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Print setup allows the user to de ne the printer and other print settings before printing In some applications, the Print menu option provides this feature and the user must view this dialog every time printing is required In this example, the features are separated to give the user an easy way to print to the default printer without accessing the setup dialog Either way you prefer, this feature is easy to implement because it uses the same PrintDocument control and associated code required to implement the Print feature To implement a Print Setup feature: 1 Ensure that there is a way for the user to select a Print Setup This is most logically de ned near the Print option In some cases, the setup is handled in the Print option, and a separate Print Setup option is not desired 2 Add the PrintDialog control to the form from which the user initiates the Print Setup process This is normally the same form containing the PrintDocument control Give the control a logical name, such as PTPrintDialog 3 In the event handler for the control that initiates the Print Setup, write the code required to display the Print dialog The code involves associating the appropriate PrintDocument control with the Print dialog, displaying the Print dialog, and then, if the user clicked OK, printing the document as follows:

I I mean. in the sense of the Newton-Wigner-Wightman group theory approach [464. 643]. 2That is the method Dirac developed to derive the Dirac equation for the e1eclron.

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One of the consequences of having a maximum speed allowed in nature is that we can no longer assume that certain physical observables can be determined exactly In particular, it turns out that although the momentum of a single particle can be determined with arbitrary accuracy, there is a limit to the accuracy that can be achieved in a measurement of position This is deeply connected with the problem of pair creation out of the vacuum mentioned above Let us now look more closely into these issues The natural way to measure the momentum of a particle is by doing a scattering experiment (ie, we let it collide with a control object) Ideally, we would like to have a control object that behaves like a perfect mirror, bouncing the particle off itself.

4

As this is a control object, we assume that we know its energy f and momentum p before and after (denoted by primes) the collision Momentum conservation applies rigorously, but energy will only be conserved within the limits prescribed by the timeenergy uncertainty relation This uncertainty relation has a status different from that of the position-momentum uncertainty relation as, unlike that relation, it is not derived from a commutator relation (see the recommended reading at the end of the chapter), and it has been often misinterpreted It does not mean that the energy cannot be known exactly at a given time, nor that the energy cannot be measured with arbitrary accuracy within a fixed time interval What it does mean is that the measurement makes the state after the measurement differ from that before the measurement.

PTPrintDialogDocument = PTPrintDocument Dim oResult As DialogResult = PTPrintDialogShowDialog If oResult = WindowsFormsDialogResultOK Then PTPrintDocumentPrint() End If

This difference causes an energy uncertainty in both the states before and after the measurement on the order of at least hi Dt, where Dt is the time the measurement lasts [388] So if we denote by P the momentum of the particle before the collision, by E its energy before the collision, and use the same symbols primed for these quantities after the collision, we can write the following conservation laws.

may be used sparingly to improve the quality of service of an already working implementation, but they should never be used to fix a program that barely works

+p =p' +p',

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