Saturday, December 28, 2019

The Discourse Community Of The English Subject - 2328 Words

What is a discourse community in the English subject? A discourse community is a group of people or communicators who share the same common goals or interests and use different forms of communication to achieve these goals. Some of these forms of communication may range from reading, writing, the use of technology such as blogging and emailing, and even visual art such as painting and drawing. As an English major focusing on the aspect of creative writing, the discourse community I so happened to be associated with is of the English subject. The discourse community of the English literature is made up of many people, genres of literature, and even terms. The discourse community of English literature can be traced back to as early as the year C.658 with the development of Anglo-Saxon literature. Some influential eras of English literature include : Romanticism, Victorian literature, Medieval Theater, Poetry, and the Elizabethan Period. Of course with every discourse community there are a vast number of people who help to make it up. In the discourse community of English some of these people include author and playwright William Shakespeare, author Mark Twain, author and poet Jane Austen , and a slew of famous African-American authors some including Toni Morrison, Alice Walker, Lorraine Hansberry, and poet Maya Angelou. African American Literature: Urban Fiction The aspect of the English discourse community I will be focusing on in my report is Urban Fiction.Show MoreRelatedAnalysis Of John Swales s Work On Genre Analysis953 Words   |  4 PagesBest known for his work on genre analysis, John Swales, a linguist, has been greatly influential on academic English. His work on discourse communities has helped to greatly define and analyze the way in which unique communities may operate and exchange information. 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Thursday, December 19, 2019

Managing A Global Business With Offices - 2147 Words

Introduction Managing a global business with offices in several countries requires excellent cross cultural management skills. The technological development of laptops, mobile phones and internet accessibility has made it near impossible to only interact with people from one culture; in fact it allows many to do business in various areas of the globe, interact and communicate with managers and employees in international offices, and develop a relationship with others through several behavioural etiquette recommendations. The topic of culture has been widely discussed in a variety of instances, and the idea of developing a ‘cultural identity’ for either an individual or a business can be a scary thought, however if accurate research into other cultures and behaviours is completed, organisations and employees should be able to develop empathy and self-confidence. The term ‘culture’ has been defined time and time again and has been vastly overused; however a solid definitio n has been created by Geert Hofstede, â€Å"Culture is the collective programming of the mind distinguishing the members of one group or category of people from others†. (Pieper, 1990) Working in teams of international origin can be rather difficult. The concept of a ‘team’ is usually defined as a number of people working together to achieve a common purpose and be jointly responsible for the work they do, including those working both inside and outside the organisation. (Browaeys et al 2011) DevelopingShow MoreRelatedManaging A Global Business With Offices1681 Words   |  7 PagesTopic 1 : Managing a global business with offices in several countries Introduction Excellent cross-cultural skills are relevant in managing businesses with offices in different countries. 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Wednesday, December 11, 2019

Tourism Management Communication Plan

Question: Discuss about theTourism Managementfor Communication Plan. Answer: Communication plan is an integral part of the marketing strategy of the organizations. The companies use proper communication strategy to enhance their position in the marketplace. Similarly, Hobbiton can align its key operators to attract the target visitors to the movie sets, so that the profits of the company can increase (100% Pure New Zealand, 2017). In this regard, it is proposed that the organization can make strategic alliance with different stakeholders. Partnering with Other Operators Whakarewarewa- The living Maori Village Whakarewarewa, a town in the central Rotorua is famous for its traditional Maori culture. It is the oldest cultural heritage for the organization and popular for showcasing the Maori culture to the tourists. In this location, the tourists are allowed with the guides wherein they experience the authentic Maori culture and tradition. They are able to view the geothermal wonders with their eyes and learn about the history of Whakarewareha. Whakarewarewa is selected as a potential tourism partner for Hobbiton as a large number of tourists come to experience and participate in the Maori cultural activities (Whakarewarewa, 2017). If Whakarewarewa collaborates with Hobbiton, it will increase the customer inflow to the movie set. Another reason for the selection of Whakarewarewa is that both the tourist destinations complement each other. Both the tourist destinations are popular among the international and domestic tourists and the tourist can experience two different tourist destinations at the same time. In the communication plan, the management should focus on providing discounts to the tourists who buy tickets for both the organizations. Collaboration with the Media The New Zealand tourism ministry has implemented a successful program to present New Zealand as an attractive international tourism destination. The International Media Programme (IMP) regularly hosts around 150 to 400 programs from print, online and broadcasting organizations which are posted on the website of the organization (Tourism New Zealand, 2017). Hobbiton can collaborate with the New Zealand tourism Ministry by so that they can arrange tourism events at the location of Movie set. The tourists and the media will be made aware of the story angle of Hobbiton movie set. It should also focus on the original set and how it was rebuilt in the later years. In the communication plan, the company can follow the strategy of offering Media Pass for the international tourists and media agency. It will assist them in exploring New Zealand as an attractive tourism location. It can also collaborate independently with the media to increase the inflow of the tourists. It can use variety of communication mediums such as television or newspaper advertisements to attract a large number of people. Moreover, it can also use the social media strategy to engage international tourists. The social media has a wide outreach and cheap method of attracting target customers. It can also be used to instantly connect with the target customers (Parente Strausbaugh-Hutchinson, 2014). References 100% Pure New Zealand. (2017). Hobbiton Movie Set Tours. Retrieved on 30 April 2017 from https://www.newzealand.com/in/plan/business/hobbiton-movie-set-tours/ Parente, D., Strausbaugh-Hutchinson, K. (2014). Advertising Campaign Strategy: A Guide to Marketing Communication Plans. Cengage Learning. Tourism New Zealand. (2017). What we do. Retrieved on 30 April 2017 from https://www.tourismnewzealand.com/about/what-we-do/campaign-and-activity/ Whakarewarewa. (2017). Visit Whakarewarewa, The Living M?ori Village. Retrieved on 30 April 2017 from https://www.whakarewarewa.com/

Wednesday, December 4, 2019

Leung Hoi Ning (14) Class 6S Group No. 8 Date of experiment 9-12-03 Essay Example

Leung Hoi Ning (14) Class: 6S Group No.: 8 Date of experiment: 9-12-03 Essay Objective We are studying the simple harmonic motion of a pendulum by attaching a ticker-tape to the bob and analyzing the dots marked on the tape.Experimental Design- Apparatus: 0.5 kg ringed mass1.5 m length of stringTicker-tape timerTicker-tapeLow voltage power supply (a.c.)Retort stand and clamp- Procedure for getting the ticker-tape1. A string with 1.5 m long was measured and tied with the 0.5 kg ringed mass2. Set the pendulum as shown in figure 1Figure 13. The ticker-tape timer was connected to the low voltage power supple (a.c.)4. The retort clamp was used to hold the clamp tightly so it would not vibrate when the mass was swinging.5. A 30cm ticker-tape was attached to the ringed mass6. The 0.5 kg ringed mass was pulled to one side with amplitude of 13cm from the equilibrium position.7. The power supply and the ticker-tape timer were switched on.8. The 0.5 kg ringed mass was allowed to swing to the other side after a few dots were stroke on the same place of the ticker-tape.9. The ticker-tape timer was switched off when the 0.5 kg ringed mass began to swing back to the equilibrium position.10. Step (3) to step(7) were repeated until 5 more ticker-tapes were got.- Procedures for plotting graphs1. The dots marked on the tape were examined.2. The tape, which the dots were perfectly stroke, was chosen.3. The two most widely spaced dots were marked on the tape. This gives the zero position (equilibrium position) of the pendulum bob.4. Every third dot from the zero position on the tape was marked. The displacement of these points from the zero position was measured and the corresponding time was worked out. Time interval between successful dots = 0.02 second.5. These data was plotted on a displacement-time graph (on Page 3 ).6. The velocity was worked out from the slopes of the curve in the displacement-time graph.The velocity-time graph was plotted (on Page 4 ).7. The acceleration was worked out from the slopes of curve in the velocity-time graph. The corresp onding displacement was found. The displacement-acceleration graph and the acceleration-time graph were plotted (on Page 5 and 6 ).Result:Displaccement x/cm11.610.48.86.54.60-2.9-5.9-8.3-10.2-11.7-12.4Time t/s0.10.20.30.40.50.60.70.80.91.01.11.2Velocity v/ cm/s-1.15-2-2.3-2.6-3.3-3.7-2.8-2.5-2.3-1.45-0.8-0.55Time t/s0.10.20.30.40.50.60.70.80.91.01.11.2Acceleration a/ cm/sà ¯Ã‚ ¿Ã‚ ½-1.55-1.43-1.25-0.95-0.6500.40.81.151.451.651.75Displaccement x/m0.1160.1040.0880.0650.0460-0.029-0.059-0.083-0.102-0.117-0.124Acceleration a/ cm/sà ¯Ã‚ ¿Ã‚ ½-1.55-1.43-1.25-0.95-0.6500.40.81.151.451.651.75Time t/s0.10.20.30.40.50.60.70.80.91.01.11.2Data evaluation:From the displacement-time graph, the curve is a half cycled cosine curve. The curve in the velocity-time graph is a negative, half-cycled sine curve. The curve in the acceleration-time graph is a negative, half-cycled cosine curve. From the acceleration-displacement graph, a straight line was shown, which the acceleration is always in the op posite direction and is directly proportional to the displacement. So we can use the following equation to represent the motion:a = -w à ¯Ã‚ ¿Ã‚ ½ x(where a is the acceleration, w is the angular velocity ( a positive constant ), x is the displacement)The definition of simple harmonic motion (S.H.M.) is:1. the acceleration of a particle is* directed towards a fixed point* directly proportional to its distance from that poing2. the acceleration is always in the opposite direction to the displacementSo, the equation a = -wà ¯Ã‚ ¿Ã‚ ½x proved that the pendulum performed S.H.M.Also, for a S.H.M. the angular velocity (w) is kept constant. Period (T) is equal to 2?/w, so the period is also kept constant and is independent of amplitude and mass of the bob.From the graphs the value of w is more or less the same within the motion.time0.10.20.30.40.50.60.70.80.91.01.11.2w0.0070.010.010.010.020.020.020.020.020.020.010.03As period (T) = 2? / wSo the period is also more or less the same within the motion.DiscussionBackground information of simple harmonic motion.There is a close connection between circular motion and simple harmonic motion. Consider an object experiencing uniform circular motion, such as a mass sitting on the edge of a rotating turntable. This is two-dimensional motion, and the x and y position of the object at any time can be found by applying the equations:The motion is uniform circular motion, meaning that the angular velocity is constant, and the angular displacement is related to the angular velocity by the equation:Plugging this in to the x and y positions makes it clear that these are the equations giving the coordinates of the object at any point in time, assuming the object was at the position x = r on the x-axis at time = 0:How does this relate to simple harmonic motion? An object experiencing simple harmonic motion is traveling in one dimension, and its one-dimensional motion is given by an equation of the formThe amplitude is simply the maximu m displacement of the object from the equilibrium position.So, in other words, the same equation applies to the position of an object experiencing simple harmonic motion and one dimension of the position of an object experiencing uniform circular motion. Note that the In the SHM displacement equation is known as the angular frequency. It is related to the frequency (f) of the motion, and inversely related to the period (T):The frequency is how many oscillations there are per second, having units of hertz (Hz); the period is how long it takes to make one oscillation.Velocity in SHMIn simple harmonic motion, the velocity constantly changes, oscillating just as the displacement does. When the displacement is maximum, however, the velocity is zero; when the displacement is zero, the velocity is maximum. It turns out that the velocity is given by:Acceleration in SHMThe acceleration also oscillates in simple harmonic motion. If you consider a mass on a spring, when the displacement is zer o the acceleration is also zero, because the spring applies no force. When the displacement is maximum, the acceleration is maximum, because the spring applies maximum force; the force applied by the spring is in the opposite direction as the displacement. The acceleration is given by:Note that the equation for acceleration is similar to the equation for displacement. The acceleration can in fact be written as:All of the equations above, for displacement, velocity, and acceleration as a function of time, apply to any system undergoing simple harmonic motion. What distinguishes one system from another is what determines the frequency of the motionWe choose a 1.5 m long string and the amplitude to be 13 cm because we need to ensure the swing angle is less than 5 à ¯Ã‚ ¿Ã‚ ½. The restoring force F = ma = mgsin?, which always tends to bring the object back to the original (zero) position.For very small ?,?S.H.M.After studying the x-t, v-t, x-a and a-t graphs , I know more about the ph ase angle. The following figure shows three instant in the motion of a pendulum.At H, the acceleration a is maximum and positive. A quarter cycle later, at O, the velocity v is maximum and positive. Another quarter cycle later, the position x is maximum and positive at K. One cycle corresponds to an increase of 2? or 360à ¯Ã‚ ¿Ã‚ ½ for à ¯Ã‚ ¿Ã‚ ½. So a quarter cycle corresponds to 1/2 ? or 90à ¯Ã‚ ¿Ã‚ ½. Thus,- the acceleration leads the velocity by 1/2 ?- the velocity leads the position by 1/2 ?Conversely, the velocity lags the acceleration by 1/2 ?, and the position lags the velocity by 1/2 ?. The acceleration and position are out of phase by ?, i.e. they are in antiphase. These differnences in the value of à ¯Ã‚ ¿Ã‚ ½ are called phase difference.The velocity and acceleration of the bob, just like the displacement, can be described by rotating vectors of magnitude wA and wà ¯Ã‚ ¿Ã‚ ½A respectively. The relative phase relations, i.e. a leads v by 1/2? and v leads x by 1/2?, a re obvious from such a figure.At H At O At KThe new equations for displacement, velocity and acceleration are as follows:x = Acosà ¯Ã‚ ¿Ã‚ ½v = -wAsin(à ¯Ã‚ ¿Ã‚ ½ + 1/2 ? )a = -wà ¯Ã‚ ¿Ã‚ ½Acos(à ¯Ã‚ ¿Ã‚ ½ + ? )As a = -(g/l)xwà ¯Ã‚ ¿Ã‚ ½ = g/lw = (g/l)1/2T = 2? /wPeriod is not only dependent on the swing angle, but also the length of string, while the amplitude and mass do not affect the period. So it is isochronous.Error AnalysisIn this experiment, the errors mainly come from frictions, with air and within the string, as well as the friction between the ticker-tape and the chair. They act as a damping force and slow down the motion. So energy is lost continuously to overcome the fictions. This damping force is directly proportional but in opposite direction to the velocity of the bob. The damping force is equal to -bv where b is a positive constant and v is the velocity of the bob. Now the restoring force is no long equal to mgsinà ¯Ã‚ ¿Ã‚ ½. The new equation of restoring is ma = mgsinà ¯Ã‚ ¿Ã‚ ½ bv. The expression a = -(g/l)x is no longer be obtained. So the motion is not simple harmonic one anymore.The swing angle is difficult to keep under 5 à ¯Ã‚ ¿Ã‚ ½. So if an angle larger then 5 à ¯Ã‚ ¿Ã‚ ½ is used, the equationscannot be held and so the motion is not a simple harmonic one.When leave the ringed mass and let it to swing, we may give an external force to it. Also the mass oscillates horizontally during the swinging motion. These may affect the swing angle and the velocity of the bob and this explained why the dots on the v-t graph cannot connect together to form a smooth curve.Another big problem is to measure the slopes of the curves accurately. This explains why the dots in v-t, x-a and a-t graphs cannot connect together to form smooth curves and straight line.Improvements1. Hold the mass stationary for a while before leaving it. Try not to exert any force to the mass.2. Twist the clamp as tight as possible so the whole system will not vibrat e or oscillate.3. Set the ticker-tape timer at a place which cannot touch the chair, while keeping on the same horizontal plane with the mass.4. use a plane mirror to get the normal of the dots and then calculate the slopes of the dots.ConclusionsSimple pendulum is a kind of simple harmonic oscillator. The experimental results satisfied the equation for simple harmonic motion ( a = wx)