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where BW noise bandwidth of the receiver, or approximately the 6-dB-down bandwidth (instead of the typical 3-dB bandwidth), and NF receiver s noise figure, dB 3 The third-order intercept point (IP3) is approximately 10 to 15 dB above the P1dB compression point, and is the location where, if the gain slope of the receiver could continue, the undesired output third-order frequency products would be at the same amplitude as the output two-tone fundamental test signals that had been originally placed at the receiver s input To compute the total cascaded input IP3 (IP ) of multiple stages of a receiver TOT (Fig 92), use the formula:

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To serve a PDF document in ASP.Net MVC requires generating a FileResult method. With IronPDF you can use mvc to return a pdf file. This method may then be served by your controller. For a more advanced example you might use your HTML View to generate a HTML string and then convert it to PDF as above.

We covered limitations briefly when we first introduced ROME in chapter 5, but they re worth mentioning again. ROME s two most significant limitations are:

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It s based on XML DOM ROME uses the DOM-based JDOM XML processing API. So when you parse or generate a newsfeed with ROME, it builds a complete model of the newsfeed in memory. If you need to parse extremely large newsfeeds, this approach may not be workable. If that s the case, you should consider using a SAX-based parser, such as the Jakarta Feed Parser. It s not liberal XML parsers, such as JDOM, reject files that are not wellformed XML. Since ROME is based on JDOM, ROME has the same problem. It does attempt to do some error correction, but if you really need to be forgiving, you ll need to use the ultra-liberal Universal Feed Parser.

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where IP receiver s total IP3 from its input to its output and IP3n and TOT GAINn are linear terms, not decibels 4 The importance of a low NF in a receiver is demonstrated by its linear relationship with SNR For instance, if a receiver has an NF of 12 dB, and the SNR at its output is 20 dB, we can improve the SNR to 30 dB (using the same input signal power and receiver gain) by decreasing the receiver s NF to 2 dB This is a 10-dB improvement in NF and in SNR Thus, if a certain signal power is placed at the input of a 5-dB NF receiver, and this creates an output with an SNR of 20 dB, then the actual input SNR to the receiver will have been 25 dB In other words, the receiver added 5 dB to the noise at its output: the receiver s NF directly correlated into a decrease in the output signal s SNR This also affects the power that the transmitter must send to the receiver s antenna to make up for the decreased SNR caused by a receiver s poor NF, with a relationship that is also dB for dB The NF for a receiver can be calculated by using Friis s equation, with the noise figure itself not needing to be referenced to any particular bandwidth, since it is a ratio between the input and the output of a receiver (or amplifier) over exactly the same bandwidth: NFTOTAL 10 log (10NF1/10) (10NF2/10) 1 (10G1/10) (10NF3/10) 1 (10G1/10) (10G2/10) (10NFn/10) 1 (10 ) (10G2/10) (10Gn/10)

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It s possible that both of those limitations will be addressed in future releases of ROME, but for now you ll have to keep them in mind. Next up, the last topic in our introduction to ROME: the ROME subprojects.

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In addition to the core ROME parser, generator, and converter API, the ROME developers are working on a set of subprojects. These projects are released separately from ROME and most are versioned separately from ROME. Some are more complete than others, and some are far from being finished. The ROME subprojects fall into two main categories: extension modules and others. Let s start with the extension modules. Extension modules

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