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| Commit | 3383a602c8252ff9b334e32ec251f8e27d815dfb (patch) | |
|---|---|---|
| Author | 2024-05-29 23:14:06 +0300 | |
| Committer | 2024-05-29 23:14:06 +0300 | |
| Files | ba187510bbd7ce734946dd45e4b259163feb9f1c | |
| uni-projects-3383a602c8252ff9b334e32ec251f8e27d815dfb.tar uni-projects-3383a602c8252ff9b334e32ec251f8e27d815dfb.tar.gz uni-projects-3383a602c8252ff9b334e32ec251f8e27d815dfb.zip | ||
| Parent | 1d7becedc3b0c87c8b38e7c59c6b482843bd83e1 (diff) | |
[OTO] Simplified calculations of last task
2 files changed, 26 insertions, 38 deletions
| -rw-r--r-- | Year 3/General theory of relativity/Project.pdf | bin | 53335 -> 51992 bytes | |||
| -rw-r--r-- | Year 3/General theory of relativity/Project.tex | 64 |
diff --git a/Year 3/General theory of relativity/Project.pdf b/Year 3/General theory of relativity/Project.pdf Binary files differindex 0c2dfc2..bd8a456 100644 --- a/Year 3/General theory of relativity/Project.pdf +++ b/Year 3/General theory of relativity/Project.pdf diff --git a/Year 3/General theory of relativity/Project.tex b/Year 3/General theory of relativity/Project.tex index 6250fca..195b2ae 100644 --- a/Year 3/General theory of relativity/Project.tex +++ b/Year 3/General theory of relativity/Project.tex @@ -264,20 +264,20 @@ $0\text{MI}080002\mathbf{\underline{8}}$, следователно ще разг Ще използваме, че: \begin{itemize} - \item гравитационния радиус на слънцето е $\alpha_\text{Слънце} = 2.953$ km + \item гравитационния радиус на слънцето е $\alpha_\text{Слънце} \approx 2.9$ km \item средния радиус на Нептун е $r_\text{средно,Нептун} = 4.5 \cdot 10^9$ km - \item ексцентритетът на Нептун е $e = 0.008678$ - \item Нептун прави една обиколка (около Слънцето) на всеки $164.8$ години + \item ексцентритетът на Нептун е $e \approx 0.008$ + \item Нептун прави една обиколка (около Слънцето) на всеки $164$ години \end{itemize} По формулата на Айнщайн: \begin{align*} - \Delta \varphi & \approx \frac{3 \pi \alpha_\text{Слънце}}{r_\text{средно,Нептун} (1 - e^2)} \approx \frac{3 \pi \cdot 2.953}{4.5 \cdot 10^9 \cdot (1 - 0.008678^2)} \approx \pi \frac{8859 \cdot 10^{-3}}{4.5 \cdot 10^9 \cdot (1 - 0.000075307684)} \\ - & \approx \pi \frac{8859}{4.5 \cdot 10^{12} \cdot 0.999924692316} \approx 6.1852145315485203527881859... \cdot 10^{-9} \; \text{ радиани на обиколка} \\ + \Delta \varphi & \approx \frac{3 \pi \alpha_\text{Слънце}}{r_\text{средно,Нептун} (1 - e^2)} \approx \frac{3 \pi \cdot 2.9}{4.5 \cdot 10^9 \cdot (1 - 0.008^2)} = \pi \frac{87}{45 \cdot 10^9 \cdot (1 - 0.000064)} \\ + & \approx \pi \frac{1.9333}{10^{9} \cdot 0.999936} \approx \pi \cdot 1.9334 \cdot 10^{-9} \; \text{ радиани на обиколка} \\ & \text{Превръщайки към дъгови секунди на 100 години}: \\ - & \approx 0.0000000061852145315485203527881859... \cdot \frac{180}{\pi} 3600 \cdot \frac{100}{164.8} \\ - & \approx 0.00077414567775884732... \, '' + & = \cancel{\pi} \cdot 1.9334 \cdot 10^{-9} \cdot \frac{180}{\cancel{\pi}} 3600 \cdot \frac{100}{164} = 1.9334 \cdot 10^{-9} \cdot 18 \cdot 36 \cdot 10^3 \cdot \frac{10^2}{164} \\ + & = 1.9334 \cdot 10^{-4} \cdot 8 \cdot 9 \cdot 9 \cdot \frac{1}{164} = 1.9334 \cdot 10^{-4} \cdot \frac{81}{20.5} \approx 0.00076 \, '' \end{align*} По точната формула: @@ -287,51 +287,39 @@ $0\text{MI}080002\mathbf{\underline{8}}$, следователно ще разг \end{align*} \begin{align*} - & r_\text{min} = (1 - e) r_\text{средно,Нептун} = (1 - 0.008678) \cdot 4.5 \cdot 10^9 = 0.991322 \cdot 4.5 \cdot 10^9 = 4.460949 \cdot 10^9 \\ - & r_\text{max} = (1 + e) r_\text{средно,Нептун} = (1 + 0.008678) \cdot 4.5 \cdot 10^9 = 1.008678 \cdot 4.5 \cdot 10^9 = 4.539051 \cdot 10^9 \\ - & \frac{\alpha_\text{Слънце}}{r_\text{min}} = \frac{2.953}{4.460949 \cdot 10^9} = \frac{2953}{4460949 \cdot 10^3} - \qquad \frac{\alpha_\text{Слънце}}{r_\text{max}} = \frac{2.953}{4.539051 \cdot 10^9} = \frac{2953}{4539051 \cdot 10^3} \\ + & r_\text{min} = (1 - e) r_\text{средно,Нептун} = (1 - 0.008) \cdot 4.5 \cdot 10^9 = 0.992 \cdot 4.5 \cdot 10^9 \approx 4.4 \cdot 10^9 \\ + & r_\text{max} = (1 + e) r_\text{средно,Нептун} = (1 + 0.008) \cdot 4.5 \cdot 10^9 = 1.008 \cdot 4.5 \cdot 10^9 \approx 4.5 \cdot 10^9 \\ + & \frac{\alpha_\text{Слънце}}{r_\text{min}} = \frac{2.9}{4.4 \cdot 10^9} = \frac{29}{44 \cdot 10^9} + \qquad \frac{\alpha_\text{Слънце}}{r_\text{max}} = \frac{2.9}{4.5 \cdot 10^9} = \frac{29}{45 \cdot 10^9} \\ \end{align*} \begin{align*} - \sqrt{1 - \frac{\alpha_\text{Слънце}}{r_\text{min}} - \frac{2 \alpha_\text{Слънце}}{r_\text{max}}} & = \sqrt{1 - \frac{2953}{4460949 \cdot 10^3} - 2 \frac{2953}{4539051 \cdot 10^3}} \\ - & = \sqrt{\frac{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3 - 2953 \cdot 4539051 - 2 \cdot 2953 \cdot 4460949}{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3}} \\ - & = \sqrt{\frac{1}{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3}} \sqrt{20248474979648817603} + \sqrt{1 - \frac{\alpha_\text{Слънце}}{r_\text{min}} - \frac{2 \alpha_\text{Слънце}}{r_\text{max}}} & = \sqrt{1 - \frac{29}{44 \cdot 10^9} - 2 \frac{29}{45 \cdot 10^9}} \\ + & = \sqrt{\frac{44 \cdot \cancel{10^9} \cdot 45 \cdot 10^9 - 29 \cdot 45 \cdot \cancel{10^9} - 2 \cdot 29 \cdot 44 \cdot \cancel{10^9}}{44 \cdot \cancel{10^9} \cdot 45 \cdot 10^9}} \\ + & = \sqrt{\frac{1980 \cdot 10^9 - 1305 - 2 \cdot 1276}{1980 \cdot 10^9}} \\ + & = \sqrt{\frac{1980 \cdot 10^{9} - 3857}{1980 \cdot 10^{9}}} \approx 0.99999999902 \end{align*} \begin{align*} - \sqrt{1 - \frac{2 \alpha_\text{Слънце}}{r_\text{min}} - \frac{\alpha_\text{Слънце}}{r_\text{max}}} & = \sqrt{1 - 2 \frac{2953}{4460949 \cdot 10^3} - \frac{2953}{4539051 \cdot 10^3}} \\ - & = \sqrt{\frac{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3 - 2 \cdot 2953 \cdot 4539051 - 2953 \cdot 4460949}{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3}} \\ - & = \sqrt{\frac{1}{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3}} \sqrt{20248474979418182397} + \sqrt{1 - \frac{2 \alpha_\text{Слънце}}{r_\text{min}} - \frac{\alpha_\text{Слънце}}{r_\text{max}}} & = \sqrt{1 - 2 \frac{29}{44 \cdot 10^9} - \frac{29}{45 \cdot 10^9}} \\ + & = \sqrt{\frac{44 \cdot \cancel{10^9} \cdot 45 \cdot 10^9 - 2 \cdot 29 \cdot 45 \cdot \cancel{10^9} - 29 \cdot 44 \cdot \cancel{10^9}}{44 \cdot \cancel{10^9} \cdot 45 \cdot 10^9}} \\ + & = \sqrt{\frac{1980 \cdot 10^9 - 2 \cdot 1305 - 1276}{1980 \cdot 10^9}} \\ + & = \sqrt{\frac{1980 \cdot 10^{9} - 3886}{1980 \cdot 10^{9}}} \approx 0.99999999901 \end{align*} \begin{align*} & M \left( \sqrt{1 - \frac{\alpha_\text{Слънце}}{r_\text{min}} - \frac{2 \alpha_\text{Слънце}}{r_\text{max}}}, \sqrt{1 - \frac{2 \alpha_\text{Слънце}}{r_\text{min}} - \frac{\alpha_\text{Слънце}}{r_\text{max}}} \right) \\ - & = M \left( \sqrt{\frac{1}{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3}} \sqrt{20248474979648817603} \; , \right. \\ - & \qquad\quad \left. \sqrt{\frac{1}{4460949 \cdot 10^3 \cdot 4539051 \cdot 10^3}} \sqrt{20248474979418182397} \right) \\ - & = \sqrt{\frac{1}{4460949 \cdot 4539051 \cdot 10^{6}}} M \left( \sqrt{20248474979648817603}, \sqrt{20248474979418182397} \right) \\ - & = 2.2223059021530026666489... \cdot 10^{-10} \cdot - 4.4998305500911364873496... \cdot 10^9 \\ - & = 0.999999999015592532735669488682770254067475544... = M_\text{стойност} + & \approx M (0.99999999902, 0.99999999901) \\ + & = M \left(\sqrt{0.99999999902 \cdot 0.99999999901}, \frac{0.99999999902 + 0.99999999901}{2} \right) \\ + & \approx M(0.999999999014, 0.999999999015) \\ + & \approx 0.9999999990145 \end{align*} \begin{align*} - \frac{2 \pi}{M_\text{стойност}} = 6.28318531336480101760716936984332803180490350... -\end{align*} - -\begin{align*} - \Delta \varphi & = 6.28318531336480101760716936984332803180490350... - 2 \pi \\ - & = 6.1852145406818826032843222... \cdot 10^{-9} \; \text{ радиани на обиколка} \\ + \Delta \varphi & = \frac{2 \pi}{0.9999999990145} - 2 \pi = 2 \pi \left( \frac{1}{0.9999999990145} - 1 \right) \approx 2 \pi \cdot 0.00000000098 \; \text{ радиани на обиколка} \\ & \text{Превръщайки към дъгови секунди на 100 години}: \\ - & = 0.0000000061852145406818826032843222... \cdot \frac{180}{\pi} 3600 \cdot \frac{100}{164.8} \\ - & = 0.00077414567890198518... \, '' -\end{align*} - -Приближението на Айнщайн е достатъчно точно за 11 цифри след запетаята (различаващите цифри са удебелени и подчертани): - -\begin{align*} - \text{По Айнщайн: } & \Delta \varphi \approx 0.00077414567\mathbf{\underline{775884732}}... \, '' \\ - \text{По точната: } & \Delta \varphi = 0.00077414567\mathbf{\underline{890198518}}... \, '' + & = 2 \cancel{\pi} \cdot 0.00000000098 \cdot \frac{180}{\cancel{\pi}} 3600 \cdot \frac{100}{164} = 0.00000000196 \cdot 10^{5} \cdot \frac{81}{20.5} \\ + & \approx 0.00077 \, '' \end{align*} \end{document}
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