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Lines CM3 - CHINA MALAYSIA 3 SERVICE SOUTH BOUND PORT NAME ETB / ETD QINGDAO SHANGHAI 6/7 1/1 XIAMEN NANSHA 4/4 5/6 PORT KELANG WEST PORT 4/5 NORTH BOUND PORT NAME ETB / ETD PENANG 6/7 PORT KELANG WEST PORT PASIR GUDANG 1/2 3/4 SHEKOU HONG KONG 2/2 2/3 QINGDAO 6/7 RNV - NORTH CHINA-VIETNAM SERVICE PORT NAME ETB / ETD HO CHI MINH CITY 2/3 HONG KONG 6/6 SHEKOU DALIAN 7/7 5/5 TIANJIN 6/7 QINGDAO 1/2 CVM - CHINA VIETNAM MALAYSIA SERVICE PORT NAME ETB / ETD SINGAPORE 5/5 PORT KELANG WEST PORT 7/1 HAIPHONG 6/7 CVT - CHINA THAILAND SERVICE SOUTH BOUND PORT NAME ETB / ETD SHANGHAI 5/6 NINGBO 7/7 XIAMEN 2/2 SHEKOU 3/4 LAEM CHABANG 1/2 NORTH BOUND PORT NAME ETB / ETD BANGKOK 2/4 LAEM CHABANG 4/5 HONG KONG 2/2 SHANGHAI 5/6 PH5 - PHILIPPINE FEEDER 5 SOUTH BOUND PORT NAME ETB / ETD QINGDAO 6/7 SHANGHAI 1/2 NINGBO 3/4 KAOHSIUNG 5/5 MANILA SOUTH PORT 1/2 MANILA NORTH PORT 2/3 NINGBO(dischg only) 1/1 SHANGHAI(dischg only) 2/2 NORTH BOUND PORT NAME ETB / ETD NIX - CHINA INDIA EXPRESS SERVICE WEST BOUND PORT NAME ETB / ETD QINGDAO 1/2 SHANGHAI NINGBO 3/4 5/5 DA CHAN BAY 1/1 PORT KELANG WEST PORT 7/1 EAST BOUND PORT NAME ETB / ETD NHAVA SHEVA 2/3 MUNDRA 4/5 HAZIRA 6/7 COLOMBO 3/4 PORT KELANG WEST PORT 1/2 T.S.
24 (2004) 3227–3266 c World Scientific Publishing Company BOUND AND SCATTERING STATES OF ITINERANT CHARGE CARRIERS IN COMPLEX MAGNETIC MATERIALS A.
In-Depth Analysis of Delegate Binding for Ron Paul Delegates to the 2012 GOP National Convention Version 1, May 14, 2012 By Mark Laurence Donald Emerson, acting in his personal, non-corporate capacity as a Nevada citizen, and as a delegate at the recent Nevada State Republican Convention SacredCampaign@gmail.com The concept of “Delegate Binding” means delegates to Presidential National Conventions can be “bound” to vote for a particular candidate on the first ballot for a presidential nominee, even if that candidate is not their choice, and even if doing so is against their conscience.
CircaNorthwest Outward Bound School 50 Years Anniversary T his June, 50 years after the first Northwest Outward Bound course adventured into the Three Sisters Wilderness of Oregon, a group of the original founders and their families—plus dozens of other former instructors and students—gathered at the NWOBS bases in Mazama, Washington and Redmond, Oregon to celebrate the half century anniversary.
Mania ○○○○○ ○○○○○ □□□□□ □□□□□ □□□□□ □□□□□ □□□□□ ○○○○○ ○○○○○ ○○○○○ ○○○○○ ○○○○○ ○○○○○ □□□□□ □□□□□ □□□□□ Bound ► Pool ► MAX:
A relationship between the complexity of a landscape and the corresponding lower bound of the expectation will be calculated.
As such, we are bound by the triple lock system, which means that we adhere to the principles of transparent accounting, good governance and good fundraising.
Name Symbol Status Up Quark 𝘂 Down Quark Grouping Electric Charge (e) Intrinsic Angular Momentum Parity Statistics Further Detail Generation Confirmed Fermionic Quark 1 2/3 1/2 𝗱 Confirmed Fermionic Quark 1 -1/3 Charm Quark 𝗰 Confirmed Fermionic Quark 2 Strange Quark 𝘀 Confirmed Fermionic Quark Top Quark 𝘁 Confirmed Fermionic Bottom Quark 𝗯 Confirmed Electron 𝗲 Muon Rest Mass (eV/C2) Rest Energy (J) Lepton Number Electronic Lepton Number Muonic Lepton Number Tauonic Lepton Number Baryon Number Charm Strangeness Truth Beauty Colour Charge Matrices Isospin Third Component of Isospin (I3) Hypercharge R-Parity (B-L) Weak Isospin Third Component of Weak Isospin (T3) Weak Hypercharge X-Charge Antiparticle Name Antiparticle Symbol -1 Up Antiquark 𝘂̅ 1 3 Down Antiquark 𝗱̅ 1 1/3 1 -1 Charm Antiquark 𝗰̅ 1/3 -2/3 1 3 Strange Antiquark 𝘀̅ 0 1/3 1 1/3 1 -1 Top Antiquark 𝘁̅ -1/2 0 1/3 -2/3 1 3 Bottom Antiquark 𝗯̅ 0 -1/2 0 -1 -2 -3 -1 Positron 𝗲+ 1/2 0 -1/2 0 -1 -2 -3 -1 Antimuon 𝝻+ -1 1/2 0 -1/2 0 -1 -2 -3 -1 Antitau 𝞃+ 1 -1 1/2 0 1/2 0 -1 0 -3 -5 Electron Antineutrino 𝗩̅𝗲 0 1 -1 1/2 0 1/2 0 -1 0 -3 -5 Muon Antineutrino 𝗩̅𝝻 0 0 1 -1 1/2 0 1/2 0 -1 0 -3 -5 Tau Antineutrino 𝗩̅𝞃 0 0 0 1 0 0 0 0 0 0 0 0 0 Gluon 𝗴 0 0 0 0 1 0 0 0 0 0 0 0 0 0 Photon 𝝲 0 0 0 0 0 1 0 ±1 ±1 ±1 ±1 0 0 0 0 W Boson 𝗪 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 Z Boson 𝗭 0 0 0 0 0 0 0 1 0 1/2 1/2 -1/2 -1/2 1 1 -2 -2 Higgs Boson 𝗛 0 0 0 0 C-1, C-2, C-3 1/2 -1/2 -1/3 1 -1/3 0 1/2 0 -1/2 -1 1/3 -1/3 1 -1 Up Quark 𝘂 -1/3 0 0 0 0 C-1, C-2, C-3 1/2 1/2 -1/3 1 -1/3 0 1/2 0 1/2 2/3 -1/3 -3 -1 Down Quark 𝗱 0 -1/3 -1 0 0 0 C-1, C-2, C-3 0 0 -1 1/3 1 -1/3 0 1/2 0 -1/2 -1 1/3 -1/3 1 -1 Charm Quark 𝗰 0 0 -1/3 0 1 0 0 C-1, C-2, C-3 0 0 2/3 1 -1/3 0 1/2 0 1/2 2/3 -1/3 -3 -1 Strange Quark 𝘀 0 0 0 -1/3 0 0 -1 0 C-1, C-2, C-3 0 0 -1 1/3 1 -1/3 0 1/2 0 -1/2 -1 1/3 -1/3 1 -1 Top Quark 𝘁 0 0 0 0 -1/3 0 0 0 1 C-1, C-2, C-3 0 0 2/3 1 -1/3 0 1/2 0 1/2 2/3 -1/3 -3 -1 Bottom Quark 𝗯 0.0000000000000818710536181118 -1 -1 0 0 0 0 0 0 0 C-1, C-2, C-3 0 0 0 1 1 0 1/2 0 1/2 2 1 1 3 Electron 𝗲 0.0000000000169283371519894 0.0000000000169283371519894 -1 0 -1 0 0 0 0 0 0 0 0 0 0 1 1 0 1/2 0 1/2 2 1 1 3 Muon 𝝻 1776980000 0.00000000028465230159729 0.00000000028470357124737 -1 0 0 -1 0 0 0 0 0 0 0 0 0 1 1 0 1/2 0 1/2 2 1 1 3 Tau 𝞃 0.001 3 0.0000000000000000000001602176565 0.0000000000000000004806529695 -1 -1 0 0 0 0 0 0 0 0 0 0 0 1 1 0 1/2 0 -1/2 0 1 5 3 Electron Neutrino 𝗩𝗲 -1 0.001 200000 0.0000000000000000000001602176565 0.0000000000000320435313 -1 0 -1 0 0 0 0 0 0 0 0 0 0 1 1 0 1/2 0 -1/2 0 1 5 3 Muon Neutrino 𝗩𝝻 -1 0.001 1830000 0.0000000000000000000001602176565 0.000000000000293198311395 -1 0 0 -1 0 0 0 0 0 0 0 0 0 1 1 0 1/2 0 -1/2 0 1 5 3 Tau Neutrino 𝗩𝞃 Lower Bound Upper Bound Lower Bound Upper Bound Left Handed Right Handed Left Handed Right Handed Left Handed Right Handed Left Handed Right Handed 1 1800000 3000000 0.0000000000002883917817 0.0000000000004806529695 0 0 0 0 1/3 0 0 0 0 C1, C2, C3 1/2 1/2 1/3 1 1/3 1/2 0 1/2 0 1/3 1 1/3 1 1/2 1 4500000 5300000 0.00000000000072097945425 0.00000000000084915357945 0 0 0 0 1/3 0 0 0 0 C1, C2, C3 1/2 -1/2 1/3 1 1/3 1/2 0 -1/2 0 1/3 -2/3 2/3 1/2 1 1180000000 1340000000 0.00000000018905683467 0.00000000021469165971 0 0 0 0 1/3 1 0 0 0 C1, C2, C3 0 0 1 1/3 1 1/3 1/2 0 1/2 0 1/3 2 -1/3 1/2 1 100000000 90000000 0.00000000001602176565 0.000000000014419589085 0 0 0 0 1/3 0 -1 0 0 C1, C2, C3 0 0 -2/3 1 1/3 1/2 0 -1/2 0 Quark 3 2/3 1/2 1 172310000000 172570000000 0.000000027607104391515 0.000000027648760982205 0 0 0 0 1/3 0 0 1 0 C1, C2, C3 0 0 1 1/3 1 1/3 1/2 0 1/2 Fermionic Quark 3 -1/3 1/2 1 4150000000 4210000000 0.000000000664903274475 0.000000000674516333865 0 0 0 0 1/3 0 0 0 -1 C1, C2, C3 0 0 -2/3 1 1/3 1/2 0 Confirmed Fermionic Lepton 1 -1 1/2 1 510998.9461 510998.9461 0.0000000000000818710536181118 0.0000000000000818710536181118 1 1 0 0 0 0 0 0 0 0 0 0 0 1 -1 1/2 𝝻 Confirmed Fermionic Lepton 2 -1 1/2 1 105658374.5 105658374.5 0.0000000000169283371519894 0.0000000000169283371519894 1 0 1 0 0 0 0 0 0 0 0 0 0 1 -1 Tau 𝞃 Confirmed Fermionic Lepton 3 -1 1/2 1 1776660000 1776980000 0.00000000028465230159729 0.00000000028470357124737 1 0 0 1 0 0 0 0 0 0 0 0 0 1 Electron Neutrino 𝗩𝗲 Confirmed Fermionic Lepton 1 0 1/2 1 0.001 3 0.0000000000000000000001602176565 0.0000000000000000004806529695 1 1 0 0 0 0 0 0 0 0 0 0 0 Muon Neutrino 𝗩𝝻 Confirmed Fermionic Lepton 2 0 1/2 1 0.001 200000 0.0000000000000000000001602176565 0.0000000000000320435313 1 0 1 0 0 0 0 0 0 0 0 0 Tau Neutrino 𝗩𝞃 Confirmed Fermionic Lepton 3 0 1/2 1 0.001 1830000 0.0000000000000000000001602176565 0.000000000000293198311395 1 0 0 1 0 0 0 0 0 0 0 Gluon 𝗴 Confirmed Bosonic Vector Boson 0 0 1 -1 0 0 0 0 0 0 0 0 0 0 0 0 0 λ1, λ2, λ3, λ4, λ5, λ6, λ7, λ8 Photon 𝝲 Confirmed Bosonic Vector Boson 0 0 1 -1 0 0 0 0 0 0 0 0 0 0 0 0 0 W Boson 𝗪 Confirmed Bosonic Vector Boson 0 ±1 1 -1 80370000000 80400000000 0.000000012876693052905 0.0000000128814995826 0 0 0 0 0 0 0 0 Z Boson 𝗭 Confirmed Bosonic Vector Boson 0 0 1 -1 91185500000 91189700000 0.0000000146095271167807 0.000000014610200030938 0 0 0 0 0 0 0 Higgs Boson 𝗛 Confirmed Bosonic Scalar Boson 0 0 0 1 124880000000 125300000000 0.00000002000798094372 0.00000002007527235945 0 0 0 0 0 0 Up Antiquark 𝘂̅ Confirmed Fermionic Antiquark 1 -2/3 1/2 -1 1800000 3000000 0.0000000000002883917817 0.0000000000004806529695 0 0 0 0 -1/3 Down Antiquark 𝗱̅ Confirmed Fermionic Antiquark 1 1/3 1/2 -1 4500000 5300000 0.00000000000072097945425 0.00000000000084915357945 0 0 0 0 Charm Antiquark 𝗰̅ Confirmed Fermionic Antiquark 2 -2/3 1/2 -1 1180000000 1340000000 0.00000000018905683467 0.00000000021469165971 0 0 0 Strange Antiquark 𝘀̅ Confirmed Fermionic Antiquark 2 1/3 1/2 -1 100000000 90000000 0.00000000001602176565 0.000000000014419589085 0 0 Top Antiquark 𝘁̅ Confirmed Fermionic Antiquark 3 -2/3 1/2 -1 172310000000 172570000000 0.000000027607104391515 0.000000027648760982205 0 Bottom Antiquark 𝗯̅ Confirmed Fermionic Antiquark 3 1/3 1/2 -1 4150000000 4210000000 0.000000000664903274475 0.000000000674516333865 Positron 𝗲+ Confirmed Fermionic Antilepton 1 1 1/2 -1 510998.9461 510998.9461 0.0000000000000818710536181118 Antimuon 𝝻+ Confirmed Fermionic Antilepton 2 1 1/2 -1 105658374.5 105658374.5 Antitau 𝞃+ Confirmed Fermionic Antilepton 3 1 1/2 -1 1776660000 Electron Antineutrino 𝗩̅𝗲 Confirmed Fermionic Antilepton 1 0 1/2 -1 Muon Antineutrino 𝗩̅𝝻 Confirmed Fermionic Antilepton 2 0 1/2 Tau Antineutrino 𝗩̅𝞃 Confirmed Fermionic Antilepton 3 0 1/2 Created by Harry Robert Alan Janes, ©2017
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Reform Essay #1 It is nearly uncontested that the national legislature of the United States is massively flawed. Seldom is it contested, specifically, that many of these flaws originate in the structure of the government. Armchair political theorists the world over note problems and generate solutions, although it must be said that no two theorists concur on either the nature of the problems or the optimal solutions thereof. That said, as an armchair political theorist, it seems incumbent upon me to spew my ideas across the land. Before we start, it must be made clear that among the more common objections to any proposed reform is that the Founders of the United States did not intend it. Leaving aside the hagiographic interpretation of American history necessary to believe that they were infallible and the many successful amendments showing that such changes as these have had a good track record, so to speak, the governance available for a largelyagricultural nation of fewer than four million residents, where the fastest transportation was the horse and the fastest calculator the abacus, is not the same as the optimal governance for the present United States, nor will either it or this be optimal in the America of nearly two and a half centuries hence. There seem to be two major schools of thought regarding the purpose of a legislator. The first, of which the FirstPastThePost system is the brainchild, suggests that a legislator’s responsibility is to the area that elected that representative, and that a legislature ought to be the meetingplace of the voices chosen to speak for various communities. The other theory, which begat Proportional Representation, contends that each representative represents an ideologicallybound swathe of the population say, onefourth of one percent of all voters that votes for a certain ideology shared by that representative, and that a legislature ought to be the political views of the nation in a microcosm. Both schools of thought have their positives and negatives. The former means that it is possible for beliefs that are common but do not prevail in any particular community to be silenced. The latter means that no one legislator is tied to a community, and thus that the interests of that community go without support. The former means that a plurality interest or view in individual communities can become the sole interest or view represented, even if the other views are similar enough that, banded together, they would outnumber them. The latter means that legislators who do badly can only be easily removed by their parties. The former means that interests bound to a particular area, even if they are despised by the country at large, can be represented. The latter necessitates large parties and disadvantages nonpartisan but popular candidates. And so on, and so forth... It seems likely that no system of government yet designed will both perfectly represent the political views of the populace and produce the optimal results for the purposes of good governance, even when the two are in concord indeed, it is unlikely that any system will successfully do either one. That said, there are nevertheless improvements to be made to the present system. While the former view the view of FPTP is massively prevalent in the United States government, the alternative also makes good points and deserves a seat at the table. And what better place than the Senate, that great Proteus of the government first the voice of the state legislatures, then that of the people of the various states, with its elections arrhythmically staggered in an odd 2/3 time signature. In truth, the states are strange choices for electoral districts except for a few examples, too small for a viable regional identity, yet too large for a local one, usually too heterogenous to represent a specific community or type of community yet too homogenous to be reasonably competitive, and nowhere near proportional, with the residents of Wyoming having more than sixty times the electoral power of an equivalent quantity of Californians. What better solution than to replace the entire thing with a system which represents all Americans equally, is founded on a national identity rather than any smaller one (or, perhaps, if necessary, a number of regional interests that elect national representatives), and is exactly as heterogenous or homogenous as the country? Granted, such a system would be illfitting for the endall and beall of the legislature but its consistency of results make it nearlyideal as an upper house. And what of the lower house? Political factions are fractal. There are two schools of thought regarding how a district ought to be designed that a district ought to reflect some kind of natural community, and that a district ought to be designed so that it changes with the nation. The extent of the former would be a district filled with homogenous electors, seldom changing its political affiliation only when the mass views or party loyalty of the public changed, as in the American South between 1960 and 1972. The latter suggests a legislature that vacillates from one supermajority to another, according to the vicissitudes of the electorate amplified to staggering crests and troughs. The former, it seems selfevident, is a better model for a legislature founded on representing the wills of individual constituencies. But while the United States House of Representatives intends to represent individual constituencies, it is subverted by gerrymandering and singlemember districts, which split natural communities. Granted, singlemember districts have their advantages. Notably, it improves minority representation when the Texas House of Representatives switched over in 1972, AfricanAmerican members were elected for the first time since Reconstruction. But that minority candidates are disadvantaged is not solely the fault of multiplemember districts after all, they remain disproportionally uncommon in singlemember legislatures. That minority candidates have been forced to obviate representative democracy means that the forces that oppose them should be tackled first, but it does not in and of itself present a reason not to use multimember districts. Where, in multimember and fairly apportioned districts, it could honestly be said that there are five national representatives for Houston (or perhaps three from South Houston and two from North Houston, or some other scheme), in this present system, it can only be said that there is one district for a swathe of Houston stretching from Atascocita to Montrose by way of Spring, another for a vaguely horseshaped zone between Bush Intercontinental and Downtown Houston, &c... But why should representation be dependent on where someone lives in many ways, the least important thing about a person? What common interests bind a Channelview longshoreman and an affluent Downtown lawyer, more than they are bound to their compatriots in, say, Los Angeles? Why should the vote of a company executive in River Oaks determine who represents a teacher in Bellaire, or vice versa? In this new world of the Internet of, as one might say, edemocracy why must we be bound to the districts of the past, which divert untold billions into porkbarrel spending? True, local affairs such as roads bind them but shouldn’t those be handled by local authorities anyway?
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Divider Page from Original TWI Materials Bound Text 111-Job Methods The Training Within Industry program of Job Methods was developed in order to provide management with a tool whereby supervisors could acquire skill in improving methods.
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