From e39701e7053f79daa423162b7aad5b42a8d13660 Mon Sep 17 00:00:00 2001 From: vobolgus <130167730+vobolgus@users.noreply.github.com> Date: Tue, 23 Jul 2024 04:58:59 +0300 Subject: [PATCH] White dwarf sec degen-stars section significantly expanded --- data/spectrum-DA.csv | 501 ++++++++++++++++++++++++++++ data/spectrum-DB.csv | 501 ++++++++++++++++++++++++++++ sections/objects/degen-stars.tex | 107 ++++-- sections/objects/variable-stars.tex | 34 +- style/astro-notebook.plot.sty | 1 + 5 files changed, 1114 insertions(+), 30 deletions(-) create mode 100644 data/spectrum-DA.csv create mode 100644 data/spectrum-DB.csv diff --git a/data/spectrum-DA.csv b/data/spectrum-DA.csv new file mode 100644 index 0000000..008b3e6 --- /dev/null +++ b/data/spectrum-DA.csv @@ -0,0 +1,501 @@ +wavelength,flux +3800,0.604 +3805,0.625 +3810,0.658 +3815,0.701 +3819,0.731 +3824,0.74 +3829,0.642 +3834,0.623 +3839,0.561 +3843,0.711 +3848,0.714 +3853,0.707 +3858,0.816 +3863,0.734 +3867,0.683 +3872,0.677 +3877,0.571 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a/sections/objects/degen-stars.tex +++ b/sections/objects/degen-stars.tex @@ -1,35 +1,86 @@ \subsection{Вырожденные звёзды} \term{Вырожденные звезды}~--- звезды, в которых силам гравитации противостоят силы давление вырожденного газа. К таким относятся \imp{белые карлики} и \imp{нейтронные звезды}. -\begin{figure}[!h] +\begin{wrapfigure}[16]{r}{0.4\tw} \centering - \begin{minipage}[c]{0.49\tw} - \tikzsetnextfilename{light-curve-b-lyr} - \begin{tikzpicture} - \begin{axis}[ - height = 4.5cm, - width = \tw, - xlabel = {Фаза}, - ylabel = {Блеск $m$, $~^m$}, - ymax = .7, - ymin = -.1, - y dir = reverse, - xmax = 1, - xmin = .0 - ] - \addplot[smooth] table[x=t, y=m, col sep = comma]{data/light-curve-B-Lyr.csv}; - \end{axis} - \end{tikzpicture} - \end{minipage} - \hfill - \begin{minipage}[c]{0.49\tw} - \centering - \includegraphics[width = .9\tw]{b-lyr} - \end{minipage} - \caption{Кривая блеска переменной типа $\beta$\,Lyr} - \label{pic:b-lyr} - \vspace{-.8pc} + \vspace{-0.7pc} + \tikzsetnextfilename{mass-radius-wd} + \begin{tikzpicture} + \begin{axis}[ + width = 4cm, + height = 6cm, + xmax = 0.8, + xmin = -0.6, + ymax = -1.5, + ymin = -3.5, + ylabel = {$\log\frac{R}{R_{\astrosun}}$}, + xlabel = {$\log\frac{M}{M_{\astrosun}}$} + ] + \addplot [domain=-0.6:0.146, samples = 100, black, smooth]{ + ln( + ( + (1.4 / (10^x))^0.66 + - + ((10^x) / 1.4)^0.66 + )^0.5 + / 93.5 + ) / ln(10)}; + \end{axis} + \end{tikzpicture} + \caption{Зависимость масса-радиус для белых карликов} + \label{pic:mass-radius-wd} +\end{wrapfigure} + +\term{Белые карлики}~--- проэволюционировавшие звёзды лишённые собственных источников термоядерной энергии и светящие за счёт остывания. Масса белого карлика находится в диапазоне от $0.6M_{\odot}$ до $1.44 M_{\odot}$. Верхняя границы массы белого карлика называется пределом Чандрасекара, звезда с массой больше данного предела не может существовать как белый карлик. Радиус белых карликов примерно в $10^2$ раз меньше солнечного, т.е. можно считать, что $R_\text{БК} \simeq R_\oplus$. Плотность белых карликов лежит в диапазоне $10^7$\,--\,$10^{10}$~$\text{кг}/\text{м}^3$. Зависимость масса-радиус для белых карликов имеет сложную форму \lookPicRef{pic:mass-radius-wd}. Вертикальная асимптота на графике соотвтетствует пределу Чандрасекара. + +Спектры белых карликов отличаются от спектров невырожденных звёзд. Главной особенностью являются \imp{широкие линии поглощения}, также примечательно малое присутствие или вовсе отсутсвие слабых линий в спектре. Белые карлики принято выделять в отдельный спектральный класс D, а подклассов выделяют по принципу присутствия тех или иных спектральных линий в спектре. Основные подклассы: +\begin{itemize} + \item \term{DA} — водородные белые карлики, составляют около 80\% от популяции белых карликов; + \item \term{DB} — гелиевые белые карлики, составляют около 20\% от популяции белых карликов. +\end{itemize} +Остальные подклассы представляются немногочисленными. Соотношение 80:20 между подклассами DA и DB объясняется эволюцией: на последних стадиях жизни у пульсирующий красных гигантов уже присутствует вырожденное ядро окруженное водородным слоевым источником. Вследствие накопления гелия в ядре периодически происходит \imp{гелиевая вспышка} — вырождение внешних гелиевых слоёв ядра и резкое ускорение реакций. Однако после выгорания накопленного гелия происходит очередной поджог водородного слоевого источника. Красный гигант может сбросить оболочку в любой стадии, при сбросе в период гелиевой вспышки образуется гелиевый белый карлик класса DB, а если сброс произошел в период горения водородного слоевого источника — обнажится водородный белый карлик класса DA. Длительность гелиевой вспышки составляет около 20\% от длительности цикла пульсации, что и объясняет соотношение водородных и гелиевых карликов. На \picRef{pic:mass-radius-wd} приведены типовые спектры белых карликов класса DA и класса DB. + + +\begin{figure}[h!] + \centering + \tikzsetnextfilename{spectrum-wd} + \begin{tikzpicture} + \begin{groupplot}[ + group style={ + group name=wdplot, + group size=1 by 2, + vertical sep=0.5cm + }, + width=\tw, + height=5cm + ] + \nextgroupplot[ + yticklabels={}, + xticklabels={}, + xmin=3800, xmax=6200, + ytick={0, 1}, + xtick={4000, 4500, 5000, 5500, 6000}, + ] + \addplot[black, smooth] table[col sep=comma, x=wavelength, y=flux] {data/spectrum-DA.csv}; + + \nextgroupplot[ + yticklabels={}, + xmin=3800, xmax=6200, + ytick={0, 1}, + xtick={4000, 4500, 5000, 5500, 6000}, + xlabel={Длина волны $\lambda,~\,\mathring{\text{A}}$} + ] + \addplot[black, smooth] table[col sep=comma, x=wavelength, y=flux] {data/spectrum-DB.csv}; + \end{groupplot} + \path (wdplot c1r1.outer north west) + -- node[anchor=south,rotate=90] {\textsf{Относительная интенсивность}} + (wdplot c1r2.outer south west) + ; + \end{tikzpicture} + \caption{Спектр водородного и гелиевого белых карликов} + \label{pic:spectrum-wd} \end{figure} -\term{Белые карлики}~--- проэволюционировавшие звёзды лишённые собственных источников термоядерной энергии и светящие за счёт остывания. Масса белого карлика находится в диапазоне от $0.6M_{\odot}$ до $1.44 M_{\odot}$. Верхняя границы массы белого карлика называется пределом Чандрасекара, звезда с массой больше данного предела не может существовать как белый карлик. Радиус белых карликов примерно в $10^2$ раз меньше солнечного, т.е. можно считать, что $R_\text{БК} \simeq R_\oplus$. Плотность белых карликов лежит в диапазоне $10^7$\,--\,$10^{10}$~$\text{кг}/\text{м}^3$. + + \term{Нейтронная звезда}~--- сверхплотная звезда, образующаяся в результате взрыва Сверхновой. Вещество нейтронной звезды состоит в основном из нейтронов. Масса нейтронной звезды лежит в пределах от $0.1M_{\odot}$ до $2$\,--\,$2.8M_{\odot}$ (предел Оппенгеймера-Волкова). Размер данной звезды составляет лишь $10$\,--\,$20$~км, а плотность составляет $10^{16}$\,--\,$10^{18}$ $\text{кг}/\text{м}^3$. Дальнейшему гравитационному сжатию нейтронной звезды препятствует давление ядерной материи, возникающее за счёт взаимодействия нейтронов. Так как нейтронные звёзды образуются в результате коллапса массивных звёзд, то из-за сохранения момента импульса скорость их вращения может достигать $10^5$~км/с. При наличии сильного магнитного поля и быстром вращении нейтронная звзеда может наблюдаться с Земли как \term{пульсар}. diff --git a/sections/objects/variable-stars.tex b/sections/objects/variable-stars.tex index ee9e498..420c5bc 100644 --- a/sections/objects/variable-stars.tex +++ b/sections/objects/variable-stars.tex @@ -60,7 +60,7 @@ \subsection{Переменные звёзды} \term{Затменно-переменные} звёзды --- системы из двух звёзд, суммарный блеск которых периодически изменяется с течением времени. Причиной изменения блеска могут быть затмения звёзд друг другом, или изменение их формы взаимной гравитацией в тесных системах. На \picRef{pic:w-uma}\,--\,\ref{pic:b-lyr} представлены кривые блеска затменно-переменных звёзд трёх основных типов. -\begin{figure}[!h] +\begin{figure}[h!] \centering \begin{minipage}[c]{0.49\tw} \tikzsetnextfilename{light-curve-w-uma} @@ -90,7 +90,7 @@ \subsection{Переменные звёзды} \label{pic:w-uma} \end{figure} -\begin{figure}[!h] +\begin{figure}[h!] \centering \begin{minipage}[c]{0.49\tw} \tikzsetnextfilename{light-curve-b-per} @@ -117,3 +117,33 @@ \subsection{Переменные звёзды} \end{minipage} \caption{Кривая блеска переменной типа $\beta$\,Per} \end{figure} + +\begin{figure}[h!] + \centering + \begin{minipage}[c]{0.49\tw} + \tikzsetnextfilename{light-curve-b-lyr} + \begin{tikzpicture} + \begin{axis}[ + height = 4.5cm, + width = \tw, + xlabel = {Фаза}, + ylabel = {Блеск $m$, $~^m$}, + ymax = .7, + ymin = -.1, + y dir = reverse, + xmax = 1, + xmin = .0 + ] + \addplot[smooth] table[x=t, y=m, col sep = comma]{data/light-curve-B-Lyr.csv}; + \end{axis} + \end{tikzpicture} + \end{minipage} + \hfill + \begin{minipage}[c]{0.49\tw} + \centering + \includegraphics[width = .9\tw]{b-lyr} + \end{minipage} + \caption{Кривая блеска переменной типа $\beta$\,Lyr} + \label{pic:b-lyr} + \vspace{-.8pc} +\end{figure} diff --git a/style/astro-notebook.plot.sty b/style/astro-notebook.plot.sty index f2b7e7e..594f38c 100644 --- a/style/astro-notebook.plot.sty +++ b/style/astro-notebook.plot.sty @@ -1,6 +1,7 @@ \RequirePackage{pgfplots} \pgfplotsset{compat = 1.3} \usepgfplotslibrary{patchplots} +\usepgfplotslibrary{groupplots} %\RequirePackage{patchplots} \pgfplotsset{ width = 14 cm,