Qrystal MqKenzie

get rid of the bloatware

Good responsive touchscreen

very easy to read

Surfs the web as fast as a desktop

Very easy to install ram

quite speedy and I feel little to no lag

clean install of windows

there is only 1 slot for memory

The hinge is EXTREMELY strong and very well built.

Even on full power mode this unit doesn't get too hot

My favorite feature? Watching the iPhad junkies jaws drop when I turn my tablet into a *real* computer in a blink of an eye.

something I can carry around the house or travel with

8.9" would be my limit for size though as keyboards cannot be any smaller

makes NO noise

nice looking, multi-touch machine to goof around with, it will not disappoint

Multi Touch

Keyboard keys are big for the dimension of the netbook.

Keyboard is a little cramped but good for the size, still is easy to type extra keys and I have small fingers.

analysis of the EPR argument. We will see that they really applied the Lüders postulate

formal application of the original von Neumann postulate blocks the EPR considerations

quantum teleportation scheme. We will see again that it is fundamentally based on the use of the Lüders postulate

If we were to replace E in this equation with the operator  ih(∂/∂t), the resulting equation of motion would involve the second  time derivative of the wave function, in contrast with the non-relativistic Schrödinger  equation, in which only the first time derivative of the wave function  appears.

justification of this  statement involved the need for the probability density of the wave to be  always positive

a wave equation  whose solutions would be solutions of (2), but that was linear in E

These four  quantities, along with unity, form the basis of what is called a Clifford  algebra

not commutative, a fact which suggests some underlying structure. (The  articulation of non-commuting entities into structures of commuting entities is  a useful heuristic principle, although it is rarely mentioned explicitly.

the wave function  of this particle must actually have four components

analogous to the relations for the components of  angular momentum of a classical particle

each of the four components y₁,  y₂, y₃, y₄ of the original four-dimensional vector of wave  functions individually satisfies the Klein-Gordon equation

either f_a by  itself or f_b by itself is  sufficient to determine the complete wave function y for a given basis

the signs of the Pauli spin matrices are reversed

left-handed and right-handed spin states of  the particle for that basis

if y is  a solution of Dirac’s equation (6), it follows that g₅y is also  a solution, but with the momentum and the energy negated relative to the sign  of the mass

when m is not zero, the  distinction between the two factors may be extremely small if the energy and  momentum are extremely large, i.e., for a particle moving at close to the  speed of light

for any given solution y, the wave functions Iy  and g₅y are also solutions, and since the Dirac  equation is linear, any linear combination of solutions is also a solution

the non-zero parts of y_L and y_R are just the two-dimensional vectors f_a and f_b discussed previously

f_a  and f_b are the same except  for having opposite intrinsic spin

each quantum “orbit” can be occupied by two electrons with opposite  spins

for a stationary  particle, the wave function y should  be independent of time, except for possibly an unobservable phase advance

in order for f_a and f_b to be  harmonic functions, the quantity in parentheses in this equation must vanish

We expect both of these “spin divergences” to vanish, so  the second equation requires us to set f_b = 0. Hence, with this  basis applied to stationary (or approximately to slowly moving) particles, we  have f_b = 0

The only non-vanishing solution is with w equal to

two components of f_a  (i.e., f₁ and f₂) consist of the two spin  states of the particle

it turns out that Dirac’s equations actually is invariant  under Lorentz transformations, provided we take into account the  transformation properties of the g  matrices

the Weyl basis is convenient for high-speed electrons (for  which the momentum is much larger than the rest mass), and the Dirac basis is  convenient for stationary or low-speed particles

let the  contravariant and covariant components of a given 4-vector be denoted with  super-scripted and sub-scripted indices respectively

The differential operators ∂/∂x^m transform as the components of a  covariant 4-vector, so for convenience we will denote them by ∂_m

the contravariant and covariant components of  any 4-vector “a” are related by

       

 

       

before we can assert that this equation is invariant under Lorentz  transformations, we need to show that y’(x’)  represents the same physical wave function with respect to the spacetime  coordinates x’ as is represented by y(x)  with respect to the spacetime coordinates x. This requires us to show that  they have the same probability density at any given event.

the four components of y can be split  into two inter-related bi-vectors y_a  and y_b, and the  interchange of these two represents another kind of “transposition”

in a relativistic theory the probability density cannot be  invariant under Lorentz transformations if probability is to be invariant,  just as the charge density cannot be invariant if charge is invariant

three transformations, consisting  of the overall transposition, the complex conjugation of the elements, and the  transposition of the two bi-vectors

. This positive-definite quantity  represents the probability density, which transforms (as it should) under a  Lorentz transformation in the same way as the time coordinate of a timelike  interval

obviously real-valued, and it is positive  definite, because the minimum value it can take is with the cosine equal to  -1

the probability current, i.e.,  the probability of the particle crossing a given plane (normal to a given  direction) per unit area and per unit time

the four components of the wave  function y can be split into two  sets, y_a and y_b, each consisting of two  components, and these two sets are redundant, so the particle can be  represented by just two wave functions, corresponding to the two possible  spin states for a given basis

the transformation from one basis to another can make  use of these four degrees of freedom to produce an unexpected (in 1927)  consequence

Our argument is  valid only provided the position of the particle is an observable. If this  assumption holds, the particle must have a spin angular momentum of half a  quantum

he didn’t regard massive bosons as “important”. It isn’t  clear what he meant by this (perhaps he meant that such particles are not elementary?

quantum wave function itself as an  operator, giving a field representation of all the possible quantum fields

any relativistic description of a particle necessarily involves not just the  wave function of a single particle, but multiple wave functions representing  the potential for other particles

Notice the physical sensation of fear- and revel in it.

Breath into it. Already you should start to feel more spacious and calm.

most of the time these phrases are TRUE- but incomplete.

clamp down from the fear, and miss the most critical and helpful part of the message

ask in your heart, with a willingness to be surprised, for the rest of the message

your friend Fear been shouting herself hoarse

allergies

balance problems

brain fog, confusion, and/or memory loss

colds, recurring and with
  decreased resistance to infection

dandruff problems [chronic]
  that don't go away despite use
  of anti-dandruff shampoos

depression/anxiety/dementia

diarrhea

fatigue [chronic, excessive, or continued]
  and/or general malaise

feeling lost or "disconnected" from what's
  happening around you

headaches

hypersensitivity to mold

irritability

learning difficulties or mental functioning
  problems or personality changes

memory loss or memory
  difficulties/Alzheimers-like symptoms

sinus congestion, sinus problems,
  and chronic sinusitis

sleep disorders

sneezing fits (more than three
  sneezes in a row, happening often)

sore throat

swollen lymph nodes

vertigo [feelings of dizziness, lightheadedness,
  faintness, and unsteadiness]

It (the dryer) is serviced from the front.

5303281153

To raise the top of the dryer, insert a putty knife into the crack between the top and the front panel and push against the spring clips to release them. There are two clips, anywhere from 23 to 8 inches in from the sides. You should be able to feel the spring tension when you push on them. Push one in slightly, and raise that side, then the same for the other end of the main top. Once the top is up, you will disconnect the wires to the door switch (right side, on the backside of the front panel), if there are 3, mark them somehow to get them back correctly, if only 2 wires, no need as location makes no difference. Then remove the phillips screw holding the yellow tab-looking plastic thing front and center in the top of the front panel. Then remove the 2 screws holding the front panel to the side panels, screw heads are inside the cabinet, screws pointing towards you. Pull the front panel away and lift off the bottom clips to remove. Now remove the belt from the idler pulley. The idler is located right behind the blower/motor unit. Make sure to note how the belt goes around the idler so you get it back on right. Once the belt is free, slide the belt to the back edge of the drum and, using it as a handle (on the top side of the drum), lift straight up to disengage the rear bearing from the cradle. This can be a very tight fit, especially if it worn badly. You may have to pull relatively hard. Once done, the drum will pull out through the front of the cabinet. Now you can see the drum support ball on the back of the drum and the cradle that holds it. Simply keep note of how you remove the cradle from the back wall to reassemble it correctly (this is where 4 hands are better than 2 and don't loose track of the ground bearing from the back). Using a small drop of supplied grease to keep the bearing in the plastic cradle makes reassembly much easier. As far as the post on the back of the drum is concerned, if the new and old parts look ABSOLUTELY identical, leave it alone and just clean it up good. If you must change it (another place where 4 hands are better than 2), be very careful with the new screws, because they are cheap and the heads strip almost instantly. Put a generous portion of supplied grease into the cradle and reassemble the dryer.

If you had to change the rear support on the back of the drum, you might want to look that over once more to make sure it's together right and tight. The rear of the drum runs very close to the heater and its ceramic insulators and I would hate to see you short out your heating element because you overlooked something. It could also be the belt tracking wrong in the idler pulley.

use #10 x 1/2" Hex Heads instead of the crappy, easily stripped screws that are included with the repair kit

I went to a Sears with a Parts area with my model # and the parts # he suggested. Paid $28.00 for the kit, went home followed his directions and replaced all the pieces in a little over an hour by myself

in my dryer there was no reason to disconnect the door switch. I wasn't going to work on the dryer with power applied, so there was no danger of accidental turn-on, and the wires only go to the front panel. I don't think there was any reason to remove the funny yellow thing either. To pop the drum out of the old bearing I used my hands leveraged against the back panel, rather than pulling on the belt.

the idler pulley in attached to a spring loaded "L" bracket that rotates, slackening the belt for removal and reattachment. I should have known this before proceeding but did not.

- the idler pulley is spring loaded. when you remove the spring be prepared for the parts around it to fall out/down. if you have a rear fan panel on the back side, it may be easier for you to access the idler this way. take a picture of what the pulley looks like before you remove the spring.
 - the smaller bearing was completely gone (ground away) so we were unsure where the new one went, but we figured it out
 - you will need new screws. buy some 10 x1/2 and a few nuts. we used hex washer heads.
 - when you are re-assembling the drum it will appear to hang too low and angle slightly. this will fix itself when you put the front panel back on.