2s space emotions v2

Emoticon Adalah Bentuk emosional dalam bentuk icon dimana biasanya digunakan dalam text chat, Artikel Blo atau website, kiriman e-mail ataupun SMS.Emoticon biasanya digunakan dalam penggambaran kondisi ekspresi seseorang pada waktu itu. Atau agar kiriman teks terlihat lebih keren.Mau koleksi Emoticon super cantik dan super keren? Tepat, silakan anda download demoticonnya di bawah ini.Downloadnya gratis kok, gak pake beli. Gak Pake lama.. 2s-Space Emoticons v1.0 | Download20 ico, png and gif files for free download.2s-Space Emotions v2.0 | DownloadPNG files 256×256 (px) size and 20 ico files Blueticons | DownloadTextThe Blacy | DownloadThe Blacy shows the world’s worst simles to you. PNG + ICO files.128X128 (px) size. Emoji | DownloadZip-File contains = 18 PNG Files 200×200 and 18 PNG Files 100×100. Emix 1 Emoticons Pack | Download12 emoticons (12 – 100*100 px, and 12 – MSN smileyEmoticons Pack | DownloadSWF download for cute emoticons, sexy girl emoticons, BebeDemon emoticons, CHampignon Mignon emoticons and Gothique Girl emoticons. Emoticons from ICQ4 | DownloadEmoticons from ICQ4 for Trillian 3.xx (works on Trillian 2.xx too) Expressions Yummies | DownloadThis kind of expressions are quite useful in Japanese manga. Different eyebrown’s shape, the mouth and eye’s size, etc combines a different expressions. Emoticons | DownloadA Zip file with each one as a 25 x 25 and 50 x 50 and 100 x 100 gif Emoticons :: 001 | DownloadThese emoticons work best on dark backgrounds. Onion Head Emoticons | DownloadOnion Head emoticons are images used for expressing Onion Head emotions in a virtual environment.POPO Emotions Full Version | DownloadPOPO emotions + addon version icon pack. ICO and PNG files Parampaa Emoticons | DownloadThis Pack contains 32 weird emoticons.Monkey Emoticons Set | DownloadFREE! All of Monkey Emoticons and other cute icons for your forums & webboard. IconTexto Emoticons | DownloadDownload this free Windows Vista icon pack for

Mindset. They both need plenty of space and cherish their moments of solitude. That’s why they are such a good match! Neither will complain to the other about their extended absences nor will they get into each other’s business. Although each has opposing agendas and their need for freedom comes from different reasons, they respect each other. Besides, they both have exciting personalities and can spend hours talking about their life experiences and perspectives.And concerning life path 9, these two numbers share the exact search for the metaphysical meaning of life. They are both spiritual, and this relationship brings peace and harmony to life path 7. They also respect each other’s personal space and don’t feel insulted or hurt by the lack of attention.Life path 2 are compassionate and dependent and don’t get along with the hermit-like attitude of their 7 partners. 2s value family and affection and struggle with life path 7’s negative comments and detached demeanor. Before long, the relationship wears thin as 7s get fed up with 2s constant demands, and 2s grow tired of begging for attention all day long.Something similar happens with the union of life paths 7 and 6. Life paths 6s are firmly committed and drive by their emotions. These numbers care for relationships and cherish every minute spend with their loved ones, while life paths 7s are secretive and loners. Life path 6 individuals demand physical contact and intimacy, and life path 7s require space and distance, something 6s can’t provide.And life

R L sinT . We can also revolve the string in such away that the string moves along the surface of If T is the period of revolution of the bob,a right circular cone of vertical axis and thepoint object performs a (practically) uniform Z 2S ghorizontal circular motion. In such a case the T L cosTsystem is called a conical pendulum. ? Period T 2S L cosT --- (1.7) Fig. 1.9 (a): In an inertial frame g Frequency of revolution, n 1 1 g --- (1.8) T 2S L cosT In the frame of reference attached to the bob, the centrifugal force should balance the resultant of all the real forces (which we call CPF) for the bob to be at rest. ∴ T0 sinθ = mrω 2 --- (in magnitude). This is the same as the Eq. (1.5) Do you know? (i) For a given set up, L and g are constant. Thus, both period and frequencyFig. 1.9 (b): In a non- inertial frame depend upon θ .Figure 1.9 shows the vertical section of (ii) During revolutions, the string cana conical pendulum having bob (point mass) NEVER become horizontal. This canof mass m and string of length L. In a given be explained in two different ways.position B, the forces acting on the bob are (i) (a) If the string becomes horizontal, the force due to tension will also beits weight mg directed vertically downwards horizontal. Its vertical component willand (ii) the force T0 due to the tension in the then be zero. In this case, nothing willstring, directed along the string, towards be there to balance mg.the support A. As the motion of the bob is a (b) For horizontal string, i = 90°. This willhorizontal circular motion, the resultant force indicate the frequency to be infinitemust be horizontal and directed towards the and the period to be zero, which arecentre C of the circular motion. For this, all impossible. Also, in this case, the tension mgthe vertical forces must cancel. Hence, we T0 cosT in the string and the kineticshall resolve the force T due to the tension. energy 1 mv2 1 mr 2Z 2 of the bob 0 2 2If θ is the angle made by the string with thevertical, at any position (semi-vertical angle will be infinite.of the cone), the vertical component T0 cos Activityθ balances the weight mg. The horizontal A stone is tied to a string and whirledcomponent T0 sinθ then becomes the resultant such that the stone performs horizontalforce which is centripetal. circular motion. It can be seen that the string is NEVER horizontal.?T0 sinT centripetal force mrZ2 --- (1.5)Also, T0 cosθ = mg --- (1.6)Dividing eq (1.5) by Eq. (1.6), we get, 8Example 1.4: A merry-go-round usually Solution: N sinT mg and N cosT mv 2consists of a central vertical pillar. At the rtop of it there are horizontal rods which can rg v2 tanTrotate about vertical axis. At the end of this ? tanT v2 ? r ghorizontal rod

WithtHheenacbes,eanncgeuolaf rexmteormnaelnutunmbal Laniscecdontosreqruveedτi.n what frequency will the remaining balloon revolve now? Neglect all non-conservative forces. m1 V1 § R1 ·3 1 Solution: m2 V2 ¨ R2 ¸This is the principle of conservation of angular © ¹ ? R1 § m1 ·3 R2 ¨ m2 ¸momentum, analogous to the conservation of © ¹linear momentum. 18Also, m1 100 100 1 Accordingly, the object possesses two m2 100 48.8 51.2 0.512 types of kinetic energies, rotational and translational. Sum of these two is its total 1 kinetic energy. § m1 ·3 1 1.25 Consider an object of moment of inertia ?¨ m2 ¸ 0.8 ¹ I, rolling uniformly. Following quantities can=n1 © 6=0 rpm 1rps, n2 = ? be related.Being sphere, moment of inertia v = Linear speed of the centre of mass ·2 5 R = Radius of the body ¸ I 2 mR 2 ? I1 § m1 ·§ R1 ¹ § m1 ·3 Z Angular speed of rotation of the body 5 I2 ¨ m2 ¸¨ R2 ¨ m2 ¸ © ¹© © ¹ ?Z v for any particle RAccording to principle of conservation ofangular momentum, I1Z1 I2Z2 M = Mass of the body 5 K = Radius of gyration of the body ? I MK 2? I1 2S n1 I2 2S n2 ? n2 § I1 · n1 § m1 ·3 Total kinetic energy of rolling = Translational ¨ I2 ¸ ¨ m2 ¸ © ¹ © ¹ K.E. + Rotational K.E. n1 1.25 5 u1 3.052 rps ?E 1 Mv 2 1 IZ 2 2 2Example 1.9: A ceiling fan having momentof inertia 2 kg-m2 attains its maximum 1Mv 2 1 MK 2 § v ·2frequency of 60 rpm in ‘2π’ seconds. 2 ¨© R ¸¹Calculate its power rating. 2Solution: 1 Mv 2 ¨§ 1 K2 · --- (1.18) 2 © R2 ¸Z0 0, Z 2S n 2S u 2 4S rad / s ¹ It must be remembered that static friction Z Z0 4S 0 2 rad/s2D t 2S is essential for a purely rolling motion. In this? P W ˜Z ID ˜Z 2u 2u 4S case, it prevents the sliding motion. You might 16S watt # 50 watt have noticed that many a times while rolling down, the motion is initially a purely rolling1.11 Rolling Motion: motion that later on turns out to be a sliding The objects like a cylinder, sphere, motion. Similarly, if you push a sphere-likewheels, etc. are quite often seen to performrolling motion. In the case of pure rolling, object along a horizontal surface, initially ittwo motions are undertaking simultaneously;circular motion and linear motion. Individual slips for some distance and then starts rolling.motion of the particles (except the one at thecentre of mass) is too difficult to describe. 1.11.1 Linear Acceleration and Speed WhileHowever, for theory considerations we canconsider the actual motion to be the result of Pure Rolling Down an Inclined Plane:(i) circular motion of the body as a whole,about its own symmetric axis and Figure 1.18 shows a rigid object

German in full: Vergeltungswaffen-2 (“Vengeance Weapon 2”) Also called: V-2 missile or A-4 V-2 rocket, German ballistic missile of World War II, the forerunner of modern space rockets and long-range missiles.Developed in Germany from 1936 through the efforts of scientists led by Wernher von Braun, it was first successfully launched on October 3, 1942, and was fired against Paris on September 6, 1944. Two days later the first of more than 1,100 V-2s was fired against Great Britain (the last on March 27, 1945). Belgium was also heavily bombarded. About 5,000 people died in V-2 attacks, and it is estimated that at least 10,000 prisoners from the Mittelbau-Dora concentration camp died when used as forced labour in building V-2s at the underground Mittelwerk factory. After the war, both the United States and the Soviet Union captured large numbers of V-2s and used them in research that led to the development of their missile and space exploration programs.The V-2 was 14 metres (47 feet) long, weighed 12,700–13,200 kg (28,000–29,000 pounds) at launching, and developed about 60,000 pounds of thrust, burning alcohol and liquid oxygen. The payload was about 725 kg (1,600 pounds) of high explosive, horizontal range was about 320 km (200 miles), and the peak altitude usually reached was roughly 80 km (50 miles). However, on June 20, 1944, a V-2 reached an altitude of 175 km (109 miles), making it the first rocket to reach space. See also rockets and missile systems: The V-2. For contemporary accounts of V-2 bombings of London as recorded in the Britannica Book of the Year, see BTW: London Classics: London in World War II. More From Britannica rocket and missile system: The V-2 The Editors of Encyclopaedia BritannicaThis article was most recently revised and updated by Erik Gregersen.