diff --git a/docs/assets/slides/l07_vreg.pdf b/docs/assets/slides/l07_vreg.pdf new file mode 100644 index 0000000..2bf4a7b Binary files /dev/null and b/docs/assets/slides/l07_vreg.pdf differ diff --git a/docs/assets/slides/l08_pll.pdf b/docs/assets/slides/l08_pll.pdf new file mode 100644 index 0000000..a2cd25a Binary files /dev/null and b/docs/assets/slides/l08_pll.pdf differ diff --git a/docs/assets/slides/l09_osc.pdf b/docs/assets/slides/l09_osc.pdf new file mode 100644 index 0000000..e42ee3d Binary files /dev/null and b/docs/assets/slides/l09_osc.pdf differ diff --git a/docs/assets/slides/l10_lpradio.pdf b/docs/assets/slides/l10_lpradio.pdf new file mode 100644 index 0000000..33b776e Binary files /dev/null and b/docs/assets/slides/l10_lpradio.pdf differ diff --git a/lectures/l10_lpradio.md b/lectures/l10_lpradio.md index 2141695..4d9a448 100644 --- a/lectures/l10_lpradio.md +++ b/lectures/l10_lpradio.md @@ -44,6 +44,8 @@ Let's make a radio (or at least, let's **pretend**) @@ -441,7 +441,7 @@ Assume we have a polycrystaline GaN material with polarized domains. If we measu If we apply stress, however, all the domains inside the material will shift. Now the free charges do not exactly cancel the electric field in the material, the free charges are in the wrong place. If we have a material with low conductivity, then it will take time for the free charges to redistribute. As such, for a while, we can measure an voltage across the material. -Assuming the above explanation is true, then there should not be piezoelectric materials with high conductivity, and indeed, most peizoelectric materials have resistance of [$10^{12}$ to $10^{14}$ Ohm](https://www.f3lix-tutorial.com/piezo-materials). +Assuming the above explanation is true, then there should not be piezoelectric materials with high conductivity, and indeed, most piezoelectric materials have resistance of [$10^{12}$ to $10^{14}$ Ohm](https://www.f3lix-tutorial.com/piezo-materials). Vibrations on a piezoelectric material will result in a AC voltage across the surface, which we can harvest. --> @@ -481,14 +481,30 @@ An example of piezoelectric energy harvester can be found in [A Fully Integrated ## "Near field" harvesting -Near Field Communcation (NFC) operates at close physical distances +Near Field Communication (NFC) operates at close physical distances ![left fit](https://upload.wikimedia.org/wikipedia/commons/thumb/5/5d/FarNearFields-USP-4998112-1.svg/618px-FarNearFields-USP-4998112-1.svg.png) -Reactive near field or inductive near field + +Reactive near field or inductive near field $$ \text{Inductive} < \frac{\lambda}{2 \pi}$$ + + --- |Standard|Frequency [MHz] | Inductive [m]| @@ -498,7 +514,6 @@ $$ \text{Inductive} < \frac{\lambda}{2 \pi}$$ |Qi| 0.205 | 232| |Bluetooth| 2400 | 0.02| - --- ## Ambient RF Harvesting @@ -608,8 +623,6 @@ tens to hundreds of volts. The key circuit challenge is the rectifier, and the high voltage output of the triboelectric generator. - - --> --- @@ -622,14 +635,40 @@ for more details. --- + + ![fit](https://ieeexplore.ieee.org/mediastore_new/IEEE/content/media/4/9546917/9441315/yoo6ab-3080383-large.gif) --- + + ![fit](https://ieeexplore.ieee.org/mediastore_new/IEEE/content/media/4/9546917/9441315/yoo1ab-3080383-large.gif) --- + + ![inline fit](https://ieeexplore.ieee.org/mediastore_new/IEEE/content/media/4/9546917/9441315/yoo2-3080383-large.gif)