared to the 22Na. The abso lute efficiencies for random coincidences was however comparable for both sources as the probability of detecting the second event within the gate width is possible for both sources. Figure 5: Absolute efficiency for real coincidences as a function of distance for 22Na Figure 6: Absolute efficiency for random coincidences as a function of distance for 22Na Figure 7: Absolute efficiency for real coincidences as a function of distance for 60Co Figure 8: Absolute efficiency for random coincidences as a function of distance for 60Co The gate delay was varied with gate width to obtain the optimum values of delay and width. The optimum gate delay was obtained as 1.2 µsec and 0.2 µsec for both 22Na and 60Co respectively and was used for the experiment. A linear graph of count rate as a function of gate width was obtained and a fixed gate width was obtained as shown in Figure 5 and 6 and table 7 and 8 Figure 5: A linear graph of count rate as a function of gate width applying a 1.2 µsec gate delay for 22Na Figure 6: A linear graph of count rate as a function of gate width by applying a 0.2 µsec gate delay for 60Co Real coincidences occur on the intercept of the linear slope gradient, whereas random coincidences can be found with the slope. For 22Na the optimum gate width obtained was 5 µsec. The graph of count rate as a function of gate width yielded a slope gradient of y = 5.019x + 200.15. By applying the optimum gate width and correcting for the gate delay, the real and random coincidences were determined using the LINEST function. The real coincidences was found to be 200  ± 2.3 whereas the random coincidences was found to be 25.1  ± 3.4. The percentage thus of random to real coincidences obtained in this experiment was 12.54  ± 1.85 %. This gives the value of pure coincidences that are not dependent on gate width. For 60Co, the optimum gate width was 5 µsec. The graph of count rate as a function of gate width yielded a slope gradient of y = 2.6801x + 76.483. When the optimum gate width was applied whilst correcting for the minute gate delay, the real and random coincidences were determined using the LINEST function. The real coincidences was found to be 76.5  ± 1.7 whereas the random coincidences was found to be 13.4  ± 2.6. The percentage of random to real coincidences obtained in this experiment was 17.52  ± 3.81 %. The above results was compared with the measured values obtained from the graph. The intercept gave the real coincidences as 200.15 and 76.48 for 22Na and 60Co respectively. The point of data convergence on the straight line gave the optimum gate width and the count equivalent was found as 225.28 and 90.02 for 22Na and 60Co respectively. The difference between this value and the real coincidences yielded the random coincidences as 25.13 and 13.56 in 22Na and 60Co respectively. Hence the percentage ratio of the random and real coincidences was obtained as 12.49% and 17.73%. This is equivalent to the values obtained from the calculated coincidences with the differences being due to uncertainties. The uncertainties with this experiment were with the NaI detector which contributed to scatter around the cover. The count rates resulted in some uncertainties as well and has been sown in table 8 for both detectors. The solid angle presented an uncertainty as the measurements for the detector could incur a large margin of errors. From all the results synthesized for both sources it could be gathered that the 22Na was an efficient source for coincidence counting compared to the 60Co. This is as a result of the geometry of the detectors as the Co system does not show a coincidence system and so there is more likelihood of a random coincidence than a real coincidence as compared to the Na system. This concludes that the 22Na will be efficient in a PET system, hence the reason for positron emitting radioisotopes being used in the PET system to ensure the maximum number of coincidences are being detected CONCLUSION The experiment was performed to examine the coincidence counting in two gamma ray sources and to determine the real and random coincidences as a function of gate width. The optimum gate width obtained was 5 µsec for both sources with gate delays of 1.2 µsec and 0.2 µsec for 22Na and 60Co respectively. The real coincidences for 22Na and 60Co were found to be 200.1  ± 2.3 and 76.5  ± 1.7 respectively. The random coincidences obtained were 25.1  ± 3.4 and 13.4  ± 2.6 for 22Na and 60Co respectively. This was determined by using the LINEST function. The measured count rates was also determined from the graph and resulted in real coincidences for 22Na and 60Co respectively as 200.15 and 76. 48 and random coincidences of 25.13 and 13.56. The percentage thus of random to real coincidences obtained in this experiment was 12.54  ± 1.85 % and 17.52  ± 3.81 % for 22Na and 60Co respectively. This gave the quality of the uncertainty in the coincidence system. It was deduced that the uncertainties in determining a random was higher in 60Co than in 22Na hence the Na system is more efficient for coincidence counting and very useful in the PET system. REFERENCES [1] The detection of bone metastases in patients with high-risk prostate cancer:99mTc-MDP planar bone scintigraphy, single- and multi-field-of-view SPECT,18F-fluoride PET, and18F-fluoride PET/CT.Even-Sapir et al, J Nucl Med(2006)47:287–97 [2] The Physics of Medical Imaging, ed. S. Webb. IoP publishing [3] Radiation and Detection Measurement, Glen N Knoll, 3rd Edition [4] Coincidence Counting, E. K. A. Advanced Physics Laboratory, Physics 3081, 4051 APPENDIXES Table 1a: Counts rate as a function of distance between source and detector for 22Na Table 1b: Absolute efficiency as a function of distance between source and detector for 22Na Table 2a: Counts rate as a function of distance between source and detector for 60Co Table 2b: Absolute efficiency as a function of distance between source and detector for 60Co Table 3: Intrinsic efficiency as a function of distance between source and detector of 22Na Table 4: Intrinsic efficiency as a function of distance between source and detector for 60Co Table 5: ÃŽ µabs for real and random coincidences as a function of distance for 22Na Distance(cm) ÃŽ µabs à ¢Ã¢â‚¬Å¾Ã‚ ¦ 4à ¯Ã¢â€š ¬Ã¢â‚¬   ÃŽ µint ÃŽ µabs for real coincidences ÃŽ µabs for random coincidences 5 0.09940 3.473 12.57 0.35967 0.0994 48.7255 10 0.05091 1.8403 12.57 0.347637 0.0509 12.8015 13 0.04015 1.3029

Communicating Anywhere, Anytime with Tablet Computing Essay -- Technol

6.4 The application of artwork in tablet computing The IPad art is created using the Brushes application which is drawn with the finger or a special pen. After that, IPad also released SketchBook Pro application,this application become top ranking artists’ application bar none. Autodesk reports that 10000 download in the first five days. The SketchBook Pro application has more brushes and tool options, and new â€Å"big screen† features or easy tool selection, drawing and editing. This application is draw with finger-controlled brushes or uses the optional Pogo stylus. The features of Brushes are high-quality brushes (with an erase mode), up to 6 layers (768x1024): reorder, merge, and adjust transparency, desktop-class colour picker, eyedropper tool, in-application replay of your paintings, Layer Blend Modes: normal, multiply, screen, overlay, and colour, eyedropper tool, extremely responsive zooming from 50% to 3200%, high resolution export with Brushes Viewer on Mac OS X, import photos to your canvas, generous level of undo and redo, in-app replay of your paintings, upload your paintings directly to Flickr . While the features of Sketchbook Pro are canvas size: 1024x768, two finger pan and zoom navigation with 2500% zoom, three finger tap for controls, three finger swipe gestures for quick access, flood fill and smear tool, draw styles for creating brush settings for each brush, synthetic pressure sensitivity, 75 preset brushes, including pencils pens, marker, natural media and photo brushes, 10 level of undo and redo,6 layers allowing ease of editing and control, import layers from Photo library, export to Photo Library, e-mail images, export as layer PSD file, eye-dropped colour selection, eye-dropper colour selection, eye-drop... ...port. The application of watercolour is named Auryn lnc. This application is pretty real watercolour experience for iPad. The Art Range has some great watercolour options but it may want to check out Auryn Ink. This is due to this application manipulate the precise amount of water on brush and on the paper. Works Cited http://www.telegraph.co.uk/technology/picture-galleries/7926157/Apple-iPad-art-paintings-created-using-Brushes-ArtStudio-and-Sketchbook-Pro-apps.html http://blogs.computerworld.com/16776/six_reasons_ipad_is_a_productivity_tool http://www.openculture.com/2010/11/david_hockneys_ipad_art_goes_on_display.html http://www.appcraver.com/drawing-apps-ipad-art/ David Hockner (2009) http://www.physorg.com/news/2011-09-british-painter-hockney-reveals-ipad.html http://todayinart.com/2010/04/16/drawing-on-the-ipad-a-brushes-sketchbook-pro-walkthrough/

A Bintel Brief †Jewish Daily Forward Essay

The Bintel Brief is a column in the Jewish Daily Forward, which was formed in 1906. During this time many Jewish immigrants have suffered a great deal of depression and anxiety because of being Jewish. Often separated from family and bewildered by life in a new country, thousands of Jewish immigrants wrote to the offices of the Jewish Daily Forward. Nothing like existed in the homeland. It seemed so American, so up-to-date, and so very needed. It was an advice column for the new Jewish immigrants, to help them with their new lives. It was called the â€Å"Bintel Brief†, Yiddish language for â€Å"Bundle of Letters. † The paper’s founder and editor was Abraham Cahan (1860-1951). Cahan formed the Bintel Brief to listen to the many Jewish immigrants from Russia, Hungary, Poland, Romania, and Middle East as they live life through hardships at the turn of the century and speak of issues through the experiences of the immigrants. Cahan would answer back with practical and sometimes very wise advice. His intended audience was mainly the immigrants of New York City. Cahan’s commitment to social realism makes his work a valuable source for insight into ways in which immigrants perceived their situation. The Jewish Daily Forward did its part to bring familiarity and bring comfort to the Jewish immigrants, to give advice, to aid those in need, and to bring together the Jewish community in America. The main detectable bias in the source is that the immigrants were lonely and needed something to turn to. Abraham Cahan founded the Jewish Daily Forward and served as the editor until his death in 1951. The major tensions of immigrant life that were revealed in the letters were the cries of help from the very poor, problems dealing with religion and discrimination, people dealing with job decisions. All the problems in the Bintel Brief are difficulties faced by immigrants and the consequences that they must face because of being who they are. Mothers were known to find their lost children through the Bintel Brief and many people lost their spouses due to discrimination. The Bintel Brief was there for any Jew to turn to if they needed it. Cahan’s responses were in likely for the Jewish immigrants. These people needed someone to discuss their problems with. Cahan’s advice given was to improve the depression and hardships the person was having. Thousands of readers wrote to the editor, asking for help with a host of issues created by their effort to blend the customs and rituals of the old world with the practices and pressures of the new. In conclusion, his advice given in the Bintel Brief is similar to the advice in columns of today such as â€Å"Dear Abby† and daytime talk shows. His advice given today is always for the good of the people.

Cultural Component

Valduron Cleare English 119 18th October, 2011 Cultural Component The components of culture are: the attitudes, beliefs, customs, traditions, art, clothing, food, language and achievements of society that are passed on to each generation. With that explanation I’ve realized that culture is in almost every aspect of our lives. I experienced at least four of these components during my recent trips to Arawak key. Firstly, as a tradition for most Bahamian birthday celebrations, the main goal is to eat more than you regularly do, and we did just that. Our party consisted of my Father and mother, my two older brothers and me.After all of the congratulations on seeing another year on this earth were done, we set out to our destination. Usually we just order pizza and call it a day but we wanted to make this day special. Our place of choice was the great Arawak Key, or as I like to call it, food central. As we arrived there was rake n’ scrape music playing and people dancing. I t was also obvious that we weren’t the only ones with that idea. Hungry faces as far as the eye can see, but no one was as hungry as me. I searched all around for an empty restaurant to seat me family of five.It felt like it was hopeless because every restaurant we looked in, a full house of hungry faces looked back at us. We finally found a diamond in the rough with a slightly empty restaurant. This restaurant had a cozy feel to it. It had basic light brown paint and Bahamian art strung up on the walls. These paintings were probably purchase from schools which made me wish I did better in art. As we ordered our food another component of culture came to me. The menu was stacked with Bahamian dishes, from the almighty conch snack to the luxurious lobster and shrimp snacks.I ordered two different meals for myself only and when I was finished, I still wasn’t full. Secondly, I went to an event known as Fam Fest. This is a free gospel concert held annually on Arawak key. Th is brings up another cultural component which is beliefs. The majority of the Bahamas is of the Christian denomination. This was seen excellently with the numbers of people that showed up. Although it could have been due only to the fact that it was free, because something that is free and a Bahamian is never far apart. Getting back to topic, with a gathering of Bahamians there has to be food.The entire right sight of the venue was covered by vendors set upped to sell their dishes. Hundreds of people gathered to praise the lord and satisfy their stomachs, not a bad combination. Arawak key is a Bahamian culture haven. From the food, the music, and the dancing, it all is truly a culture filled place. Also the clothes worn by employees to accentuate their restaurant’s Bahamian qualities are brilliant. Firstly, the food is pure Bahamian influenced. The sound of conch salad being prepared fills the air and the smell of fried foods just flow through your nostrils.Furthermore, the r ake n’ scrape music played by live bands or speakers just set the mood and make for the perfect Bahamian experience. Also, the dancing, although mostly done by drunken men and women, still gives a nice feel to the place. In conclusion, it is clear to say that the components of culture, or just culture itself is evident almost everywhere you go. Arawak Key is a perfect place to go if you want a true culture experience. Although some of the components are seen more than others, each of them plays a vital role in the complete culture of the Bahamas.