This disambiguation page lists articles associated with the title Canon. If an internal link led you here, you may wish to change the link to point directly to the. Stuurprogramma's, software, firmware en handleidingen voor uw Canon-product downloaden en online toegang verkrijgen tot technische ondersteuning en probleemoplossing. Find all HP Printer Ink Cartridges and HP Toner Cartridges. Welcome to our Hewlett Packard printer supplies page. HP printers have been printing pioneers. The 8 Best All- In- One (AIO) Printers to Buy in 2. We haven't realized the paperless office yet. Most people still need a good printer now and then, and a good all- in- one, or AIO, a printer that can also copy, scan, and sometimes, depending on the type of machine, fax, can come in handy. Like everything tech, printers are less- expensive than ever before, and now most all- in- one printers work wirelessly through Wi. Fi, and many support mobile connectivity through Wi. Fi Direct, Near- Field Communication (NFC), and numerous cloud sites, such as Google Cloud Print. Nowadays, the convenience and productivity options seem endless; to help you pick out which AIO is best for you, here's a list of the best printers to buy in 2. The Epson Work. Force Pro WF- 4. AIO high- volume printer, and it's been around long enough that it's usually on sale for less than $2. Print quality is excellent, including near- laser quality text, NFC touch- to- print and Wi. Fi Direct support for network- free printing are supported. And, like just about every printer available nowadays, you can easily print from your i. Phone, i. Pad or Android devices. The Epson Work. Force WF- 4. It can perform two- sided printing, copying, scanning, and faxing, and it has a 3. Its intuitive touchscreen control panel makes it easy to use, and it's rated at 2. This four- color inkjet printer has a maximum resolution of 4. If you use this printer's high- yield cartridges, it will provide you an excellent cost per page. Operating costs are less than 1 cent per black and white page, and less than 5 cents per color page. It also has great features for the office, including duplex (two- sided) printing, and wireless printing from devices via Air. Print, Google Cloud Print, Mopria, Brother i. Print& Scan and Wi. Fi Direct. Networking is enabled via Wi. Fi, Ethernet, Wi. Gutenprint and Gimp-Print for Mac OS X (10.2 through 10.11 and later) High quality printer drivers for Canon, Epson, Lexmark, and PCL printers. Download Printer / Scanner drivers, firmware, bios, tools, utilities. Official Canon imageRUNNER ADVANCE 8105 Free Driver Download for Windows 7, 2008, 2003, XP, 2000 - UFRII. World's most popular driver. Fi Direct, or you can print directly from USB. Paper capacity is 1. You can print up to 1. You can manage your printing jobs via a 4. Wireless printing is facilitated by Air. Print for Apple devices and NFC touch- to- print for other smart devices. Some users have commented they have had difficulty setting up wireless functionality, but once up and running it offers a seamless and convenient way to bring your documents to life. Impressive print management options are buoyed by high speeds, with ultra- fast automatic two- sided printing and a 5. HP claims the specs are 2. The high volume trays and efficient ink model result in up to 5. Documents scan at 1. I like the HP Envy 5. All- in- One because it performs all of its main features, print, copy, and scan, well. It prints photos better than many equally priced AIOs. This is, however, a low- volume, entry- level printer; hence the paper input drawer is somewhat small (1. Choose this printer is you have a relatively low print volume. You can print, copy, scan or fax from this compact AIO, and the automatic document feeder is capable of holding 3. Two- sided printing is available, and print speeds are rated at 9. The XP- 8. 30 has the additional ability to print on pre- surfaced optical discs. This Small- in- One is a great option for someone who doesn’t have heavy usage demands and wants an inexpensive all- in- one with superior print quality. Mobile printing options, such as printing directly from your phone or tablet, are a snap thanks to Epson Connect software and other mobile printing options. A 4. 3- inch touchscreen makes it easy to use. And it’s small, at 1. It delivers excellent text output quality and has a solid set of features. Wi. Fi Direct allows you to connect to mobile devices without a router, and you can print and scan on- the- go with Canon Print, Apple Air. Print, Mopria and Google Cloud Print. You can use USB Direct to print to and scan from a USB connected device. Secure Print ensures the privacy of your printed documents, and you can set up password protection for up to 3. The MF4. 14dw is rated by Canon for speeds of up to 3. An intuitive 3. 5- inch touch LCD display makes menu navigation simple. You can load this printer with up to 2. ADF for scanning, as well as a 5. The printer purchase includes one cartridge and it's good for about 2,4. You get a 5. 00- sheet paper cassette up front and an 8. It supports Wi. Fi, Ethernet, and USB, as well as Wi. Fi Direct and Near- Field Communication (NFC) for making peer- to- peer connections with your mobile devices. You can add two 5. Ink comes in huge cartridges capable of thousands of pages. It's rated at 8 pages per minute (ppm) for black- and- white pages, and 4ppm for color pages, which is relatively slow. The included My Image Garden software is unfortunately not too intuitive, but you can print from any software, including apps from the Apple Store and Google's Play Store. The maximum color resolution of 4. Google Cloud Print are great to have at this price point. One ink cartridge is included with this printer, and it’ll last you about 3. This is a good deal, but it only makes sense to buy it if you plan to print occasionally, as the printer uses a lot of ink and the price of replacement ink is on the high side.
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A more detailed discussion of fission weapon design is aided by introducing more carefully defined means of quantifying the dimensions and time scales involved in fission explosions. These scale factors make it easier to analyze time- dependent neutron multiplication in systems of varying composition and geometry. It uses the concept of the . If the interaction is a scattering event, then one neutron is emitted. If the interaction is a fission event, then the average number of neutrons produced per fission is emitted (this average number is often designated by nu). By combining these we get the average number of neutrons produced per collision (also called the number of secondaries), designated by c. MFP = 1/(cross. This rate is measured by the number of neutrons lost per collision. For a given geometry, the rate is determined by the size of the system in MFPs. Put another way, for a given geometry and degree of reactivity, the size of the system as measured in MFPs, is determined only by the parameter c. The higher the value of c, the smaller the assembly can be. Since the mass of the system is equal to volume*density, and volume varies with the cube of the radius, we can immediately derive the following scaling law. Eq. C is the degree of compression (density ratio). This scaling law applies to bare cores, it also applies cores with a surrounding reflector, if the reflector is density has an identical degree of compression. This is usually not the case in real weapon designs, a higher degree of compression generally being achieved in the core than in the reflector. For most implosion weapon designs (since C. We are thus very interested in measuring the rate of the fission reaction. This is done using a quantity called the effective multiplication rate or . The neutron population at time t is given by. Eq. This interval is known as the . The more familiar concept of . The time constant goes to infinity at criticality. Therefore I will henceforth refer to the quantity 1/alpha as the . If we assume no losses from the system then alpha can be calculated by. It provides an upper bound for reaction rates, and provides a good indication of the relative reaction rates in different materials. For very large assemblies, consisting of many critical masses, neutron losses may actually become negligible and approach the alphas given below. In real systems there is always some leakage, when this leakage is taken in account we get the . When the effective neutron number is zero the system is exactly critical. Calculating tau and alpha from differential cross section measurements, adjusted neutron spectrums, etc. Compression to above normal density (achievable factors range up to 3 or so in weapons) reduce the MFPs, alphas (and the physical dimensions of the system) proportionately. In real fission weapons (unboosted) effective values for alpha are typically in the range 2. Collecting data for systems at high densities requires extremely difficult high explosive experiments, and data for high alpha systems can only be done in actual nuclear weapon tests. The most convenient measurements are of the negative alpha value for fast neutron chain reactions at delayed criticality. Since at prompt critical alpha is exactly zero, the ratio of the magnitude of this delayed critical measurement to the fraction of fission neutrons that are delayed allows the alpha value to be calculated. These were the only sort of alpha measurements available to the Manhattan Project for the design of the first atomic bombs. These two systems used bare metal weapon grade cores, so the properties of weapons material was being measured directly. Godiva consisted of oralloy (9. U- 2. 35, 5. 2. 4 wt% U- 2. U- 2. 34), Jezebel of weapon- grade delta- phase plutonium alloy (9. Pu- 2. 39, 4. 8. 48 wt% Pu- 2. Table 4. 1. 2- 2 Properties of Bare Critical Metal Assemblies. Mass, Density, and Measured Alpha are at Delayed Critical (D. C.). Assembly Material Mass Density Meas. Alpha. Name kg (1/microsec) Fraction (1/microsec). Godiva Oralloy 5. Jezebel WG- Pu 1. The calculated values of alpha from the Godiva and Jezebel experiments are reasonably close to those calculated above from 1 Me. V cross section data. Adjusting for density, we get 2. U- 2. 35 (1 Mev data) vs 1. If the system radius R = r. The more critical masses present, the closer alpha comes to the limiting value. This can be estimated from the relation. Eq. Since the rate of energy release at any point in the core is proportional to the flux at that point, this also affects the energy density throughout the core. This is a matter of some significance, since it influences weapon efficiency and the course of events in terminating the divergent fission chain reaction. Computing the ratio between the flux at the surface of the critical system, and the maximum flux (in the center) we find. Table 4. 1. 3- 1 Relative Flux at Surface. If the system is supercritical, then the flux distribution becomes flatter, since neutron production over- balances loss. The greater the value of alpha for the system, the flatter it becomes. The addition of a neutron reflector also flattens the distribution, even for the same degree of reactivity. The flux distribution function is useful though, since the maximum rate of fission occurs at the moment when the core passes through second criticality (on the way to disassembling, see below). The fission reaction rate at any point in the core is proportional to the flux. The net burnup of fissile material (and total energy release) is determined by the reaction rate integrated over time. The outer layers of material will be fissioned less efficiently than the material near the center. The steeper the drop off in flux the greater this effect will be. We can thus expect less efficient utilization of fissile material in small cores, and in materials with low values of c. From the relatively low value of c for U- 2. U- 2. 33 and Pu- 2. U- 2. 35 will be used less efficiently. This is observed in pure fission tests, the difference being about 1. Nearly all of the energy present has thus been produced in the last one or two multiplication intervals, which in a high alpha system is a very short period of time (1. There is not much time for heat flow to significantly alter this energy distribution. Since most of the energy is present as a photon gas the dominant mechanism is radiation (photon) heat transport, although electron kinetic heat transport may be significant as well. This heat flow can be modelled by the diffusion approximation just like neutron transport, but in this case estimating the photon mean free path (the opacity of the material) is quite difficult. A rough magnitude estimate for the photon MFP is a few millimeters. In a bare core this cooling can be quite dramatic, but the presence of a high- Z tamper (which absorbs and re- emits energy) greatly reduces this cooling. Losses also occur deeper in the core, but below a few photon MFPs it becomes negligible. Otherwise, there is a significant shift in energy out of the center of the core that tends to flatten the energy distribution. Since the temperature in radiation dominated matter varies with the fourth power of the energy density, the temperature distribution is rather flat (except near the surface perhaps). The pressure is proportional to the energy density, so it varies in similar degree. The final event in the process - disassembly - is especially important since it terminates the fission energy release and thus determines the efficiency of the bomb. In each of these states a different set of physical processes dominates. Reactivity insertion begins by increasing the average density of the configuration in some way. Although nearly all neutrons produced by fission are emitted as soon as the atom splits (within 1. U- 2. 35, 0. 2. 5% for Pu- 2. In delayed criticality these neutrons are required to maintain the chain reaction. These long delays mean that power level changes can only occur slowly. All nuclear reactors operate in a state of delayed criticality. Due to the slowness of neutron multiplication in this state it is of no significance in nuclear explosions, although it is important for weapon safety considerations. Rapid multiplication can occur after this point. In bomb design the term . For our purposes we can take the value of alpha as being zero at this point. The reactivity change required to move from delayed to prompt criticality is quite small (for plutonium the prompt and delayed critical mass difference is only 0. U- 2. 35 it is 2. Passage through prompt criticality into the supercritical state is also termed . During this phase the reactivity climbs, along with the value of alpha, as the density of the core continues to increase. Any insertion system will have some maximum degree of reactivity which marks the end of the insertion phase. This phase may be terminated by reaching a plateau value, by passing the point of maximum reactivity and beginning to spontaneously deinsert, or by undergoing explosive disassembly. Any neutrons introduced into the core after prompt criticality will initiate a rapid divergent chain reaction that increases in power exponentially with time, the rate being determined by alpha. If exponential multiplication begins before maximum reactivity, and insertion is sufficiently fast, there may be significant increases in alpha during the course of the chain reaction. 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