Integrate Electronically Signing Termination with airSlate SignNow
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Your step-by-step guide — integrate electronically signing termination
Using airSlate SignNow’s eSignature any business can speed up signature workflows and eSign in real-time, delivering a better experience to customers and employees. integrate electronically signing termination in a few simple steps. Our mobile-first apps make working on the go possible, even while offline! Sign documents from anywhere in the world and close deals faster.
Follow the step-by-step guide to integrate electronically signing termination:
- Log in to your airSlate SignNow account.
- Locate your document in your folders or upload a new one.
- Open the document and make edits using the Tools menu.
- Drag & drop fillable fields, add text and sign it.
- Add multiple signers using their emails and set the signing order.
- Specify which recipients will get an executed copy.
- Use Advanced Options to limit access to the record and set an expiration date.
- Click Save and Close when completed.
In addition, there are more advanced features available to integrate electronically signing termination. Add users to your shared workspace, view teams, and track collaboration. Millions of users across the US and Europe agree that a system that brings everything together in one holistic work area, is the thing that businesses need to keep workflows functioning effortlessly. The airSlate SignNow REST API allows you to embed eSignatures into your application, internet site, CRM or cloud. Try out airSlate SignNow and get faster, smoother and overall more effective eSignature workflows!
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Integrate esign termination
- Hey, everybody. Thanks for tuning in. I'm Zach Peterson, I'm a technical consultant with Altium, and today we're gonna continue talking about a topic that we started on a little bit ago, and we're gonna wrap it up today. And this topic is input impedance, and specifically how it relates to termination in transmission lines into the circuits. So, this was inspired by a viewer question that was sent into our Q and A, and I wanted to look at this one specifically because it is an interesting question and it is something that comes up when you're working in RFPCDs. So let's go ahead and dig into it and get started. (upbeat music) Okay, so before we get started, I wanna look at a question that was sent in by one of our viewers, Mohammed Ahmad. "Hi, Sir, your video tutorials are really nice and helpful. Please answer the following questions." And he goes into a question about microstrip transmission lines and using a PI matching filter along the line. Now, this is typical in RF interconnects, and specifically what he's doing here in this image is he has what looks like a feed line for a Bluetooth antenna. And this BLE line is being matched with a... looks like a PI filter going along this loop here, and then we've got a capacitor here, looks like for AC coupling going into the antenna feed line. So this is all in the coplanar arrangement. The question says, "Normally the footprints of the lump components such as capacitors, inductors, or resistors, are more thicker than the trace width. For example, in the below circuit." And here he's saying he has to control the impedance of this particular coplanar waveguide trace. So, what this question is actually asking is, "How do you maintain control impedance on a transmission line or a coplanar waveguide in this case, when you have to put some components along the transmission line for purposes like impedance matching or filtering?" This is a case where in this particular question, we're looking at a PI matching filter, but you might also come across this in AC coupling caps. So, such as on like a PCIe trace. That's what we're gonna look at today. So to answer this question, we need to look back at the concept of input impedance. The question here is, we have a discontinuity along the transmission line, and we wanna know how does this discontinuity, in this case in the form of some component, affect the input impedance. So, if we go back to the input impedance equation, we have Z in equals a characteristic impedance, and then this multiplied by this big fraction. So here we have the load impedance, again the characteristic impedance. Here we have the hyperbolic tangent function, and inside the hyperbolic tangent function, we have an important quantity. We have our propagation constant and then the length of this section. Here we just kind of swap ZL and...
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