vault backup: 2023-03-07 14:27:42
|
|
@ -12,8 +12,8 @@
|
|||
"checkpointList": [
|
||||
{
|
||||
"path": "/",
|
||||
"date": "2023-03-03",
|
||||
"size": 974036
|
||||
"date": "2023-03-07",
|
||||
"size": 977638
|
||||
}
|
||||
],
|
||||
"activityHistory": [
|
||||
|
|
@ -1123,6 +1123,10 @@
|
|||
{
|
||||
"date": "2023-03-03",
|
||||
"value": 0
|
||||
},
|
||||
{
|
||||
"date": "2023-03-07",
|
||||
"value": 3602
|
||||
}
|
||||
]
|
||||
}
|
||||
|
|
|
|||
|
|
@ -47,30 +47,6 @@
|
|||
},
|
||||
"showLogAboutPerformanceInConsole": false,
|
||||
"selectionHistoryTree": {
|
||||
"cjl/slohy": {
|
||||
"cjl/slohy": {
|
||||
"frontMatter": {
|
||||
"count": 4,
|
||||
"lastUpdated": 1674631178064
|
||||
}
|
||||
}
|
||||
},
|
||||
"Objemový tok": {
|
||||
"Objemový tok": {
|
||||
"internalLink": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1674555407566
|
||||
}
|
||||
}
|
||||
},
|
||||
"\\frac{p_2V_2}{T_2}": {
|
||||
"\\frac{p_2V_2}{T_2}": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1674557552976
|
||||
}
|
||||
}
|
||||
},
|
||||
"Dějová linka": {
|
||||
"Dějová linka": {
|
||||
"internalLink": {
|
||||
|
|
@ -79,22 +55,6 @@
|
|||
}
|
||||
}
|
||||
},
|
||||
"Kramerius": {
|
||||
"Kramerius": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1674630993511
|
||||
}
|
||||
}
|
||||
},
|
||||
"Knihkupectví": {
|
||||
"Knihkupectví": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1674631137330
|
||||
}
|
||||
}
|
||||
},
|
||||
"cjl/slohy/romantismus": {
|
||||
"cjl/slohy/romantismus": {
|
||||
"frontMatter": {
|
||||
|
|
@ -103,30 +63,6 @@
|
|||
}
|
||||
}
|
||||
},
|
||||
"hrají": {
|
||||
"hrají": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1674631807272
|
||||
}
|
||||
}
|
||||
},
|
||||
"Německé": {
|
||||
"Německé": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1674632124708
|
||||
}
|
||||
}
|
||||
},
|
||||
"Šárka Pražáková": {
|
||||
"Šárka Pražáková": {
|
||||
"internalLink": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1674632664293
|
||||
}
|
||||
}
|
||||
},
|
||||
"teplo": {
|
||||
"teplo": {
|
||||
"currentFile": {
|
||||
|
|
@ -158,6 +94,54 @@
|
|||
"lastUpdated": 1677049823397
|
||||
}
|
||||
}
|
||||
},
|
||||
"2x-\\frac\\pi4": {
|
||||
"2x-\\frac\\pi4": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1678175910376
|
||||
}
|
||||
}
|
||||
},
|
||||
"strukturu": {
|
||||
"strukturu": {
|
||||
"currentFile": {
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||||
"count": 1,
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||||
"lastUpdated": 1678187766010
|
||||
}
|
||||
}
|
||||
},
|
||||
"stavu": {
|
||||
"stavu": {
|
||||
"currentFile": {
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||||
"count": 1,
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||||
"lastUpdated": 1678187906558
|
||||
}
|
||||
}
|
||||
},
|
||||
"k\\frac{F}S": {
|
||||
"k\\frac{F}S": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1678188601234
|
||||
}
|
||||
}
|
||||
},
|
||||
"Zákon sudnyj ljudem": {
|
||||
"Zákon sudnyj ljudem": {
|
||||
"internalLink": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1678188734961
|
||||
}
|
||||
}
|
||||
},
|
||||
"k\\in\\mathbb{Z}\\}": {
|
||||
"k\\in\\mathbb{Z}\\}": {
|
||||
"currentFile": {
|
||||
"count": 1,
|
||||
"lastUpdated": 1678194179087
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||||
}
|
||||
}
|
||||
}
|
||||
}
|
||||
}
|
||||
37
notes/.obsidian/workspace.json
vendored
|
|
@ -4,15 +4,19 @@
|
|||
"type": "split",
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||||
"children": [
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||||
{
|
||||
"id": "0111a1bc9ac38a42",
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||||
"id": "7183e76da3e7b8c7",
|
||||
"type": "tabs",
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||||
"children": [
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||||
{
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||||
"id": "3b72681fe46d1d0e",
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||||
"id": "fd3a9f5eae0d1fde",
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||||
"type": "leaf",
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||||
"state": {
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||||
"type": "empty",
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||||
"state": {}
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||||
"type": "markdown",
|
||||
"state": {
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||||
"file": "mat/Funkce/Příklady.md",
|
||||
"mode": "source",
|
||||
"source": false
|
||||
}
|
||||
}
|
||||
}
|
||||
]
|
||||
|
|
@ -73,6 +77,7 @@
|
|||
"state": {
|
||||
"type": "backlink",
|
||||
"state": {
|
||||
"file": "mat/Funkce/Příklady.md",
|
||||
"collapseAll": false,
|
||||
"extraContext": false,
|
||||
"sortOrder": "alphabetical",
|
||||
|
|
@ -89,6 +94,7 @@
|
|||
"state": {
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||||
"type": "outgoing-link",
|
||||
"state": {
|
||||
"file": "mat/Funkce/Příklady.md",
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||||
"linksCollapsed": false,
|
||||
"unlinkedCollapsed": true
|
||||
}
|
||||
|
|
@ -134,7 +140,9 @@
|
|||
"type": "leaf",
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||||
"state": {
|
||||
"type": "outline",
|
||||
"state": {}
|
||||
"state": {
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||||
"file": "mat/Funkce/Příklady.md"
|
||||
}
|
||||
}
|
||||
},
|
||||
{
|
||||
|
|
@ -208,10 +216,23 @@
|
|||
"breadcrumbs:Breadcrumbs Visualisation": false
|
||||
}
|
||||
},
|
||||
"active": "8c976bdcdc74c84c",
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||||
"active": "fd3a9f5eae0d1fde",
|
||||
"lastOpenFiles": [
|
||||
"Untitled.canvas",
|
||||
"mat/mat.md",
|
||||
"fyz/fyz.md",
|
||||
"fyz/Mechanika tekutin/Mechanika tekutin.md",
|
||||
"fyz/Deformace.md",
|
||||
"data/Pasted image 20230307123141.png",
|
||||
"data/Pasted image 20230307122841.png",
|
||||
"data/Pasted image 20230307122120.png",
|
||||
"data/Pasted image 20230307122111.png",
|
||||
"data/Pasted image 20230307122109.png",
|
||||
"data/Pasted image 20230307121956.png",
|
||||
"data/Pasted image 20230307121620.png",
|
||||
"data/Pasted image 20230307121603.png",
|
||||
"fyz/Mechanika tekutin/Termodynamika/Termodynamika.md",
|
||||
"mat/Funkce/Příklady.md",
|
||||
"Untitled.canvas",
|
||||
"mat/Funkce/Cotangens.md",
|
||||
"mat/Funkce/Tangens.md",
|
||||
"data/Pasted image 20230302110903.png",
|
||||
|
|
@ -221,11 +242,9 @@
|
|||
"psi/psi.md",
|
||||
"cjl/literatura/slohy/Romantismus/Příprava na test.md",
|
||||
"data/data.md",
|
||||
"fyz/fyz.md",
|
||||
"cjl/literatura/slohy/Romantismus/Karel Hynek Mácha.md",
|
||||
"cjl/literatura/Tropy a figury.md",
|
||||
"mat/Funkce/Goniometrické funkce.md",
|
||||
"mat/Funkce/Příklady.md",
|
||||
"fyz/Mechanika tekutin/Termodynamika/Tepelné čerpadlo.md",
|
||||
"fyz/Mechanika tekutin/Termodynamika/Chladící stroj.md"
|
||||
]
|
||||
|
|
|
|||
BIN
notes/data/Pasted image 20230307121603.png
Normal file
|
After Width: | Height: | Size: 104 KiB |
BIN
notes/data/Pasted image 20230307121620.png
Normal file
|
After Width: | Height: | Size: 88 KiB |
BIN
notes/data/Pasted image 20230307121956.png
Normal file
|
After Width: | Height: | Size: 18 KiB |
BIN
notes/data/Pasted image 20230307122109.png
Normal file
|
After Width: | Height: | Size: 12 KiB |
BIN
notes/data/Pasted image 20230307122111.png
Normal file
|
After Width: | Height: | Size: 12 KiB |
BIN
notes/data/Pasted image 20230307122120.png
Normal file
|
After Width: | Height: | Size: 20 KiB |
BIN
notes/data/Pasted image 20230307122841.png
Normal file
|
After Width: | Height: | Size: 40 KiB |
BIN
notes/data/Pasted image 20230307123141.png
Normal file
|
After Width: | Height: | Size: 19 KiB |
94
notes/fyz/Deformace.md
Normal file
|
|
@ -0,0 +1,94 @@
|
|||
# Deformace
|
||||
|
||||
## Pevné látky
|
||||
|
||||
### Krystalické
|
||||
|
||||
- monokrystaly
|
||||
- polykrystaly
|
||||
|
||||

|
||||
|
||||
### Amorfní
|
||||
|
||||
- nemají krystalickou strukturu
|
||||
- plasty, buničina, papír, vosk, sklo..
|
||||
|
||||

|
||||
|
||||
- kolem částice jsou přibližně pravidlně, dál od částice už spíše nepravidelně
|
||||
|
||||
## Druhy deformace
|
||||
|
||||
### Pružná
|
||||
|
||||
Vrátí se do původního stavu
|
||||
|
||||
### Elastická
|
||||
|
||||
Nevrátí se do původního stavu
|
||||
|
||||
### Tahem
|
||||
|
||||
Působí síly ven z tělesa
|
||||
|
||||
### Tlakem
|
||||
|
||||
Působí síly do tělesa
|
||||
|
||||
### Ohybem
|
||||
|
||||
V různých místech různými silami
|
||||

|
||||
|
||||
### Deformace smykem
|
||||
|
||||

|
||||
|
||||
### Deformace kroucením
|
||||
|
||||

|
||||
|
||||
## Normálové napětí
|
||||
|
||||
> [!SENTENCE]
|
||||
> $\sigma_n=\frac{F_p}S$
|
||||
> $[\sigma_n]=Nm^{-2}=Pa$
|
||||
|
||||
Zjednodušený model, síla působící na plochu která je vložena kolmo (v podstatě tlak u pevných věcí).
|
||||
|
||||
---
|
||||
|
||||
Jaký poloměr musí mít závěsné lano jeřábu, aby při rovnoměrném zvedání nákladu o hmotnosti 2.5t nepřekročilo normálové napětí v libovolném příčném řezu hodnotu 60MPa?
|
||||
|
||||
$\sigma_n=\frac{F_p}{\pi r^2}$
|
||||
$\sigma_n\pi r^2=F_p$
|
||||
|
||||
$r=\sqrt{\frac{F_p}{\sigma_n\pi}}$
|
||||
|
||||
---
|
||||
|
||||
|
||||
## Práce s lanem
|
||||
|
||||

|
||||
|
||||
$\Delta l=k\frac{F}S*l_0$ /$: l_0$
|
||||
$\frac{\Delta l}{l_0}=k\frac{F}S$
|
||||
$\epsilon=\frac{\Delta l}{l_0}$ relativní prodloužení (%)
|
||||
$\epsilon=k\sigma_n$
|
||||
|
||||
### Křivka deformace
|
||||
|
||||
$\sigma_n=E\epsilon$
|
||||
Hookův zákon
|
||||
> čím víc prodloužím tím větší napětí, záleží na materiálu
|
||||
|
||||
$E$ = modul pružnosti (materiálová konstanta, v tabulkách)
|
||||
$[E]=Pa$
|
||||
|
||||

|
||||
|
||||
#### Trhací zkouška
|
||||
|
||||
Trhá materiál, ukládá napětí, grafický znázornění => křivka deformace (obrázek nahoře)
|
||||
|
|
@ -7,6 +7,7 @@ type: folder_brief_live
|
|||
imagePrefix: 'data/'
|
||||
```
|
||||
%% Zoottelkeeper: Beginning of the autogenerated index file list %%
|
||||
- [[fyz/Deformace|Deformace]]
|
||||
- [[fyz/Exponencionální zápis|Exponencionální zápis]]
|
||||
- [[fyz/Jednotky SI|Jednotky SI]]
|
||||
- [[fyz/Mechanika tekutin/Mechanika tekutin|Mechanika tekutin]]
|
||||
|
|
|
|||
|
|
@ -445,3 +445,128 @@ $2n\log6+\log5=n\log7+\log56$
|
|||
$2n\log6-n\log7=\log5+\log56$
|
||||
$n(2\log6-\log7)=\log5+\log56$
|
||||
$n=\frac{\log5+\log56}{2\log6-\log7}$
|
||||
|
||||
---
|
||||
|
||||
### Goniometricke rovnice
|
||||
|
||||
52/6 a
|
||||
$\sin3x=1$
|
||||
$t=3x$
|
||||
$\sin t=1$
|
||||
$t=\pi+2k\pi$
|
||||
$t=3x$
|
||||
$3x=\pi+2k\pi$
|
||||
$x=\frac{\pi+2k\pi}3$
|
||||
|
||||
$K=\{\frac{\pi+2k\pi}3;k\in\mathbb{Z}\}$
|
||||
|
||||
52/6 b
|
||||
$\cos 10x=\frac{\sqrt2}2$
|
||||
$t=10x$
|
||||
$\cos t=\frac{\sqrt2}2$
|
||||
$t=45\degree=\frac14\pi$
|
||||
$x=t/10$
|
||||
$x=\frac{\frac14\pi}{10}$
|
||||
|
||||
$k=\frac{\pi}{40}$
|
||||
|
||||
52/6 c
|
||||
$\cos\frac52x=0$
|
||||
$t=\frac52x$
|
||||
$\cos t=0$
|
||||
$t_1=2k\pi$
|
||||
$t_2=2k\pi+\pi$
|
||||
|
||||
$K=\{2k\pi+\pi;k\in\mathbb{Z}\}$
|
||||
|
||||
$\frac52x=2k\pi$
|
||||
$x_1=\frac{4k\pi}5$
|
||||
$x_2=\frac{4k\pi+\pi}5$
|
||||
|
||||
$K=\{\frac{4k\pi+\pi}5;k\in\mathbb{Z}\}$
|
||||
|
||||
52/6 d
|
||||
$\sin(2x-\frac\pi4)=\frac{\sqrt2}2$
|
||||
$t=2x-\frac\pi4$
|
||||
$\sin t=\frac{\sqrt2}2$
|
||||
$t=45\degree=\frac14\pi$
|
||||
$\frac14\pi=2x-\frac\pi4$
|
||||
$2x=\frac14\pi+\frac14\pi$
|
||||
$x=\frac14\pi$
|
||||
$K={\frac14\pi}$
|
||||
|
||||
|
||||
71a
|
||||
|
||||
a) $2\sin(3x+\pi)=-1$
|
||||
$t=3x+\pi$
|
||||
$2sin(t)=-1$
|
||||
$\sin(t)=-\frac12$
|
||||
$t_1=210\degree C=\frac76\pi+2k\pi$
|
||||
$t_2=330\degree C=\frac{11}6\pi+2k\pi$
|
||||
|
||||
$t=3x+\pi$
|
||||
$x=\frac{t-\pi}3$
|
||||
$x_1=\frac{-\pi+\frac76\pi+2k\pi}3=\frac{\frac16\pi+2k\pi}3$
|
||||
$x_2=\frac{-\pi+\frac{11}6\pi+2k\pi}3=\frac{\frac{5}6\pi+2k\pi}3$
|
||||
|
||||
$K=\cup_{k\in\mathbb{Z}}\{\frac{\frac16\pi+2k\pi}3;\frac{\frac{5}6\pi+2k\pi}3\}$
|
||||
|
||||
b)
|
||||
|
||||
$\sin(2x)=\cos(3x)*\sin(2x)$
|
||||
|
||||
$\cos(3x)=1$
|
||||
$t=3x$
|
||||
|
||||
$\cos(t)=1$
|
||||
$t=2k\pi$
|
||||
|
||||
$x=\frac{2k\pi}3$
|
||||
|
||||
$K=\{\frac{2k\pi}3;k\in\mathbb{Z}\}$
|
||||
|
||||
alt:
|
||||
|
||||
$0=\cos(3x)\sin(2x)-\sin(2x)$
|
||||
$0=\sin(2x)(\cos(3x)-1)$
|
||||
|
||||
$\sin(2x)=0$
|
||||
$2x=k\pi$
|
||||
$x=\frac12k\pi$
|
||||
|
||||
nebo
|
||||
$cos(3x)-1=0$
|
||||
$t=3x$
|
||||
$\cos(t)=1$
|
||||
$3x=0+2k\pi$
|
||||
$x=\frac23k\pi$
|
||||
|
||||
$x=\{\frac12k\pi\}\cup\{\frac23k\pi\};k\in\mathbb{Z}$
|
||||
|
||||
---
|
||||
|
||||
$\tg^2x+2\tg x=3$
|
||||
$m^2+2m-3=0$
|
||||
$(m-1)(m+3)=0$
|
||||
$m=1$
|
||||
$m=-3$
|
||||
|
||||
$\tg x=1$
|
||||
$x=\frac{1}4\pi+k\pi$
|
||||
|
||||
$\tg x=-3$
|
||||
$x=\tg^{-1}(-3)$
|
||||
$x=-71\degree33'$
|
||||
|
||||
---
|
||||
|
||||
42/22 a
|
||||
|
||||
$\tg\frac76\pi=\frac{\sqrt3}2$
|
||||
$\tg4\pi=1$
|
||||
$\tg\frac54\pi=\frac{\sqrt2}2$
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42/22 b
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