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GNU GENERAL PUBLIC LICENSE GNU GENERAL PUBLIC LICENSE
Version 3, 29 June 2007 Version 3, 29 June 2007
Copyright © 2007 Free Software Foundation, Inc. <http://fsf.org/> Copyright © 2007 Free Software Foundation, Inc. <https://fsf.org/>
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If conditions are imposed on you (whether by court order, agreement or otherwise) that contradict the conditions of this License, they do not excuse you from the conditions of this License. If you cannot convey a covered work so as to satisfy simultaneously your obligations under this License and any other pertinent obligations, then as a consequence you may not convey it at all. For example, if you agree to terms that obligate you to collect a royalty for further conveying from those to whom you convey the Program, the only way you could satisfy both those terms and this License would be to refrain entirely from conveying the Program. A compilation of a covered work with other separate and independent works,
which are not by their nature extensions of the covered work, and which are
13. Use with the GNU Affero General Public License. not combined with it such as to form a larger program, in or on a volume of
Notwithstanding any other provision of this License, you have permission to link or combine any covered work with a work licensed under version 3 of the GNU Affero General Public License into a single combined work, and to convey the resulting work. The terms of this License will continue to apply to the part which is the covered work, but the special requirements of the GNU Affero General Public License, section 13, concerning interaction through a network will apply to the combination as such. a storage or distribution medium, is called an "aggregate" if the compilation
and its resulting copyright are not used to limit the access or legal rights
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The Free Software Foundation may publish revised and/or new versions of the GNU General Public License from time to time. Such new versions will be similar in spirit to the present version, but may differ in detail to address new problems or concerns. of a covered work in an aggregate does not cause this License to apply to
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Each version is given a distinguishing version number. If the Program specifies that a certain numbered version of the GNU General Public License “or any later version” applies to it, you have the option of following the terms and conditions either of that numbered version or of any later version published by the Free Software Foundation. If the Program does not specify a version number of the GNU General Public License, you may choose any version ever published by the Free Software Foundation.
6. Conveying Non-Source Forms.
If the Program specifies that a proxy can decide which future versions of the GNU General Public License can be used, that proxy's public statement of acceptance of a version permanently authorizes you to choose that version for the Program.
You may convey a covered work in object code form under the terms of sections
Later license versions may give you additional or different permissions. However, no additional obligations are imposed on any author or copyright holder as a result of your choosing to follow a later version. 4 and 5, provided that you also convey the machine-readable Corresponding
Source under the terms of this License, in one of these ways:
15. Disclaimer of Warranty.
THERE IS NO WARRANTY FOR THE PROGRAM, TO THE EXTENT PERMITTED BY APPLICABLE LAW. EXCEPT WHEN OTHERWISE STATED IN WRITING THE COPYRIGHT HOLDERS AND/OR OTHER PARTIES PROVIDE THE PROGRAM “AS IS” WITHOUT WARRANTY OF ANY KIND, EITHER EXPRESSED OR IMPLIED, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE. THE ENTIRE RISK AS TO THE QUALITY AND PERFORMANCE OF THE PROGRAM IS WITH YOU. SHOULD THE PROGRAM PROVE DEFECTIVE, YOU ASSUME THE COST OF ALL NECESSARY SERVICING, REPAIR OR CORRECTION. a) Convey the object code in, or embodied in, a physical product (including
a physical distribution medium), accompanied by the Corresponding Source fixed
16. Limitation of Liability. on a durable physical medium customarily used for software interchange.
IN NO EVENT UNLESS REQUIRED BY APPLICABLE LAW OR AGREED TO IN WRITING WILL ANY COPYRIGHT HOLDER, OR ANY OTHER PARTY WHO MODIFIES AND/OR CONVEYS THE PROGRAM AS PERMITTED ABOVE, BE LIABLE TO YOU FOR DAMAGES, INCLUDING ANY GENERAL, SPECIAL, INCIDENTAL OR CONSEQUENTIAL DAMAGES ARISING OUT OF THE USE OR INABILITY TO USE THE PROGRAM (INCLUDING BUT NOT LIMITED TO LOSS OF DATA OR DATA BEING RENDERED INACCURATE OR LOSSES SUSTAINED BY YOU OR THIRD PARTIES OR A FAILURE OF THE PROGRAM TO OPERATE WITH ANY OTHER PROGRAMS), EVEN IF SUCH HOLDER OR OTHER PARTY HAS BEEN ADVISED OF THE POSSIBILITY OF SUCH DAMAGES.
b) Convey the object code in, or embodied in, a physical product (including
17. Interpretation of Sections 15 and 16. a physical distribution medium), accompanied by a written offer, valid for
If the disclaimer of warranty and limitation of liability provided above cannot be given local legal effect according to their terms, reviewing courts shall apply local law that most closely approximates an absolute waiver of all civil liability in connection with the Program, unless a warranty or assumption of liability accompanies a copy of the Program in return for a fee. at least three years and valid for as long as you offer spare parts or customer
support for that product model, to give anyone who possesses the object code
END OF TERMS AND CONDITIONS either (1) a copy of the Corresponding Source for all the software in the
product that is covered by this License, on a durable physical medium customarily
used for software interchange, for a price no more than your reasonable cost
of physically performing this conveying of source, or (2) access to copy the
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If you convey an object code work under this section in, or with, or specifically
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7. Additional Terms.
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Termination of your rights under this section does not terminate the licenses
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not qualify to receive new licenses for the same material under section 10.
9. Acceptance Not Required for Having Copies.
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10. Automatic Licensing of Downstream Recipients.
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You may not impose any further restrictions on the exercise of the rights
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If, pursuant to or in connection with a single transaction or arrangement,
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you entered into that arrangement, or that patent license was granted, prior
to 28 March 2007.
Nothing in this License shall be construed as excluding or limiting any implied
license or other defenses to infringement that may otherwise be available
to you under applicable patent law.
12. No Surrender of Others' Freedom.
If conditions are imposed on you (whether by court order, agreement or otherwise)
that contradict the conditions of this License, they do not excuse you from
the conditions of this License. If you cannot convey a covered work so as
to satisfy simultaneously your obligations under this License and any other
pertinent obligations, then as a consequence you may not convey it at all.
For example, if you agree to terms that obligate you to collect a royalty
for further conveying from those to whom you convey the Program, the only
way you could satisfy both those terms and this License would be to refrain
entirely from conveying the Program.
13. Use with the GNU Affero General Public License.
Notwithstanding any other provision of this License, you have permission to
link or combine any covered work with a work licensed under version 3 of the
GNU Affero General Public License into a single combined work, and to convey
the resulting work. The terms of this License will continue to apply to the
part which is the covered work, but the special requirements of the GNU Affero
General Public License, section 13, concerning interaction through a network
will apply to the combination as such.
14. Revised Versions of this License.
The Free Software Foundation may publish revised and/or new versions of the
GNU General Public License from time to time. Such new versions will be similar
in spirit to the present version, but may differ in detail to address new
problems or concerns.
Each version is given a distinguishing version number. If the Program specifies
that a certain numbered version of the GNU General Public License "or any
later version" applies to it, you have the option of following the terms and
conditions either of that numbered version or of any later version published
by the Free Software Foundation. If the Program does not specify a version
number of the GNU General Public License, you may choose any version ever
published by the Free Software Foundation.
If the Program specifies that a proxy can decide which future versions of
the GNU General Public License can be used, that proxy's public statement
of acceptance of a version permanently authorizes you to choose that version
for the Program.
Later license versions may give you additional or different permissions. However,
no additional obligations are imposed on any author or copyright holder as
a result of your choosing to follow a later version.
15. Disclaimer of Warranty.
THERE IS NO WARRANTY FOR THE PROGRAM, TO THE EXTENT PERMITTED BY APPLICABLE
LAW. EXCEPT WHEN OTHERWISE STATED IN WRITING THE COPYRIGHT HOLDERS AND/OR
OTHER PARTIES PROVIDE THE PROGRAM "AS IS" WITHOUT WARRANTY OF ANY KIND, EITHER
EXPRESSED OR IMPLIED, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES
OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE. THE ENTIRE RISK AS
TO THE QUALITY AND PERFORMANCE OF THE PROGRAM IS WITH YOU. SHOULD THE PROGRAM
PROVE DEFECTIVE, YOU ASSUME THE COST OF ALL NECESSARY SERVICING, REPAIR OR
CORRECTION.
16. Limitation of Liability.
IN NO EVENT UNLESS REQUIRED BY APPLICABLE LAW OR AGREED TO IN WRITING WILL
ANY COPYRIGHT HOLDER, OR ANY OTHER PARTY WHO MODIFIES AND/OR CONVEYS THE PROGRAM
AS PERMITTED ABOVE, BE LIABLE TO YOU FOR DAMAGES, INCLUDING ANY GENERAL, SPECIAL,
INCIDENTAL OR CONSEQUENTIAL DAMAGES ARISING OUT OF THE USE OR INABILITY TO
USE THE PROGRAM (INCLUDING BUT NOT LIMITED TO LOSS OF DATA OR DATA BEING RENDERED
INACCURATE OR LOSSES SUSTAINED BY YOU OR THIRD PARTIES OR A FAILURE OF THE
PROGRAM TO OPERATE WITH ANY OTHER PROGRAMS), EVEN IF SUCH HOLDER OR OTHER
PARTY HAS BEEN ADVISED OF THE POSSIBILITY OF SUCH DAMAGES.
17. Interpretation of Sections 15 and 16.
If the disclaimer of warranty and limitation of liability provided above cannot
be given local legal effect according to their terms, reviewing courts shall
apply local law that most closely approximates an absolute waiver of all civil
liability in connection with the Program, unless a warranty or assumption
of liability accompanies a copy of the Program in return for a fee. END OF
TERMS AND CONDITIONS
How to Apply These Terms to Your New Programs How to Apply These Terms to Your New Programs
If you develop a new program, and you want it to be of the greatest possible use to the public, the best way to achieve this is to make it free software which everyone can redistribute and change under these terms. If you develop a new program, and you want it to be of the greatest possible
use to the public, the best way to achieve this is to make it free software
which everyone can redistribute and change under these terms.
To do so, attach the following notices to the program. It is safest to attach them to the start of each source file to most effectively state the exclusion of warranty; and each file should have at least the “copyright” line and a pointer to where the full notice is found. To do so, attach the following notices to the program. It is safest to attach
them to the start of each source file to most effectively state the exclusion
of warranty; and each file should have at least the "copyright" line and a
pointer to where the full notice is found.
<one line to give the program's name and a brief idea of what it does.> <one line to give the program's name and a brief idea of what it does.>
Copyright (C) <year> <name of author>
This program is free software: you can redistribute it and/or modify it under the terms of the GNU General Public License as published by the Free Software Foundation, either version 3 of the License, or (at your option) any later version. Copyright (C) <year> <name of author>
This program is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License for more details. This program is free software: you can redistribute it and/or modify it under
the terms of the GNU General Public License as published by the Free Software
Foundation, either version 3 of the License, or (at your option) any later
version.
You should have received a copy of the GNU General Public License along with this program. If not, see <http://www.gnu.org/licenses/>. This program is distributed in the hope that it will be useful, but WITHOUT
ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS
FOR A PARTICULAR PURPOSE. See the GNU General Public License for more details.
You should have received a copy of the GNU General Public License along with
this program. If not, see <https://www.gnu.org/licenses/>.
Also add information on how to contact you by electronic and paper mail. Also add information on how to contact you by electronic and paper mail.
If the program does terminal interaction, make it output a short notice like this when it starts in an interactive mode: If the program does terminal interaction, make it output a short notice like
this when it starts in an interactive mode:
<program> Copyright (C) <year> <name of author> <program> Copyright (C) <year> <name of author>
This program comes with ABSOLUTELY NO WARRANTY; for details type `show w'.
This is free software, and you are welcome to redistribute it under certain conditions; type `show c' for details.
The hypothetical commands `show w' and `show c' should show the appropriate parts of the General Public License. Of course, your program's commands might be different; for a GUI interface, you would use an “about box”. This program comes with ABSOLUTELY NO WARRANTY; for details type `show w'.
You should also get your employer (if you work as a programmer) or school, if any, to sign a “copyright disclaimer” for the program, if necessary. For more information on this, and how to apply and follow the GNU GPL, see <http://www.gnu.org/licenses/>. This is free software, and you are welcome to redistribute it under certain
conditions; type `show c' for details.
The GNU General Public License does not permit incorporating your program into proprietary programs. If your program is a subroutine library, you may consider it more useful to permit linking proprietary applications with the library. If this is what you want to do, use the GNU Lesser General Public License instead of this License. But first, please read <http://www.gnu.org/philosophy/why-not-lgpl.html>. The hypothetical commands `show w' and `show c' should show the appropriate
parts of the General Public License. Of course, your program's commands might
be different; for a GUI interface, you would use an "about box".
You should also get your employer (if you work as a programmer) or school,
if any, to sign a "copyright disclaimer" for the program, if necessary. For
more information on this, and how to apply and follow the GNU GPL, see <https://www.gnu.org/licenses/>.
The GNU General Public License does not permit incorporating your program
into proprietary programs. If your program is a subroutine library, you may
consider it more useful to permit linking proprietary applications with the
library. If this is what you want to do, use the GNU Lesser General Public
License instead of this License. But first, please read <https://www.gnu.org/
licenses /why-not-lgpl.html>.

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# TTT4260 # TTT4160
Kilden til designprosjekt 1-4 i TTT4260 Elektronisk systemdesign og analyse Kilden til designprosjekt 1-4 i TTT4160 Elektronisk systemdesign og analyse

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#!/usr/bin/env python3
# -*- coding: utf-8 -*-
"""
Created on Fri Jan 18 22:30:00 2019
@author: oyvind
"""
import math
import matplotlib.pyplot as plt
# Name for the saved graph
filename = "4b"
# Tau in microseconds
tau = 10
# Square wave freq in kHz
sqWFreq = 5
# How many taus you want
periods = 40
# The resolution of each tau
resolution = 1000
# Calculates the length of each squarewave in taus
sqTime = (1/sqWFreq) * 10**3
sqTau = sqTime / tau
# Creats the square wave
# Default values are in the argument list
def CreateSquareWave(amp=0.5, offset=0.5, symetry=0.5):
squareWave = []
# Only generates as many datapoints we need
while len(squareWave) < periods * resolution:
# First generate the first half
for r in range(int(resolution*sqTau * symetry)):
squareWave.append(amp + offset)
# Then the second
for r in range(int(resolution*sqTau * (1 - symetry))):
squareWave.append(offset - amp)
squareWave = squareWave[:(resolution*periods)]
return squareWave
# Generate all the time-ticks
def GenerateTime():
times = []
for t in range(periods * resolution):
times.append(t/resolution)
print(len(times))
return(times)
def CapVoltage(wave, times):
cP = wave[0] # Start voltage-supply
v0 = 0 # Start voltage
cT = 0 #Start time
volt = []
for p in range(len(wave)):
# If the voltage-supply changes, recalculate startvalues
if wave[p] != cP:
v0 = volt[-1] # New start voltage, uses the last voltage calculated
cP = wave[p] # Variable so the array is not accessed.
cT = times[p] # Offset time for each period
# Calculate the voltage over the CAPACITOR with the start values
volt.append(cP + (v0 - cP) * math.exp(-(times[p] - cT)))
return(volt)
SquareWave = CreateSquareWave()
time = GenerateTime()
CapWave = CapVoltage(SquareWave, time)
plt.figure(figsize=(15,5))
plt.plot(time, SquareWave, time, CapWave)
plt.xlabel("Time [τ]")
plt.ylabel("Voltage [V]")
plt.legend(["Supply voltage", "Capacitor voltage"], loc="lower right")
plt.savefig(filename + ".png", dpi = 300)
plt.show()

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\documentclass[10pt]{article}
\usepackage{pgf,tikz,pgfplots}
\pgfplotsset{compat=1.15}
\usepackage{mathrsfs}
\usetikzlibrary{arrows}
\pagestyle{empty}
\begin{document}
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View File

@ -0,0 +1,401 @@
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View File

@ -0,0 +1,433 @@
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\draw (0.9826971286425398,1.0091692065822461) node[anchor=north west] {$(\tau, 0.79\text{V})$};
\draw (1.7132719478893085,0.5951090467957184) node[anchor=north west] {$(2\tau, 0.29\text{V})$};
\draw (2.588565094705576,0.46352472684146245) node[anchor=north west] {$(3\tau, 0.11\text{V})$};
\draw (3.592848810526346,0.35387112687958255) node[anchor=north west] {$(4\tau, 0.04\text{V})$};
\draw (4.597132526347116,0.35387112687958255) node[anchor=north west] {$(5\tau, 0.01\text{V})$};
\begin{scriptsize}
\draw[color=qqwuqq] (0.14886523614914818,2.1083287262696615) node {$v_c$};
\draw [fill=uuuuuu] (1.,0.7872620041068866) circle (2.0pt);
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\draw [fill=uuuuuu] (5.,0.0144192065780429) circle (2.0pt);
\end{scriptsize}
\end{axis}
\end{tikzpicture}

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\documentclass[11pt,largemargins, norsk]{homework}
\newcommand{\hwname}{Øyvind Skaaden}
\newcommand{\hwemail}{oyvindps@ntnu.no}
\newcommand{\hwtype}{Øving}
\newcommand{\hwnum}{1}
\newcommand{\hwclass}{TTT4260}
\newcommand{\hwlecture}{}
\newcommand{\hwsection}{}
\newcommand*{\eq}{=}
\renewcommand{\questiontype}{Oppgave}
\newcommand{\figref}[1]{Figur \ref{#1}}
\begin{document}
\maketitle
\question
\begin{alphaparts}
\item Vi har krets \ref{circ:1a} som vist under med verdiene $R_1 = 1\text{k}\Omega $, $ C_1 = 100\mu\text{F} $ og $V = 5\text{V} $.
\begin{figure} [h]
\centering
\begin{circuitikz}
\draw
(0,3) to [V, l=$V$] (0,0)
(0,3) to [closing switch, l = $t\eq0$ ] (3,3)
to [R, l=$R_1$] (6,3)
to [C, l=$C_1$] (6,0) -- (0,0);
\end{circuitikz}
\caption{Krets til oppgave 1}
\label{circ:1a}
\end{figure}
$\tau$ er gitt ved
$$ \tau = R \cdot C $$
Da er $\tau$ i denne kretsen er da
$$ \tau = R_1 \cdot C_1 = 1\text{k}\Omega \cdot 100\mu\text{F} = 100\text{ms}$$
En funksjon for spenningen over kondensatoren er da
$$ v_c(t) = 5 \text{V} \cdot ( 1 - e ^ {\frac{-t}{100\text{ms}}}) $$
\pagebreak
\begin{figure}[!ht]
\centering
\input{grafer/condisO1a}
\caption{Utvikling av spenning over kondensator $v_c$}
\label{graph:kondensator1}
\end{figure}
\item
Etter å ha koblet opp kretsen ser vi at spenningen (se \figref{graph:1b}) over kondensatoren når $63\%$ eller $3.16$V etter $\Delta x = 94.83$ms.
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{TauMaaling.png}
\caption{Spennigsutvikling av krets i oppgave 1, $\tau$ er lik $\Delta x$}
\label{graph:1b}
\end{figure}
\pagebreak
\item
Når det skjer utladning av kondensatoren har ikke strømmen noe sted å gå, eneste er å gå gjennom kondensatoren litt og litt.
\end{alphaparts}
\question
For å løse kretsen i oppgave 2, vist i kretsen \figref{circ:krets2} under.
\begin{figure}[h]
\centering
\begin{circuitikz}
\draw
(-6,3) to [V, v=V] ++(0,-3)
(-6,3) to [opening switch, l=$S_1$] ++(3,0)
to [R, l=$R_1$] +(3,0) to [short,-*] ++(0,0)
(-6,0) to [short,-*] (0,0)
(0,0) to [R, l=$R_2$] (0,3)
(0,0) -- (2,0) to [short,-*] (2,0) to [R, l=$R_3$] (2,3) to [short,-*] ++(0,0) -- (0,3)
(2,3) to [R, l=$R_4$] (6,3)
to [C, l=$C_1$, v_=$v_c$] (6,0) -- (2,0);
\end{circuitikz}
\caption{Krets i oppgave 2}
\label{circ:krets2}
\end{figure}
Vi må finne spenningen som ligger over $R_2||R_3$ for å finne startspenningen på $C_1$.
Begynner med å finne $$R_2||R_3 = \frac{470\ohm \cdot 220\ohm}{470\ohm + 220\ohm} = \frac{10340}{69} \ohm $$
$$ v_{R_2||R_3} = \frac{V}{R_1 + R_2||R_3} \cdot (R_2||R_3) = \frac{5\text{V}}{200\ohm + \frac{10340}{69} \ohm} \cdot \frac{10340}{69} \ohm = \frac{2585}{1207}\text{V} \approx 2.14\text{V} $$
Dette er da startspenningen på $c_1$.
Når bryteren brytes, vi vi få en forenklet krets, som vist i \figref{circ:oppgave2}
\begin{figure}
\centering
\begin{circuitikz}
\draw
(0,0) to [R, l=$R_2$] (0,3)
(0,0) -- (2,0) to [short,-*] (2,0) to [R, l=$R_3$] (2,3) to [short,-*] ++(0,0) -- (0,3)
(2,3) to [R, l=$R_4$] (6,3)
to [C, l=$C_1$, v_=$v_c$] (6,0) -- (2,0);
\end{circuitikz}
\caption{Foreklet krets i oppgave 2}
\label{circ:oppgave2}
\end{figure}
Vi kan da regne ut $R$ i kretsen
$$ R = R_4 + R_2||R_3 = 300\ohm + \frac{10340}{69} \ohm = \frac{31040}{69}\ohm \approx 449.9\ohm $$
$\tau$ er da gitt ved $\tau = R \cdot C_1 = = 4.5\mu\text{s}$.
Funksjonen for spenningen over $v_c$:
$$ v_c(t) = 2.14e^{\frac{-t}{4.5\mu\text{s}}} $$
\begin{figure}[h]
\centering
\input{grafer/condisO2}
\caption{Graf for oppgave 2}
\label{graph:oppg2}
\end{figure}
\clearpage
\question
\begin{alphaparts}
\item
Vi har kretsen som gitt i oppgave 3, men tegnet på en forenklet måte i \figref{circ:3a1}.
\begin{figure}[h]
\centering
\begin{circuitikz}
\draw
(0,3) to [V, v_=V] (0,0)
(0,3) to [R, l=$R_1\eq1\text{k}\ohm$] (3,3)
to [closing switch, l=$S_1$] (5,3)
to [R, l_=$R_2\eq1\text{k}\ohm$] (5,0) -- (0,0)
(5,3) to [short,*-] ++(2,0)
to [C, l=$C_1\eq100\mu\text{F}$] ++(0,-3)
to [short,-*] (5,0);
\end{circuitikz}
\caption{Forenklet krets til oppgave 3a}
\label{circ:3a1}
\end{figure}
Vi skriver om til en Norton ekvivalent ved å regne ut $I_n = \tfrac{V}{R_1}$
$$ I_n = \frac{1\text{V}}{1\text{k}\ohm} = 1\text{mA} $$
Vi har da to like motstander i parallell. Siden de er like er den totale motstanden lik halvparten av den ene. Så
$$ R_{eq} = 0.5\text{k}\ohm $$
Vi regner deretter den nye kretsen tilbake til en thevenin-ekvivalent krets.
$$ V_{th} = I_n \cdot R_{eq} = 1\text{mA}\cdot 0.5\text{k}\ohm = 0.5\text{V}$$
Vi har da den nye kretsen under i \figref{circ:3a2}
\begin{figure}[h]
\centering
\begin{circuitikz}
\draw
(0,3) to [V, v_=V$_{th}$] (0,0)
(0,3) to [R, l=$R_{eq}\eq0.5\text{k}\ohm$] ++(3,0)
to [C, l=$C_1\eq100\mu\text{F}$, v=$v_{C_1}$] ++(0,-3)
-- (0,0);
\end{circuitikz}
\caption{Thevenin-ekvivalent krets til oppgave 3a}
\label{circ:3a2}
\end{figure}
Det er da veldig lett å lage en funksjon som besrkiver spenningen, $v_{C_1}$, over $C_1$.
\begin{align*}
v_{C_1}(t)&= V_{th}\left(1-e^\frac{-t}{R_{eq}C_1}\right) \\
v_{C_1}(t)&= 0.5\text{V}\left(1-e^\frac{-t}{0.5\text{ms}}\right)\\
v_{C_1}(t)&= 0.5\text{V}\left(1-e^\frac{-t}{\tau}\right)
\end{align*}
\clearpage
\item
Etter $6\tau$ har kondensatoren nådd ``steady-state'', da er spenningen $v_{C_1} = V_{th} = 0.5\text{V}$. Når bryteren $S_2$ lukkes får vi en veldig lik krets som i opgpave 3a. Se \figref{circ:3b1}
\begin{figure}[h]
\centering
\begin{circuitikz}
\draw
(0,3) to [V, v_=V$\eq1\text{V}$] (0,0)
(0,3) to [R, l=$R_1\eq1\text{k}\ohm$] (4,3)
to [R, l_=$R_2\eq1\text{k}\ohm$] ++(0,-3) -- (0,0)
(4,3) to [short,*-] ++(3,0)
to [R, l_=$R_3\eq1\text{k}\ohm$] ++(0,-3)
to [short,-*] (4,0)
(7,3) to [short,*-] ++(3,0)
to [C, l=$C_1\eq100\mu\text{F}$] ++(0,-3)
to [short,-*] ++(-3,0);
\end{circuitikz}
\caption{Forenklet krets til oppgave 3a}
\label{circ:3b1}
\end{figure}
Vi gjør det samme som sist, gjør om til norton-ekvivalent, samler motstandene og går tilbake til en thevenin-ekvivalent.
Siden det her er tre like motstander i parallell er den totale motstanden lik $1/3$ av en av motstandene. Vi får da $V_{th} = \frac{1}{3}\text{V}=\approx 333.3\text{mV}$ og $R_{eq} \approx 333.3\ohm$.
Kretsen ser da ut som \figref{circ:3b2}
\begin{figure}[h]
\centering
\begin{circuitikz}
\draw
(0,3) to [V, v_=V$_{th}\approx 333.3\text{mV}$] (0,0)
(0,3) to [R, l=$R_{eq}\approx 333.3\ohm$] ++(3,0)
to [C, l=$C_1\eq100\mu\text{F}$, v=$v_{C_1}$] ++(0,-3)
-- (0,0);
\end{circuitikz}
\caption{Thevenin-ekvivalent krets til oppgave 3a}
\label{circ:3b2}
\end{figure}
Da er det enkelt å sette opp likningen for spenningen $v_{C_1}$
Vi setter $\tau = 1$ for at det skal være lettere å lese grafene. Grafene ser helt like ut men tidsenheten blir da $\tau$ i steden for ms.
\begin{align*}
v_{C_1}(t) &= V_{th}+\left[v_{C_1}(t_0) - V_{th} \right]e^{-\frac{t-t_0}{R_{eq}C_1}}\\
&\downarrow \\
v_{C_1}(t) &= \frac{1}{3}\text{V} + \frac{1}{6}\text{V} \cdot e^{-\frac{t-6\tau}{\tau}}
\end{align*}
En skisse av spenningsutviklingen kan sees i \figref{fig:3b}.
\pagebreak
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{grafer/3b.png}
\caption{Spenningen $V_{C_1}$ som graf, der $S_2$ lukkes etter $6\tau$}
\label{fig:3b}
\end{figure}
\item
For å lage en funksjon for kretsen når bryter $S_2$ lukkes når $t=0.5\tau$, tar vi utgangspunkt i funksjonen fra oppgave 3b og spenningen $v_{C_1}(0.5\tau)\approx \frac{1}{5}\text{V}$.
Funksjonen for spenningen over $C_1$ fra $t=0.5\tau$ blir da
\begin{align*}
v_{C_1}(t) &= V_{th}+\left[v_{C_1}(t_0) - V_{th} \right]e^{-\frac{t-t_0}{R_{eq}C_1}}\\
&\downarrow \\
v_{C_1}(t) &=\frac{1}{3}\text{V}+\left[\frac{1}{5}\text{V} - \frac{1}{3}\text{V} \right]e^{-\frac{t-0.5\tau}{\tau}}\\
v_{C_1}(t) &= \frac{1}{3}\text{V} - \frac{2}{15}\text{V} \cdot e^{-\frac{t-0.5\tau}{\tau}}
\end{align*}
En skisse av spenningsutviklingen kan sees i \figref{fig:3c}.
\pagebreak
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{grafer/3c.png}
\caption{Spenningen $V_{C_1}$ som graf, der $S_2$ lukkes etter $0.5\tau$}
\label{fig:3c}
\end{figure}
\end{alphaparts}
\question
\begin{alphaparts}
\item
Tidskonstanten $\tau$ er gitt ved
$$ \tau = R \cdot C $$
I denne kretsen vil $\tau$ bli følgende.
$$ \tau = 1\text{k}\ohm \cdot 1\text{nF} = 1\mu\text{s} $$
\pagebreak
\item
Graf ved $f=5$kHz
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{Oppgave4Python/4b.png}
\caption{Graf for kretsen i oppgave 4, ved $f=5\text{kHz}$}
\label{graph:4b}
\end{figure}
\item
Graf ved $f=30$kHz
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{Oppgave4Python/4c2.png}
\caption{Graf for kretsen i oppgave 4, ved $f=30\text{kHz}$}
\label{graph:4c}
\end{figure}
\item
Etter oppkobling av kretsen ser vi at kondensatoren oppfører seg veldig likt som regnet ut i oppgave 4b. 4c ($30$kHz) er litt mer ulik da kondensatoren lades og utlades litt raskere enn beregnet. Den når litt høyere og litt lavere spenninger enn beregnet.
\pagebreak
\item
Vi ser fra \figref{graph:4b} at firkantpulsen er $1$V i $10\tau = 10 \cdot 10\mu\text{s} = 100\mu\text{s}$.
Vi ønsker da at likningen $v_{C_1}(100\mu\text{s}) = 0.8$V. Vi setter kondensatorverdien konstant og regner ut motstanden $R$ i kretsen.
\begin{align*}
v_{C_1}(t) &= V_1+\left[v_{C_1}(t_0) - V_1 \right]e^{-\frac{t-t_0}{R\cdot C_1}}\\
0.8\text{V} &= 1\text{V}\cdot\left(1-e^{-\frac{100\mu\text{s}}{R\cdot10\text{nF}}}\right) \\
R &= \frac{10000}{\ln 5}\\
R&\approx 6213 \ohm
\end{align*}
Tester dette og ser at den lader seg litt for mye opp.
Etter å har justert til $6300\ohm$ ser det ut som at spenningen når ca $0.8$V på firkantpulsen.
\end{alphaparts}
\end{document}

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\documentclass[11pt,largemargins, norsk]{homework}
\newcommand{\hwname}{Øyvind Skaaden}
\newcommand{\hwemail}{oyvindps@ntnu.no}
\newcommand{\hwtype}{Øving}
\newcommand{\hwnum}{2}
\newcommand{\hwclass}{TTT4260}
\newcommand{\hwlecture}{}
\newcommand{\hwsection}{}
\renewcommand{\questiontype}{Oppgave}
\newcommand{\figref}[1]{Figur \ref{#1}}
\begin{document}
\maketitle
\question
\begin{alphaparts}
\item
Når $A$ er logisk høy, er $C$ logisk lav. Når $A$ er logisk lav, er $C$ logisk høy.
\item
Kretsen i oppgave 1 er en inverter fordi den tar inn et logisk signal, og sender ut det motsatte ut etter kretsen. Dersom inngangen er 1 er utgangen 0, og når inngangen er 0 er utgangen 1.
\item
Når det er $0$V på inngangen $A$ er det $5$V på utgangen $C$.
\item Vi gjør målinger på kretsen, setter spenning på $A$ lik $v_A $ og måler spenningen $v_C $ på utgangen $C$. 43
\begin{table}[h]
\centering
\begin{tabular}{|c|c|}
\hline
$v_A$ & $v_C $ \\ \hline
\hline
0 & 4.98 \\
0.5 & 4.95 \\
1 & 4.95 \\
1.5 & 4.95 \\
2 & 4.93 \\
2.1 & 4.89 \\
2.2 & 4.79 \\
2.3 & 4.56 \\
2.4 & 4.13 \\
2.5 & 3.4 \\
2.6 & 2.32 \\
2.7 & 1.11 \\
2.8 & 0.23 \\
2.9 & 0.12 \\
3 & 0.08 \\
3.5 & 0.03 \\
4 & 0.02 \\
4.5 & 0.018 \\
5 & 0.014 \\
\hline
\end{tabular}
\caption{Målte spenninger på $C$, alle verdier har enhet V}
\label{tab:oppg1}
\end{table}
\begin{figure}[h!]
\centering
\includegraphics[width=\textwidth]{grafOppg1.png}
\caption{Spenning $v_C$ som funksjon av $v_A$}
\label{graph:oppg1}
\end{figure}
\item
Vi ser i \figref{graph:oppg1} at transistoren begynner å lede rundt $2.2$V til $2.3$V. Den er som en kortslutning ved ca $3.0$V.
\item
Dioden begynner å lyse når $A$ er ca $2$V. Da er $C$ lik $2.42$V.
\end{alphaparts}
\question
\begin{alphaparts}
\item
Her er begge grafene skisserte.
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{bilder/oppg2_a1.png}
\caption{Graf ved $T=10\tau$}
\label{graph:2a1}
\end{figure}
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{bilder/oppg2_a2.png}
\caption{Graf ved $T=2\tau$}
\label{graph:2a2}
\end{figure}
\clearpage
\item
Vi ønsker at kretsen skal nå $2$V. Vi ønsker å finne tiden det tar.
$$ 2\text{V} = 5V(1-e^{\frac{-t}{\tau}})$$
Som gjør at
$$ t = \frac{1}{2}\tau $$
Vi vet også at perioden er $T=1$ms. Vi vet også at $v_1 $ er $5$V i $1/2$ periode. Som betyr at
$$ \frac{1}{2}T = \frac{1}{2}\tau \Leftrightarrow \tau = 1\text{ms}$$
Vi må lage $\tau$. Velger kondensator lik $100\mu$F.
$$ \frac{1\text{ms}}{100\mu\text{F}} = 10\ohm$$
\item
Kobler opp kretsen og oppladning når maksimalt $2$V.
\item
Ved frekvensen $1$kHz vil dioden lyse, og samme for frekvenser over.
For lave frekvenser, feks $1$Hz vil dioden blinke med frekvensen $1$Hz.
\item
Dioden lyser hele tiden egentlig. Ved veldig lave frekvenser blinker dioden, desto høyere frekvenser jo serkere lys, men veldig lite forskjell.
\end{alphaparts}
\end{document}

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#!/usr/bin/env python3
# -*- coding: utf-8 -*-
"""
Created on Sun Jan 13 16:30:58 2019
@author: oyvind
"""
import csv
import matplotlib.pyplot as plt
header = []
data = []
filename = "0.1V1K"
with open(filename + ".csv") as csvfile:
csvreader = csv.reader(csvfile)
header = next(csvreader)
for dataplot in csvreader:
values = [float(value) for value in dataplot]
data.append(values)
time = [p[0] * 1000 for p in data]
ch1 = [p[1] for p in data]
ch2 = [p[2] for p in data]
plt.plot(time,ch1, time,ch2)
plt.xlabel("Tid (ms)")
plt.ylabel("Spenning (V)")
plt.legend(["Forsterket signal","Inngangssignal"])
plt.savefig(filename + ".png", dpi=200)
plt.show()

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\documentclass[11pt,largemargins, norsk]{homework}
\newcommand{\hwname}{Øyvind Skaaden}
\newcommand{\hwemail}{oyvindps@ntnu.no}
\newcommand{\hwtype}{Øving}
\newcommand{\hwnum}{10}
\newcommand{\hwclass}{TTT4260}
\newcommand{\hwlecture}{}
\newcommand{\hwsection}{}
\renewcommand{\questiontype}{Oppgave}
\newcommand{\figref}[1]{Figur \ref{#1}}
\begin{document}
\maketitle
\question
\begin{alphaparts}
\item
For å finne utgangsspenningen $v_2 $ må vi først finne spenningen over $R_i $, $v_1 $. Den er
$$ v_1 = \frac{R_i}{R_i + R_s} v_s \quad\Rightarrow\quad v_1 = \frac{100\text{k}\Omega}{100\text{k}\Omega + 33\Omega} \cdot 0.6\text{mV} \approx 0.6\text{mV}$$
Spenningen $Av_1 $, der $A = 10^4 $ blir $Av_1 = 6$V.
Spenningen $v_2 $ blir da spenningen over $R_L $. Den er
$$ v_2 = \frac{R_L}{R_L + R_0} Av_1 \quad\Rightarrow\quad v_2 = \frac{1\text{k}\Omega}{1\text{k}\Omega + 200\Omega} = 5\text{V}$$
\item Se \figref{graph:oppgave1b}
\begin{figure}[h]
\centering
\includegraphics[width=0.8\textwidth]{pic/SkissetTegning.png}
\caption{Skissert spenning $v_2 $ med ikke-ideell op-amp}
\label{graph:oppgave1b}
\end{figure}
\item
Signalet er klippet fra 5V og oppver. Dette kan forhindres ved å senke amplituden til inngangssignalet ned til $0.5$mV. Dette kan gjøres ved å øke motstanden $R_s $ og senke $R_i $.
\end{alphaparts}
\question
\begin{alphaparts}
\item
Kretsen i figur 3 er en buffer. Den vil kunne ta inn et inngangssignal og levere akkurat det samme tilbake til kretsen. Den har en forsterkning på 1, altså det samme signalet inn som ut. Den brukes ofte der kretsen som leverer signalet ikke klarer å levere nok strøm til det den leverer til. Bufferen klarer da å levere nok strøm.
\item
Kretsen i figur 4 er en inverterende forsterker. Det går ingen strøm gjennom forsterkeren, men det går en strøm fra $v_i $ til $v_o $. Vi kan da sette opp KVL, basert på at det går en strøm fra $v_i $ til $v_o $.
\begin{align}
-v_i + R_1 \cdot i + R_2 \cdot i + v_o = 0
\label{eq:2b}
\end{align}
Vi har også at spenningen til terminalene er like mellom seg, og at den ikke inverterende er koblet til jord.
$$ -v_i + R_1\cdot i = 0 \qquad\Leftrightarrow\qquad i = \frac{v_i}{R_1} $$
Setter vi dette inn i (\ref{eq:2b}), får vi
\begin{align*}
-v_i + R_1 \cdot \frac{v_i}{R_1} + R_2 \cdot \frac{v_i}{R_1} + v_o &= 0 \\
\frac{v_o}{v_i} &= -\frac{R_2}{R_1}
\end{align*}
\item
Kretsen i figur 5 er en ikke inverterende forsterker. Spenningen over terminalene er lik. Bruker nodespenning.
\begin{align*}
\frac{v_i}{R_1} + \frac{v_i + v_o}{R_2} &= 0 \\
\frac{R_2}{R_1} &= \frac{-v_i + v_o}{v_i} \\
\frac{v_o}{v_i} - 1 &= \frac{R_2}{R_1} \\
\frac{v_o}{v_i} &= \frac{R_2 + R_1}{R_1}
\end{align*}
\item
Kretsen i figur 6 er en derivator. Vi vet at strømmen gjennom en kondensator er $ i_c = C\frac{dv_c}{dt} $ Vi vet også at det ikke går noe strøm gjennom forsterkeren, så all strøm må gå gjennom motstanden $R_1 $. Siden det ikke er noen spenning mellom terminalene på forsterkeren, og den ikke inverterende er koblet til jord vil spenningen over motstanden $R_1 $ være $-v_o $
Setter dette lik hverandre.
\begin{align*}
C\frac{dv_i}{dt} &= \frac{-v_o}{R_1}\\
v_o &= -RC\frac{dv_i}{dt}
\end{align*}
\item
Kretsen i figur 7 er en integrator. Her er det tilsvarende som oppgaven over.
Finner strømmen gjennom $R $ og $C $.
\begin{align*}
\frac{v_i}{R_1} &= -C\frac{dv_o}{dt} \\
\frac{dv_o}{dt} &= -\frac{v_i}{RC} \\
v_o &= -\frac{1}{RC}\int v_i\ dt
\end{align*}
\item
Kretsen i figur 8 er en komparator. Den har en terskelspenning som kan settes på den inverterende inngangen. Dersom inngangssignalet er mindre enn terskelspenningen vil utgangssignalet trekkes ned mot det nedre spenningsforsyningen.
Dersom den er større, vil utgangssignalet trekkes til den øvre spenningsforsyning.
\end{alphaparts}
\question
\begin{alphaparts}
\item Kretsen i figur 9 fungerer ikke på samme måte som kretsen i figur 4 (inverterende forsterker). Denne kretsen vil vokse veldig fort oppover når inngangsspenning er positiv og omvendt når inngangen er negativ.
Etter litt søking på internettet er dette en ``Schmitt-trigger'' \footnote{Wikipedia contributors. (2019, January 20). Operational amplifier. In Wikipedia, The Free Encyclopedia. Retrieved 10:43, February 7, 2019, from \url{https://en.wikipedia.org/w/index.php?title=Operational_amplifier&oldid=879387924}}
\item
Dersom $v_1 $ er et trekantsignal vil signalet ut på $v_2 $ bli et firkantsignal.
\item
Dersom vi integrerer et firkantsignal vil vi få en kurve som alternerer mellom et konstant stignigstall som er positivt og et negativt. Den eneste kurven som passer dette, er en trekantbølge.
\end{alphaparts}
\question
\begin{alphaparts}
\item Krets koblet opp. Inngangsamplitude er på $0.1$V. Forventet utgangsamplitude er $1$V, forsterkingen er på -10. Valgte motstander $R_1 = 1\text{k}\Omega $ og $R_2 = 10\text{k}\Omega$
Vi kan se forsterkningssignalet i \figref{graph:oppgave4a}
\begin{figure}[h]
\centering
\includegraphics[width=0.7\textwidth]{pic/vanligForsterker.JPG}
\caption{Oppkoblet krets etter Figur 4 i oppgavetekten, en inverterende forsterker}
\label{pic:oppgave4a}
\end{figure}
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{graf/0.1V1K.png}
\caption{OP-Amp med inngangsspenning $0.1$V og forventet utgangsspenning på $1$V}
\label{graph:oppgave4a}
\end{figure}
\item
Forsterkeren blir mettet når inngangssignalet overstiger 0.5V. Vi kan se dette i grafen i \figref{graph:oppgave4b}
\begin{figure}[h]
\centering
\includegraphics[width=\textwidth]{graf/0.5V1K.png}
\caption{OP-Amp med inngangsspenning $0.5$V. Her klipper forsterkeren på ca 4V}
\label{graph:oppgave4b}
\end{figure}
\end{alphaparts}
\clearpage
\question
Kobler opp kretsen i oppgave 5. Bruker inngangsspenning 1V og spenningskilde 5V og -5V. Bruker et 10k potmeter. Kan variere forsterkningen fra 3.45V til 0.18V, eller i dB, ca +10db til -14.9dB
\begin{figure}[h]
\centering
\includegraphics[width=0.7\textwidth]{pic/varierendeForsterker.JPG}
\caption{Fysisk krets for en varierende inverterende forserker}
\label{pic:oppgave5}
\end{figure}
\end{document}

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#!/usr/bin/env python3
# -*- coding: utf-8 -*-
"""
Created on Thu Feb 28 11:00:18 2019
@author: oyvind
"""
import numpy as np
import matplotlib.pyplot as plt
def H(f):
w = 2 * np.pi * f
return (w * 10**(-4))/np.sqrt(1+(w*10**(-4))**2)
frq = []
values = []
for i in range(2*10**5):
frq.append(i)
value = 20 * np.log10(abs(H(i)))
values.append(value)
plt.plot(frq, values)
plt.xscale('log')
plt.gca().xaxis.grid(True)

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#!/usr/bin/env python3
# -*- coding: utf-8 -*-
"""
Created on Thu Feb 28 11:00:18 2019
@author: oyvind
"""
import numpy as np
import matplotlib.pyplot as plt
def H13(f):
w = 2 * np.pi * f
return (w * 10**(-4))/np.sqrt(1+(w*10**(-4))**2)
def H2(f):
w = 2 * np.pi * f
return (1/np.sqrt(1+(w*100*10**(-9)*10**4)**2))
def H4(f):
w = 2 * np.pi * f
R = 99.76
L = 100 * 10**(-3)
t = L / R
return (1/np.sqrt(1+(w*t)**2))
frq = []
values = []
for i in range(2*10**4):
frq.append(i)
value = 20 * np.log10(abs(H4(i)))
values.append(value)
plt.plot(frq, values)
plt.xscale('log')
plt.gca().xaxis.grid(True)
plt.gca().yaxis.grid(True)

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#!/usr/bin/env python3
# -*- coding: utf-8 -*-
"""
Created on Thu Feb 28 11:00:18 2019
@author: oyvind
"""
import numpy as np
import matplotlib.pyplot as plt
def H13(f):
w = 2 * np.pi * f
return np.arctan(1/(w * 10**-4)) * 180 / np.pi
def H2(f):
w = 2 * np.pi * f
return np.arctan(w * 100*10**(-9) * 10**4) * 180 / np.pi
def H4(f):
w = 2 * np.pi * f
R = 99.76
L = 100 * 10**(-3)
t = L / R
return np.arctan(w * t) * 180 / np.pi
frq = []
values = []
for i in range(1, 2*10**4):
frq.append(i)
value = H4(i)
values.append(value)
plt.plot(frq, values)
plt.xscale('log')
plt.gca().xaxis.grid(True)

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#Digilent WaveForms Network Analyzer - Bode
#Device Name: Discovery2NI
#Serial Number: SN:210321A36D3D
#Date Time: 2019-03-04 13:47:34.600
#Start: 10 Hz
#Stop: 20000 Hz
#Steps: 151
#Wavegen: Wavegen1
#Amplification: 1 X
#Settle: 10 ms
#MinPeriods: 16
#Channel: Channel 1
#Range: 5.47148 V
#Offset: -3.64348e-05 V
#Relative: no
#Channel: Channel 2
#Range: 5.48107 V
#Offset: -6.42632e-05 V
#Relative: yes
Frequency (Hz),Channel 1 Magnitude (dB),Channel 2 Magnitude (dB),Channel 2 Phase (°)
10,-0.00537326,-0.00481132,-0.3339
10.5198,-0.00550897,-0.00468579,-0.350273
11.0666,-0.00553953,-0.00497733,-0.366327
11.6418,-0.00540155,-0.00537231,-0.38602
12.2469,-0.00550687,-0.00508884,-0.406273
12.8835,-0.00509335,-0.00539532,-0.427304
13.5532,-0.00553483,-0.00544864,-0.448588
14.2577,-0.00527835,-0.0057729,-0.469659
14.9987,-0.00519837,-0.00589985,-0.495311
15.7784,-0.00532765,-0.00593774,-0.520151
16.5985,-0.00538368,-0.00622925,-0.547678
17.4613,-0.00528162,-0.00670784,-0.57488
18.3689,-0.00546862,-0.00668217,-0.604199
19.3237,-0.00555204,-0.00687947,-0.634738
20.3281,-0.00533271,-0.00723183,-0.666323
21.3847,-0.00538782,-0.00742054,-0.701453
22.4962,-0.00546445,-0.00789399,-0.735715
23.6656,-0.00519679,-0.00848513,-0.774108
24.8957,-0.00538932,-0.00843235,-0.812998
26.1897,-0.00523701,-0.00917148,-0.853232
27.551,-0.00518192,-0.00980661,-0.898256
28.9831,-0.00530315,-0.00982177,-0.943569
30.4896,-0.00545199,-0.0100736,-0.991705
32.0744,-0.00528373,-0.0106913,-1.0408
33.7415,-0.00529,-0.0111226,-1.09468
35.4954,-0.0052797,-0.0118656,-1.14995
37.3404,-0.00554357,-0.0121321,-1.20827
39.2813,-0.00531512,-0.0130159,-1.27031
41.323,-0.00543937,-0.013854,-1.33445
43.471,-0.00540697,-0.0144741,-1.40109
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