[Twitter] Download of articles

[arisboch]

Twitter did introduce some time ago the (premium) function of publishing longer articles. The URL of an article looks the same at first glance, but when I try to download it, it just downloads a text tweet (if one has configured gallery-dl to download them) with the real URL, which gallery-dl doesn't accept.
Would it be possible (and practicable) to implement downloading these articles (as a PDF or more)?

Here are a few examples:

https://x.com/i2cjak/status/2013081545259553196
https://x.com/i2cjak/status/2012552153479389277
https://x.com/SceneinCinema/status/2014564610003894378

[mikf]

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        "title": "i2cjak explains capacitors, decoupling and otherwise",
        "preview_text": "A capacitor is one of four fundamental circuit elements, a platonic solid governed by a few equations (depending on if you're working in time-domain/meatspace or Fourier's Fucky Frequency Funhouse)\ni",
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              "text": "A capacitor is one of four fundamental circuit elements, a platonic solid governed by a few equations (depending on if you're working in time-domain/meatspace or Fourier's Fucky Frequency Funhouse)",
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              "text": "i = C \\frac{dv}{dt}",
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              "text": "Z = \\frac{1}{j \\omega C}",
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              "text": "WHAT IS I2CJAK EVEN TALKING ABOUT HERE? ",
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              "text": "The first expression (time domain) explains that the current through a capacitor is proportional to the change in voltage over time. As the voltage changes, the current through it changes! Capacitance is the value we assign to this relationship and is measured in \"Farads\" (named after Michael Faraday). ",
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              "text": "Imagine that you are a funny little digital IC and you are drawing 1mA of current at 3.3V. Your effective \"resistance\" as governed by Ohm's law is 3.3kR. Now you have a big 100mA current spike and your effective resistance goes to 33R. HUGE. A STEP CHANGE IN CURRENT SINKING CAPACITY. The capacitor sees this attempt to change the voltage, the possible drooping of the supply rail and begins dumping charge back to the supply rail to maintain the voltage at its previous level. It actively resists voltage droop. The same is true when the opposite happens and the effective resistance is suddenly much higher. It will shunt a little bit of current to ground.",
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              "text": "The second expression has a few more inventors (https://en.wikipedia.org/wiki/Electrical_impedance) but is a WACKY frequency domain transformation of the previous equation. Sort of. Z is \"impedance\" or \"AC resistance.\" If you've done circuit analysis with resistors like this...",
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              "text": "You'd know that the output voltage of this divider is given by",
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              "text": "V_{out} = V_{in} \\frac{R2}{R1+R2}",
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              "text": "This applies for AC or DC signals. A capacitor (and inductor, for that matter) has an \"impedance\" (again, just special resistance) that decreases as frequency increases. Let's try this same circuit but with a capacitor...",
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              "text": "WOW! It is also a voltage divider for AC? Insane. You can use this same expression to explain how RC filters work. The resistor attenuates a bit, the capacitor is selective about what frequencies it attenuates. The other variables, Omega and j, are frequency (in radians) and the imaginary constant (sqrt(-1). There are complex (haha) reasons that j is used here. Look into rotating phasors. It's just a more convenient way to handle this stuff. It also explains that a capacitor is a short to AC (very low resistance), an open circuit (infinite resistance) to DC. Just as I predicted. I am smart.",
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              "text": "This is important! For decoupling capacitors and digital electronics, you want the MOST STABLE DC voltage possible. You want to SHUNT the AC component of your power supply (often called \"noise\") to ground as FAST as possible. For AC, high frequency noise, the impedance presented by a decoupling capacitor is almost zero! For DC, it is (essentially) infinite!",
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              "text": "Somewhat related is the inductor, whose impedance is governed by",
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              "text": "Z = j \\omega L",
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              "text": "An inductor's impedance INCREASES as frequency increases. Huh. That is interesting! It's almost like the inductor and capacitor are... mirrors of each other? Just briefly look at the time domain expression too.",
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              "text": "v = L \\frac{di}{dt}",
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              "text": "Weird. Anyways, this is about capacitors. WHY ARE WE TALKING ABOUT INDUCTORS?",
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              "text": "Capacitors and inductors create resonant circuits at certain frequencies. ",
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              "text": "It's a system with inertia. That's all it is. Take a diffeq class if you want more info, sorry anon.",
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              "text": "Okay but who gives a fuck? I don't have any inductors Mr. i2cjak. That's where you ARE WRONG, DIRTY SOFTWARE ENGINEER! The inductors are all around us, wherever there is current moving through something there is inductance. Here is a more realistic model of a capacitor, different from our little BABY ideal capacitor model we used before.",
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              "text": "Our AC short to ground is not an AC short to ground anymore!!! Some digital signal on your PCB is going to exceed the ~25MHz resonant frequency of a 100nF 0603 capacitor (assuming idk 0.4nH of inductance or something close) and make your capacitor useless. This is the GREAT benefit of adding multiple caps in parallel. Capacitors in parallel ADD together, inductors and resistors in parallel are reduced following the parallel operator (||). You'll often see these graphs from manufacturers that explain the resonant frequencies of specific caps.",
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              "text": "How can you combat this sudden rise in impedance at higher frequencies? Adding multiple capacitors of the same value in parallel, using larger capacitors for the same ESL (series inductance is mostly a product of package size). ESR is also important, but has prerequisite knowledge in signal processing (see: poles of transfer functions). Sometimes more ESR can even be better! Mixing low ESR caps with high ESR caps can reduce noise, as can adding a low value series resistor in series with an MLCC. (Nobody actually does that though.) There are OTHER CONSIDERATIONS beyond this ESL/ESR issue that force you into certain directions...",
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              "text": "Capacitors are REAL things in the REAL world, and multi-layer ceramic capacitors (MLCCs) like these have a few unfortunate properties. For one, they have a maximum operating voltage. Exceed this and they will turn into dead shorts. This operating voltage is ONLY a maximum that is guaranteed to not SHORT! An MLCC's effective capacitance ALSO decreases with applied DC voltage! Significantly!  ",
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              "text": "Temperature and humidity also affect this! It's crazy. So what is a STRONG gigachad engineer to do? \"Derate\" your capacitors. If the effective capacitance decreases under these conditions, then to achieve the ideal capacitance for your circuit, you must derate them. A good rule of thumb is to use a capacitor with 2x the max voltage of the expected signal. If you need to decouple a 3.3V power rail, use a capacitor with at least 6.6V rated voltage. If the device is going to be operating in a high temp environment, maybe even 4x this! Caps are pretty cheap now so this isn't a huge deal.",
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              "text": "Murata provides a webapp, \"SimSurfing\" that helps in estimating these values.",
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              "text": "OKAY YOU'RE WELCOME @kenwheeler",
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[mikf]

There is now support for downloading article media files: 98ef34a