This commit is contained in:
guoyz 2025-06-01 13:36:24 +08:00
commit 27ad36d05f
4867 changed files with 2437 additions and 2308 deletions

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.DS_Store vendored

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@ -1,12 +1,12 @@
{ {
"id": "obsidian-excalidraw-plugin", "id": "obsidian-excalidraw-plugin",
"name": "Excalidraw", "name": "Excalidraw",
"version": "2.9.2", "version": "2.9.2",
"minAppVersion": "1.1.6", "minAppVersion": "1.1.6",
"description": "An Obsidian plugin to edit and view Excalidraw drawings", "description": "An Obsidian plugin to edit and view Excalidraw drawings",
"author": "Zsolt Viczian", "author": "Zsolt Viczian",
"authorUrl": "https://www.zsolt.blog", "authorUrl": "https://www.zsolt.blog",
"fundingUrl": "https://ko-fi.com/zsolt", "fundingUrl": "https://ko-fi.com/zsolt",
"helpUrl": "https://github.com/zsviczian/obsidian-excalidraw-plugin#readme", "helpUrl": "https://github.com/zsviczian/obsidian-excalidraw-plugin#readme",
"isDesktopOnly": false "isDesktopOnly": false
} }

0
.obsidian/plugins/obsidian-git/obsidian_askpass.sh vendored Executable file → Normal file
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@ -33,5 +33,6 @@
"useInternalPlugins": false "useInternalPlugins": false
}, },
"InterestingStuffs": "LiCoffee", "InterestingStuffs": "LiCoffee",
"补课": "🧑‍🏫" "补课": "🧑‍🏫",
"书籍/力学书籍": "📚"
} }

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@ -20,21 +20,21 @@ $$
where $\left[\varSigma\right]$ is a diagonal matrix containing the singular values of $[A]$ , which are $\sqrt{e i g e n\nu a l u e s\;o f\left[A\right]\left[A\right]^{T}}\;=\sqrt{e i g e n\nu a l u e s\;o f\left[A\right]^{T}\left[A\right]}\;.$ where $\left[\varSigma\right]$ is a diagonal matrix containing the singular values of $[A]$ , which are $\sqrt{e i g e n\nu a l u e s\;o f\left[A\right]\left[A\right]^{T}}\;=\sqrt{e i g e n\nu a l u e s\;o f\left[A\right]^{T}\left[A\right]}\;.$
![](images/b2c0bc757ff696893b956868f5c253bf5635452cfb9931e91b125836026cce64.jpg) ![](b2c0bc757ff696893b956868f5c253bf5635452cfb9931e91b125836026cce64.jpg)
This was derived symbolically by J. Jonkman by computing $\left[U\right]\!\!\left[V\right]^{T}$ by hand with verification in Mathematica. This was derived symbolically by J. Jonkman by computing $\left[U\right]\!\!\left[V\right]^{T}$ by hand with verification in Mathematica.
Tower Base / Platform Coordinate System Tower Base / Platform Coordinate System
![](images/88207e1709e48057eba3e20a48c5537a392d9b45b23b859db0e1ec4e12258df7.jpg) ![](88207e1709e48057eba3e20a48c5537a392d9b45b23b859db0e1ec4e12258df7.jpg)
Tower Element-Fixed Coordinate System Tower Element-Fixed Coordinate System
![](images/3242641825dce121996aa8b64d069f719111b388bf56b4d23f53af451eb49b9d.jpg) ![](3242641825dce121996aa8b64d069f719111b388bf56b4d23f53af451eb49b9d.jpg)
Tower-Top / Base Plate Coordinate System Tower-Top / Base Plate Coordinate System
![](images/e15be66677d4a32e794cee5226c75216651a32afe750bafa3f1e124e9814b9c2.jpg) ![](e15be66677d4a32e794cee5226c75216651a32afe750bafa3f1e124e9814b9c2.jpg)
Nacelle / Yaw Coordinate System${\pmb d}_{t}$ cos (qYaw) 0 sin (qYaw) b${\pmb d}_{2}$ 0 1 0 b${\pmb d}_{3}$ sin (qYaw) 0 cos (qYaw) b Nacelle / Yaw Coordinate System${\pmb d}_{t}$ cos (qYaw) 0 sin (qYaw) b${\pmb d}_{2}$ 0 1 0 b${\pmb d}_{3}$ sin (qYaw) 0 cos (qYaw) b
@ -74,7 +74,7 @@ The equation for $i^{B2}$ is similar.
Blade / Pitched Coordinate System Blade / Pitched Coordinate System
![](images/a2a9c533925e493d652a0d69730b87a5df026cde2fee0e7d5f9aaa614a8fa533.jpg) ![](a2a9c533925e493d652a0d69730b87a5df026cde2fee0e7d5f9aaa614a8fa533.jpg)
The equation for $j^{B2}$ is similar. The equation for $j^{B2}$ is similar.
@ -94,26 +94,26 @@ $$
where, where,
![](images/cf71b1f3353b9439b47212c215710ee64d1df808df03c0029378347d198cafb7.jpg) ![](cf71b1f3353b9439b47212c215710ee64d1df808df03c0029378347d198cafb7.jpg)
The equation for ${\pmb n}^{B2}(r)$ is similar. The equation for ${\pmb n}^{B2}(r)$ is similar.
Blade Element-Fixed Coordinate System Used for Calculating and Returning Aerodynamic Loads This coordinate system is coincident with $i^{B I}$ when the blade is undeflected. Blade Element-Fixed Coordinate System Used for Calculating and Returning Aerodynamic Loads This coordinate system is coincident with $i^{B I}$ when the blade is undeflected.
![](images/402bb29e7129df0062d48b3c5d723765784131fb70c72e23f07e9c78b7e694af.jpg) ![](402bb29e7129df0062d48b3c5d723765784131fb70c72e23f07e9c78b7e694af.jpg)
The equation for $m^{B2}(r)$ is similar. The equation for $m^{B2}(r)$ is similar.
Blade Element-Fixed Coordinate System Aligned with Local Aerodynamic Axes (i.e., chordline) / Trailing Edge Coordinate System Blade Element-Fixed Coordinate System Aligned with Local Aerodynamic Axes (i.e., chordline) / Trailing Edge Coordinate System
![](images/b7bec12025e6f227efffe993d420000c18ea244ff8bae921c771471511c7eeae.jpg) ![](b7bec12025e6f227efffe993d420000c18ea244ff8bae921c771471511c7eeae.jpg)
The equation for $t e^{B2}(r)$ is similar. The equation for $t e^{B2}(r)$ is similar.
Tail-Furl Coordinate System Tail-Furl Coordinate System
![](images/533bb40e8037410168158086acafc99d91b7370bfc9c854092d68c0b8bfaea2e.jpg) ![](533bb40e8037410168158086acafc99d91b7370bfc9c854092d68c0b8bfaea2e.jpg)
Tail Fin Coordinate System Tail Fin Coordinate System
![](images/326d9d71696178edb5d7849627247735ea5edae14d157ee4fcf3753eb8210851.jpg) ![](326d9d71696178edb5d7849627247735ea5edae14d157ee4fcf3753eb8210851.jpg)

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