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\author{Alexcharaon}
\pdfinfo{
  /Title (physik-q1.pdf)
  /Creator (Cheatography)
  /Author (Alexcharaon)
  /Subject (Physik Q1 Cheat Sheet)
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    {\parbox{\dimexpr\textwidth-2\fboxsep\relax}{\noindent
        \hspace*{-6pt}\includegraphics[width=5.8cm]{/web/www.cheatography.com/public/images/cheatography_logo.pdf}}
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\begin{tabulary}{11cm}{L}
    \vspace{-2pt}\large{\bf{\textcolor{DarkBackground}{\textrm{Physik Q1 Cheat Sheet}}}} \\
    \normalsize{by \textcolor{DarkBackground}{Alexcharaon} via \textcolor{DarkBackground}{\uline{cheatography.com/219101/cs/48477/}}}
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\noindent
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  \mymulticolumn{2}{p{5.377cm}}{\bf\textcolor{white}{Cheatographer}}  \\
  \vspace{-2pt}Alexcharaon \\
  \uline{cheatography.com/alexcharaon} \\
  \end{tabulary}
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  \mymulticolumn{1}{p{5.377cm}}{\bf\textcolor{white}{Cheat Sheet}}  \\
   \vspace{-2pt}Published 1st October, 2026.\\
   Updated 1st October, 2026.\\
   Page {\thepage} of \pageref{LastPage}.
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  %\includegraphics[width=48px,height=48px]{dave.jpeg}
  Measure your website readability!\\
  www.readability-score.com
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\begin{document}
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\begin{tabularx}{17.67cm}{X}
\SetRowColor{DarkBackground}
\mymulticolumn{1}{x{17.67cm}}{\bf\textcolor{white}{Physik Q1}}  \tn
% Row 0
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{{\bf{Ladungstr{\"a}ger in elektrischen und magnetischen Feldern}}} \tn 
% Row Count 2 (+ 2)
% Row 1
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- gleiche Ladungen sto{\ss}en sich ab, unterschiedliche Ladungen ziehen sich an} \tn 
% Row Count 4 (+ 2)
% Row 2
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- "+" -{}-\textgreater{} "-"} \tn 
% Row Count 5 (+ 1)
% Row 3
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 5 (+ 0)
% Row 4
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{{\bf{Elektrische Ladung "Q" ("q")}}} \tn 
% Row Count 6 (+ 1)
% Row 5
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- entweder positiv "+" oder negativ "-"} \tn 
% Row Count 7 (+ 1)
% Row 6
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- ein neutraler K{\"o}rper besitzt gleich viele {\emph{positive}} wie {\emph{negative Ladungstr{\"a}ger}}} \tn 
% Row Count 9 (+ 2)
% Row 7
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- negative Ladung (Q\textless{}0) ≙ Elektronenüberschuss} \tn 
% Row Count 10 (+ 1)
% Row 8
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- positive Ladung (Q\textgreater{}0) ≙ Elektronenmangel} \tn 
% Row Count 11 (+ 1)
% Row 9
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- bei {\emph{elektrischen Ladungen}} wirkt eine {\emph{elektrische Kraft}}} \tn 
% Row Count 13 (+ 2)
% Row 10
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- gleichnamige Ladungen sto{\ss}en sich ab \{\{nl\}\} - ungleichnamige Ladungen ziehen sich an} \tn 
% Row Count 15 (+ 2)
% Row 11
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{Einheit der elektrischen Ladung:} \tn 
% Row Count 16 (+ 1)
% Row 12
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- Flie{\ss}t ein Strom I der St{\"a}rke 1 A (Ampère) für 1 Sekunde, so wird eine Ladungsmenge Q von 1 C (Coulomb) übertragen:} \tn 
% Row Count 19 (+ 3)
% Row 13
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{-\textgreater{} 1 C = 1 A * 1 s \{\{nl\}\} bzw. \{\{nl\}\} Ladung = Stromst{\"a}rke * Zeit} \tn 
% Row Count 21 (+ 2)
% Row 14
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{1 {[}Q{]} = 1 C (Coulomb)} \tn 
% Row Count 22 (+ 1)
% Row 15
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 22 (+ 0)
% Row 16
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{{\bf{Influenz}}} \tn 
% Row Count 23 (+ 1)
% Row 17
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- Umverteilung der elektrischen Ladung eines Objekts durch ein elektrisches Feld} \tn 
% Row Count 25 (+ 2)
% Row 18
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- durch das elektrische Feld wird die Bewegung von Ladungstr{\"a}gern initiiert} \tn 
% Row Count 27 (+ 2)
% Row 19
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{Bei einem Elektroskop: \{\{nl\}\} - "geringe Ladung" führt zu geringem Ausschlag \{\{nl\}\} - "gro{\ss}e Ladung" führt zu starkem Ausschlag} \tn 
% Row Count 30 (+ 3)
\end{tabularx}
\par\addvspace{1.3em}

\begin{tabularx}{17.67cm}{X}
\SetRowColor{DarkBackground}
\mymulticolumn{1}{x{17.67cm}}{\bf\textcolor{white}{Physik Q1 (cont)}}  \tn
% Row 20
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{-\textgreater{} die 'Kraft' des elektrischen Feldes geht mit der St{\"a}rke der Ladung einher} \tn 
% Row Count 2 (+ 2)
% Row 21
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 2 (+ 0)
% Row 22
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{{\bf{Die elektrische Feldst{\"a}rke E\textasciicircum{}-\textgreater{}\textasciicircum{}}}} \tn 
% Row Count 3 (+ 1)
% Row 23
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- E\textasciicircum{}-\textgreater{}\textasciicircum{}  = F\textasciicircum{}-\textgreater{}\textasciicircum{}/Q} \tn 
% Row Count 4 (+ 1)
% Row 24
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- die elektrische Feldst{\"a}rke E ist der Quotient (und somit die Proportionalit{\"a}tskonstante) aus der elektrischen Kraft F, die auf eine Ladung Q wirkt} \tn 
% Row Count 7 (+ 3)
% Row 25
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{{[}E\textasciicircum{}-\textgreater{}\textasciicircum{}{]} = N/C (Newton / Coulomb)} \tn 
% Row Count 8 (+ 1)
% Row 26
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 8 (+ 0)
% Row 27
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 8 (+ 0)
% Row 28
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{{\bf{Die wirkweise eines elektrischen Feldes}}} \tn 
% Row Count 9 (+ 1)
% Row 29
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- Die Feldst{\"a}rke nimmt nach au{\ss}en hin ab} \tn 
% Row Count 10 (+ 1)
% Row 30
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- "homogenes elektrisches Feld" \{\{nl\}\} -\textgreater{} die Feldst{\"a}rke ist im inneren Bereich überall gleich gro{\ss} (-\textgreater{} homogen)} \tn 
% Row Count 13 (+ 3)
% Row 31
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{\{\{popup="https://www.lernhelfer.de/sites/default/files/styles/lightbox/public/lexicon/image/BWS-PHY-0104-09.gif?itok=c5vYZzhf"\}\}Beispielfoto\{\{/link\}\} \{\{nl\}\} -\textgreater{} durch beide Ladungen wird jeweils eine Kraft F\textasciicircum{}-\textgreater{}\textasciicircum{}\textasciitilde{}1\textasciitilde{} und F\textasciicircum{}-\textgreater{}\textasciicircum{}\textasciitilde{}2\textasciitilde{} auf die positive Probeladung ausgeübt. Mit einem Kr{\"a}fteparallelogramm l{\"a}sst sich die resultierende Kraft F\textasciicircum{}-\textgreater{}\textasciicircum{}\textasciitilde{}res\textasciitilde{} ermitteln. Die Feldlinien geben also immer die Kraft auf eine positive Probeladung an.} \tn 
% Row Count 22 (+ 9)
% Row 32
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{\{\{link="https://media.springernature.com/lw685/springer-static/image/chp\%3A10.1007\%2F978-3-662-67936-4\_18/MediaObjects/155876\_9\_De\_18\_Fig22\_HTML.png"\}\}Elektrisches Feld mit zwei positiven Punktladungen} \tn 
% Row Count 27 (+ 5)
% Row 33
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{Regeln für das Zeichnen von Punktladungen:} \tn 
% Row Count 28 (+ 1)
% Row 34
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- Feldlinien verlaufen von "+" zu "-"} \tn 
% Row Count 29 (+ 1)
% Row 35
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- Feldlinien stehen {\bf{immer}} senkrecht zur Leiteroberfl{\"a}che} \tn 
% Row Count 31 (+ 2)
\end{tabularx}
\par\addvspace{1.3em}

\begin{tabularx}{17.67cm}{X}
\SetRowColor{DarkBackground}
\mymulticolumn{1}{x{17.67cm}}{\bf\textcolor{white}{Physik Q1 (cont)}}  \tn
% Row 36
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- Feldlinien schneiden sich {\bf{nie}}} \tn 
% Row Count 1 (+ 1)
% Row 37
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- Feldlinien sind nur ein {\bf{Hilfsmittel}} zum {\bf{Visualisieren}} und {\bf{nicht real}}} \tn 
% Row Count 3 (+ 2)
% Row 38
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- die Dichte der Feldlinien ist proportional zur elektrischen Feldst{\"a}rke E} \tn 
% Row Count 5 (+ 2)
% Row 39
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{Wovon h{\"a}ngt das elektrische Feld ab:} \tn 
% Row Count 6 (+ 1)
% Row 40
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- Distanz der Ladungstr{\"a}ger} \tn 
% Row Count 7 (+ 1)
% Row 41
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- St{\"a}rke der Ladungen} \tn 
% Row Count 8 (+ 1)
% Row 42
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- Medium, in dem sich die Ladungen befinden} \tn 
% Row Count 9 (+ 1)
% Row 43
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 9 (+ 0)
% Row 44
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{{\bf{das Gesetz von Coulomb}}} \tn 
% Row Count 10 (+ 1)
% Row 45
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{- F \textbackslash{}\textasciitilde{} q} \tn 
% Row Count 11 (+ 1)
% Row 46
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- F \textbackslash{}\textasciitilde{} r\textasciicircum{}-2\textasciicircum{} bzw. F \textbackslash{}\textasciitilde{} 1/r\textasciicircum{}2\textasciicircum{}} \tn 
% Row Count 12 (+ 1)
% Row 47
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{-\textgreater{} F\textbackslash{}\textasciitilde{} k * ((q\textasciitilde{}1\textasciitilde{} * q\textasciitilde{}2\textasciitilde{}) / r\textasciicircum{}2\textasciicircum{}) \{\{nl\}\} (k = Proportionalit{\"a}tskonstante)} \tn 
% Row Count 14 (+ 2)
% Row 48
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{=\textgreater{} F\textasciitilde{}er\textasciitilde{} = k * ((q\textasciitilde{}1\textasciitilde{} * q\textasciitilde{}2\textasciitilde{}) / r\textasciicircum{}2\textasciicircum{}) \{\{nl\}\} \textless{}=\textgreater{} F\textasciitilde{}er\textasciitilde{}*r\textasciicircum{}2\textasciicircum{} = k * q\textasciitilde{}1\textasciitilde{} * q\textasciitilde{}2\textasciitilde{} \{\{nl\}\} \textless{}=\textgreater{} k = (F\textasciitilde{}er\textasciitilde{}*r\textasciicircum{}2\textasciicircum{}) / (q\textasciitilde{}1\textasciitilde{}*q\textasciitilde{}2\textasciitilde{})} \tn 
% Row Count 17 (+ 3)
% Row 49
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{(Kursergebnis \{\{nl\}\}F\textasciitilde{}er\textasciitilde{} = 280,861 N \{\{nl\}\} q\textasciitilde{}1\textasciitilde{} = 10\textasciicircum{}-5\textasciicircum{} C \{\{nl\}\} q\textasciitilde{}2\textasciitilde{} = 5*10\textasciicircum{}-6\textasciicircum{} C \{\{nl\}\} r = 0,04 m \{\{nl\}\} \{\{nl\}\} =\textgreater{} 280,861 = k * ((10\textasciicircum{}-5\textasciicircum{} * 5*10\textasciicircum{}-6\textasciicircum{})/0,04\textasciicircum{}2\textasciicircum{}) \{\{nl\}\} \textless{}=\textgreater{} k = ((280,861 * 0,04\textasciicircum{}2\textasciicircum{})/(10\textasciicircum{}-5\textasciicircum{} * 5*10\textasciicircum{}-6\textasciicircum{})) \{\{nl\}\} =\textgreater{} k = 8,9876 * 10\textasciicircum{}9\textasciicircum{} (N * m\textasciicircum{}2\textasciicircum{}) / C\textasciicircum{}2\textasciicircum{} \{\{nl\}\})} \tn 
% Row Count 23 (+ 6)
% Row 50
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{-\textgreater{} Die Kraft, die zwei kugelf{\"o}rmige bzw. punktf{\"o}rmige Ladungen q\textasciitilde{}1\textasciitilde{} \& q\textasciitilde{}2\textasciitilde{} aufeinander auswirken, ist definiert durch F = k*(q\textasciitilde{}1\textasciitilde{} * q\textasciitilde{}2\textasciitilde{})/r\textasciicircum{}2\textasciicircum{} \{\{nl\}\} k ist dabei die Coulomb-Konstante. Diese ist definiert durch "k = 1/(4π*ε\textasciitilde{}0\textasciitilde{}) ≈ 8,99*10\textasciicircum{}9\textasciicircum{} (N * m\textasciicircum{}2\textasciicircum{}) / C\textasciicircum{}2\textasciicircum{} \{\{nl\}\} ε\textasciitilde{}0\textasciitilde{} = elektrische Feldkonstante} \tn 
% Row Count 30 (+ 7)
\end{tabularx}
\par\addvspace{1.3em}

\begin{tabularx}{17.67cm}{X}
\SetRowColor{DarkBackground}
\mymulticolumn{1}{x{17.67cm}}{\bf\textcolor{white}{Physik Q1 (cont)}}  \tn
% Row 51
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 0 (+ 0)
% Row 52
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{Elektrische Feldkonstante:} \tn 
% Row Count 1 (+ 1)
% Row 53
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{ε\textasciitilde{}0\textasciitilde{}*r\textasciicircum{}2\textasciicircum{} = (q\textasciitilde{}1\textasciitilde{}*q\textasciitilde{}2\textasciitilde{})/(4π*F)} \tn 
% Row Count 2 (+ 1)
% Row 54
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{ε\textasciitilde{}0 Lit\textasciitilde{} ≈ 8,854*10\textasciicircum{}-12\textasciicircum{} C\textasciicircum{}2\textasciicircum{}/(N*m\textasciicircum{}2\textasciicircum{})} \tn 
% Row Count 3 (+ 1)
% Row 55
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 3 (+ 0)
% Row 56
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{{\bf{elektrische Feldst{\"a}rke in einem homogenen elektrischen Feld}}} \tn 
% Row Count 5 (+ 2)
% Row 57
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{I \textbackslash{}\textasciitilde{} U \{\{nl\}\} \& \{\{nl\}\} E \textbackslash{}\textasciitilde{} I \{\{nl\}\} =\textgreater{} E \textbackslash{}\textasciitilde{} U} \tn 
% Row Count 6 (+ 1)
% Row 58
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{die elektrische Feldst{\"a}rke E eines homogenen elektrischen Feldes ist proportional zur Spannung der beiden Ladungstr{\"a}gern U und dem Kehrwert des Abstandes zwischen den Ladungstr{\"a}gern d (1/d)} \tn 
% Row Count 10 (+ 4)
% Row 59
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{im homogenen Feld gilt also: \{\{nl\}\} E = U/d} \tn 
% Row Count 11 (+ 1)
% Row 60
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{das hei{\ss}t: \{\{nl\}\} F\textasciitilde{}el\textasciitilde{} = q * E, da E = F\textasciitilde{}el\textasciitilde{}/q \{\{nl\}\} =\textgreater{} F\textasciitilde{}el\textasciitilde{} = q * (U/d) \{\{nl\}\} \{\{nl\}\} U:anliegende Spannung  {[}V{]} \{\{nl\}\} d: abstand der Ladungstr{\"a}ger {[}m{]} \{\{nl\}\} q: elektrische Ladung {[}C{]}} \tn 
% Row Count 15 (+ 4)
% Row 61
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 15 (+ 0)
% Row 62
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{{\bf{Millikan Versuch}}} \tn 
% Row Count 16 (+ 1)
% Row 63
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{Ziel: "Gibt es eine kleinste Ladung?"} \tn 
% Row Count 17 (+ 1)
% Row 64
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{"Schwebemetode":} \tn 
% Row Count 18 (+ 1)
% Row 65
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{- Plattenkondensator \{\{nl\}\} - Öltr{\"o}pfchen (Annahme: kugelf{\"o}rmig)} \tn 
% Row Count 20 (+ 2)
% Row 66
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{F\textasciitilde{}el\textasciitilde{} = q * U/d \{\{nl\}\} F\textasciitilde{}G\textasciitilde{} = m * g \{\{nl\}\} =\textgreater{} F\textasciitilde{}G\textasciitilde{} = V * ρ * g \{\{nl\}\} =\textgreater{} F\textasciitilde{}G\textasciitilde{} = 4/3π * r\textasciicircum{}3\textasciicircum{} * ρ * g \{\{nl\}\}} \tn 
% Row Count 23 (+ 3)
% Row 67
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{Auftriebskraft: \{\{nl\}\}F\textasciitilde{}A\textasciitilde{} (zeigt nach oben) \{\{nl\}\} F\textasciitilde{}A\textasciitilde{} = 4/3πr\textasciicircum{}3\textasciicircum{} * ρ\textasciitilde{}Luft\textasciitilde{} * g \{\{nl\}\} Luft zwischen Platten -\textgreater{} Auftrieb in Luft} \tn 
% Row Count 26 (+ 3)
% Row 68
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{-\textgreater{} F\textasciitilde{}G\textasciitilde{} - F\textasciitilde{}A\textasciitilde{} = F\textasciitilde{}G'\textasciitilde{} \{\{nl\}\}F\textasciitilde{}G'\textasciitilde{} = 4/3πr\textasciicircum{}3\textasciicircum{} * g (ρ\textasciitilde{}Öl\textasciitilde{} - ρ\textasciitilde{}Luft\textasciitilde{}) \{\{nl\}\} =\textgreater{} F\textasciitilde{}G'\textasciitilde{} = 4/3πr\textasciicircum{}3\textasciicircum{} * g * ρ' \{\{nl\}\} \{\{nl\}\} Es gilt F\textasciitilde{}G\textasciitilde{} = F\textasciitilde{}el\textasciitilde{} \{\{nl\}\} =\textgreater{} 4/3πr\textasciicircum{}3\textasciicircum{} * ρ' * g = q * U/d \{\{nl\}\} =\textgreater{} q = (4/3πr\textasciicircum{}3\textasciicircum{} * ρ' * g * d) / U} \tn 
% Row Count 31 (+ 5)
\end{tabularx}
\par\addvspace{1.3em}

\begin{tabularx}{17.67cm}{X}
\SetRowColor{DarkBackground}
\mymulticolumn{1}{x{17.67cm}}{\bf\textcolor{white}{Physik Q1 (cont)}}  \tn
% Row 69
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\mymulticolumn{1}{x{17.67cm}}{Radius bestimmen: \{\{nl\}\} F\textasciitilde{}g\textasciitilde{} = F\textasciitilde{}A\textasciitilde{} * F\textasciitilde{}R\textasciitilde{} |-F\textasciitilde{}A\textasciitilde{} \{\{nl\}\} F\textasciitilde{}G\textasciitilde{} - F\textasciitilde{}A\textasciitilde{} = F\textasciitilde{}R\textasciitilde{} \{\{nl\}\} 4/3πr\textasciicircum{}3\textasciicircum{} * g (ρ\textasciitilde{}Öl\textasciitilde{} - ρ\textasciitilde{}Luft\textasciitilde{}) = 6 πr * η * v |r, π kürzen \{\{nl\}\}  4/3r\textasciicircum{}2\textasciicircum{} * g * ρ' = 6 * η * v | * (3/4*g*ρ') \{\{nl\}\} r\textasciicircum{}2\textasciicircum{} = (9 * η * v) / (2 * ρ' * g) | Quadratwurzel \{\{nl\}\} r = Quadratwurzel( (9 * η * v) / (2 * ρ' * g) )} \tn 
% Row Count 7 (+ 7)
% Row 70
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{Herr Millikan hat mit diesem Versuch nachgewiesen, dass es diskrete Ladungen gibt, die vielfache von einer {\emph{kleinsten Ladung}} sind. Diese kleinste Ladungen nennen wir {\bf{Elementarladung e}} \{\{nl\}\} e = 1,602176634 * 10 \textasciicircum{}-19\textasciicircum{} \{\{nl\}\} ein Elektron hat genau diese Elementarladung als Ladung} \tn 
% Row Count 13 (+ 6)
% Row 71
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{} \tn 
% Row Count 13 (+ 0)
% Row 72
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{{\bf{Potential und Spannung im homogenen elektrischen Feld (z.B. Plattenkondensator)}}} \tn 
% Row Count 15 (+ 2)
% Row 73
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\mymulticolumn{1}{x{17.67cm}}{s = Strecke zwischen pos. Ladungstr{\"a}ger und pos. Platte} \tn 
% Row Count 17 (+ 2)
% Row 74
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{wir betrachten die Bewegung des pos. Ladungstr{\"a}gers} \tn 
% Row Count 19 (+ 2)
% Row 75
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{W = F * s (Arbeit = Work = W)} \tn 
% Row Count 20 (+ 1)
% Row 76
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\mymulticolumn{1}{x{17.67cm}}{Wir wissen: F = q * E \{\{nl\}\} =\textgreater{}W = q * E * s \{\{nl\}\} W/q = φ} \tn 
% Row Count 22 (+ 2)
% Row 77
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\mymulticolumn{1}{x{17.67cm}}{s\textasciitilde{}1\textasciitilde{} = Abstand zur neuen Position \{\{nl\}\} s\textasciitilde{}2\textasciitilde{} = Abstand zwischen neuer Position und pos. Platte} \tn 
% Row Count 24 (+ 2)
% Row 78
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{W(1 -\textgreater{} 2) = q* E * (s\textasciitilde{}1\textasciitilde{} - s\textasciitilde{}2\textasciitilde{}) \{\{nl\}\} = q * (Es\textasciitilde{}1\textasciitilde{} - Es\textasciitilde{}2\textasciitilde{}) \{\{nl\}\} = q * (φ\textasciitilde{}1\textasciitilde{} - φ\textasciitilde{}2\textasciitilde{}) \{\{nl\}\} = q * Δφ} \tn 
% Row Count 27 (+ 3)
% Row 79
\SetRowColor{LightBackground}
\mymulticolumn{1}{x{17.67cm}}{die {\bf{Potentialdifferenz Δφ}} hei{\ss}t {\bf{elektrische Spannung U}}} \tn 
% Row Count 29 (+ 2)
% Row 80
\SetRowColor{white}
\mymulticolumn{1}{x{17.67cm}}{U = W/q \{\{nl\}\} \textless{}=\textgreater{} W= q*U \{\{nl\}\} {[}U{]} = {[}W{]}/{[}q{]} = J/As = V (1 V*As = 1 J)} \tn 
% Row Count 31 (+ 2)
\hhline{>{\arrayrulecolor{DarkBackground}}-}
\end{tabularx}
\par\addvspace{1.3em}



\end{document}