Saturday, June 13, 2009
Thursday, June 4, 2009
Sample Final Exam
Tuesday, May 12, 2009
Photoresistors!! 5-11-09
On Monday we learned about photoresistors and had a robot day! Photoresistors are light sensitive resistors whose resistance decreases with the amount of light falling on them.
We will be using photoresistors on our robots for the "Follow the line" competition and for "Robot Sumo."
We've all seen photoresisitors somewhere in our lives.....for instance my car as an auto setting for my headlights to turn on and off. When the resistor has enough light falling onto it, it causes electrons to jump into the next conduction band. The resulting free electron conduct electriciy, and therefore low the resistance of the resistor.
To use this on our robots, we needed to figure out the resistance range of the resistor for different light intensities. We used the 'white' of the our white boards and the black of non reflective electrical tape.
Once this is figured out, interface the resistors using voltage dividers to your microprocessor. The photoresistors will control one or both of your motors. You'll want to think about how you want your robotto behave for the line following competition and also think about what you want your robot to do when it faces the white outline of the sumo ring.
Oh...Mason also did some cool stuff in class...no he didn't light either of the Peter's on fire, but he put stuff in a microwave that shouldn't have gone into it, and made sparks fly.
LRC Circuits - 5/6/09
We took a good look at phase angles and how to caluclate them and what they mean. Basically when looking at both current and voltage in an oscilloscope, current and voltage will both oscillate sinusoidally but not at the same time. The difference in which the current leads or lags the voltage is called the phase angle.
Phase angle (phi) = tan(-1)(XL-XC)/R = 2pi*delta t/T(dr)
Where T(dr) = the period of oscillcation of the driving emf.
Since it has been almost 10 years since I had to figure out the period of a function, I spent the entire class asking myself WTF? So it also might be really useful to know how to find the period;
Period(T) = 1/f
w=2*pi*f
We briefly went over the Root Mean Square Current and Voltage. Mason proved that the average current and voltage on always equal to zero, but the average power of the AC circuit is not equal to zero....ya we've all been zapped by AC circuit.
In general, your equations of Voltage and Current will look something like this for a LRC AC circuit in series;
If circuit is voltage diriven;
V(f)= Vmax*sin(wt)
I(f)= Imax*sin(wt-phi)
phi = phase angle
If circuit is current driven.
I(f)= Imax*sin(wt)
V(f)= Vmax*sin(wt-phi)
The circuit will still obey Kirchoff's rules.
Good luck on all of the H-dub!!
Wednesday, May 6, 2009
Tuesday, May 5, 2009
STRIKE #3
We took our tests last Monday, right? So... extra credit? XD
Monday, April 27, 2009
Wednesday April 22, 2009
Tuesday, April 21, 2009
More magnets and electricity! Hey at least nothing was melted...
So here it goes!
We started off first by getting the news that our last homework involved with chapter 28 instead of 27 only. Wait a minute, I thought that homework was on chapter 27 only. I guess that's why I did terrible on a couple questions (or maybe it was just me not realize that? Jeez...).
We then did experiements about Faraday's Law which involving wire loops and magnetic field. We found out that the more loops there are in the coil, the stronger the magnetic field of the coil is. Based on the results, we found out that the magnetic field of the coil is proportional to the current flowing through the wire and the number of loops there are in the coil.
We then learned about electromotive force, or emf. emf is from the potential difference generated magnetically. It's effected by the area, the number of loops, and rate which magnetic field changes (velocity) of the coil.
One thing that caught my interest at the end of the class was that Mason and Peter tried to demostrated something that reminded me about a phenomenon called Maglev, or magnetic levitation. This tech is used quite frequently in Japan's train system. Now, I don't know the exact detail of the system or the relationship between those two, so maybe professor Mason can explain a little bit about this? I know it's offtopic but I still find it rather interesting.
That's all folks! I hope you are still awake at this point after reading through all that! Celebration (?) is next monday so hopefully everyone is getting ready for it!
PS. Nerf offshore flow please. 100 degree weather in April is ridiculous 囧rz.
Wednesday, April 8, 2009
Wednesday April 8th, 2009
Tuesday, April 7, 2009
Working with Transistor
Monday, April 6, 2009
Wednesday, April 1, 2009
4/1 homework
any thoughts?
Tuesday, March 31, 2009
Monday March 30, 2009.
We should be covering Gauss's law (Chapter 22) on Wednesday for those who want to get ahead.
Monday, March 23, 2009
Day 8 March 18
F=ma
F=qV/d
and 2D- kinematics equations for the trajectory of the electron we were able to solve for d, and we realized that the deflection is proportional to Voltage(the higher the voltage the greater the deflection). we needed this information in order to understand the second part of class, which delt with function Generators and Oscilloscopes.
For the second part of class we played around with a function Generator, also called (wave generator) which is a device that can produce different voltages in a regular pattern. we connected a speaker to the wave Generator and we played around with different dials and bottons on it and we noticed the sound changes: 1) changing the frequency changes the pitch of the sound. 2) changing(increasing) the amplitude makes the sound louder . 3) changing the function(sine, triangle or square) changes the timbre of the sound coming out of the speaker. After that we learned how to use an Oscilloscope and we connected in to the function Generator and noticed how changing the frequency and amplitude changes the graph(motion of electron)displayed on the screen of the Oscilloscope. we also learned how to calculate the period by just looking at the graph.
for the last part of lab we built capacitive filter cicuits on our breadbord, and we conected it to the Oscilloscope and the function generator. then we collected data for the changes in amplitude and voltage when we change the input frequency. then we graphed the data we got using loger-pro. and we noticed the constant votage drop in the first circuit(capacitor and resister), and the constant voltage in the second circuit(two resisters).
GOOD LUCK ON THE EXAM!
O MY BAD, (CELEBRATION OF KNOWLEDGE!)
Friday, March 20, 2009
Practice test for celebration 1
Peter's Practice Test
The answers for my practice test will be posted Monday night. I will attempt to have the answers for Masons up on Tuesday night or Wednesday morning. Good luck with studying =)
Edit** For problem one, there is a positive test charge at the point where you need to find the force and electric field.
Problem two, it should be surface charge, not linear
Sunday, March 15, 2009
Day 6 March 11, 2009
Generally, we use the sum of current and voltage in a loop are both equal to zero to find the current. First, The junction rule I1=I2+I3 will setup the first formula, and the loop rule will create the other two formulas. Then, we can do some algebra for the unknowns in the formulas to find the current. After that, V = IR can be used to find the voltage by current and resistant. Finally, use P = IV to get the power of each resistor, and add them up to get the total power.
I did the questions wrongly, but I found my mistakes soon. All loops have to in the SAME direction. It was a good quiz because I even did not find I was doing something wrong in the homework!
The second part in class was slightly different with the class. We were learning something which is not in the book! The robot project was started! Before touching the hardware, we had to learn some theory for that.
What we learned in this part was the protocol for the devices to communicate. We learn how it works. It translate ASCII code(American Standard Code for Information Interchange), which is commonly used in computer system to represent characters and to some digital signals. The character in ASCII code first translates to 0 and 1, then it reverses the order of the code then translates to positive voltage for 1 and positive voltage for 0.
The third part was doing some labs. We use a voltage divider, a potentiometer to build a bridge circuit to measure the temperature. We take the voltage in the freezing and melting point, which are already known as 100 and 0 degree Celsius, to calculate the room and the body temperature. From the result, we will get a line which show that they are in linear function.
An interesting thing in the lab is that we found this device is really sensitive. It could even catch the temperature change caused by our human body moved away for a few centimeters!
Friday, March 13, 2009
Solving circuits with matrices
http://docs.google.com/fileview?id=F.f9c99189-1d8a-4dce-8ad0-9bd68b62ef01
Wednesday, March 11, 2009
Hmm
Here's one that's PC, kosher, etc.
SI times are set for the rest of the semester. I have no intention of changing them anymore. Hope to see all there!
Tuesday, March 10, 2009
Day 5 Physics 4B March 9, 2009
Really long recap:
Some important announcements were made before class today. First of all Peter set a new SI session date. His new session will be on Friday from 10:00am-12:00pm. I cannot confirm this as a static date/time so you’ll have to prod him for more information whether it will change or not. His other sessions that are an hour before class will remain the same for all your last minute homework needs. Incase you didn’t know an hour before class is 11:00am-12:00pm (class starts at 12:00pm). That brings me to the next announcement. BE ON TIME! The more you guys are late the more often we have quizzes. I don’t know whose idea it was to reward the people that are on time with quizzes but something seems quite off with the logic.
In class today was more of a problem solving day with some hands on but not quite as much as the previous week. We covered sections 4.5 to 4.13.1e in the packet in the seamlessly short 220 minutes we have together; although most of us didn’t get even close to part E so we should be continuing it on Wednesday. The first lab we worked on involved comparing which resistor gets hotter (spoiler: the one that causes more pain gets hotter). The purpose of this was to see whether more or less resistance causes more or less heat respectively. The answers may not surprise you. To prove this Mason hypothesized it would be less painful to light a 5 ohm resistor on fire than to hold it. After a lot of waiting and smoke the flames never emerged and we were all disappointed with Masons promises not delivered. With the lesson of not lighting resistors on fire learned , or in my case “try this at home until we get results”, we next learned how to identify the resistance of a resistor by the color coding on the resistor itself. There are some easy rhymes to remember the BBROWGBVGW that can be found with Google but posting there here might be frowned upon for not being PC (about 80% contain rape for red and it only goes downhill from there). After practicing the codes for a while we moved onto the meat of the day; Resistors in series and parallel calculations by either brute force or Kirchoffs Law. I will make the lessons learned from these at the end of the blog in an easy access location. This part of the day dragged on endlessly for what seemed like eleventeen hours. But when it was all said and done I shall, along with many others, be harassing Peter for help on Friday about Kirchoffs law (since when was a law ever easy to understand). In our curiosity about the 5 ohm resistor that was “lit on fire” we decided to test the change in its resistance after being exposed to high heat. There was a minimal change in resistance as recorded by the multimeter. Those lil’ guys are Tonka tough.
Notes:
One of the more interesting things we did as a quick refresher was we wrote V, I, Resistance and P in terms of SI units. They turned out to be:
-V = ( Kg * m^2 ) / ( s^2 * C )
-I = C / s
-Resistance = ( Kg * m^2 ) / s
-P = ( Kg * m^2 ) / s^3
Some handy notes for series/parallel resistors were:
-In series the voltages will add together but the currents will always be the same.
-In parallel the voltages will always be the same but the currents will add together.
-Add the resistances together for total sum in a series: R1+R2+R# =Rtotal
-For parallel multiply the resistance of each resistor then divide by the sum of all the resistors: (R1*R2*R#)/(R1+R2+R#)=Rtotal
Kirchoffs Law:
-The algebraic sum of currents into any junction must be equal to zero.
-The algebraic sum of the potential differences will also total out to zero.
-As long as proper signs are used Algebra or matrices can be used to solve these problems relatively easily.
-Page 888 of the book has more details on this (what a conveniently easy number to remember).
Fun things:
-On March 9 1934 Yuri Gagorin was born. He was the first man to go into space. (closest fun fact related to Physics I could find for March 9). On the plus side if you look at his picture on Wikipedia he has more medals than Michael Phelps.
-As an apology for such a sad fun fact here’s an awesome Physics related game to play when you’re bored… but not bored in class… unless you’re Mason… or Peter…
http://www.fantasticcontraption.com
Whenever you finish a level go look at some of the other ones people have created. They make you feel really bad for not being that clever.
In summary:
Read sections 26.1 and 26.2 of the book as well as 4.8 in the packet to recap everything we did today.
Sunday, March 8, 2009
Day 4 03/04/09
Today is another exciting day at our Physics4B class. At the beginning of the class, we took our first quiz of the semester. I was a little bit nervous at the first, but once I look at the quiz, it is exactly the same as our homework, and we also can use the notes from homework. I am very happy that I know I get a 10/10 on the quiz, and it makes my day.- During the class, we did several experiments about series and parallel circuits. In the first experiment, we found out that in a series circuit both V and I are the same, but in a parallel circuit that the parallel bulb split the current. Then, we did an experiment to find out the resistance. We set up a circuit and use the V meter and I meter to find out both V and I of the resister, then use logger pro to get the resistance. I like today’s experiments and we learn a lot of things from them.
- At the end, we had the change to use the multi-meter, it is pretty cool because you can measure a ton of things from it. Professor Mason also told us the multi-meter only measure the V from the object that makes it more awesome. Anyways, the best thing of today is I did well on the quiz, and the experiments are pretty good. Look forward of Monday’s class, by the way this weekend we got change the time one hour early, it means we have an hour less of sleep. Hope to see all of ur guys on Monday, good luck on all the classes!!!!!!!!!!
Monday, March 2, 2009
Day 3 3/2/09
Before we played with our light bulbs and batteries, we continued in the packet from 2.9 to 3.8.
finishing up the subject of potential energy. That brought us in the topic of Equipotential surfaces. A big fancy word for a very simple concept. dont freak out with all the lines, just remember the equipotential lines always go perpendicular to the direction of the electric field lines.
The best news all day was to cross out section 2.11. we're not doing it, ever. (songs of rejoice)
Now after all the hard math and complicated integrals we got to simplify our mines and connect the dots. or the circuit. playing with completing circuits to power up the light bulb, or 3 light bulbs, and drawing the circuit diagrams for them. learning the ideas and concepts of current, resistence, and voltage. were all basic in concept, but all vital for any further process.
But if i could get you to remember one thing from this whole day, I would have to say, GET TO CLASS ON TIME!! Prof Mason has been nice enough to grace us with no quizzes but because of the lack of bodies there at 12 he is threatening us. so for the sake of me you and the guy next to you, please get there on time so we can avoid these annoying quizzes!
see you all wednesday, at 12 noon!
Friday, February 27, 2009
Thursday, February 26, 2009
From your SI
My contact information is the following:
email: peter.s.tran@gmail.com
MSN Messenger: peter.s.tran@gmail.com
AIM: jianeses
feel free to contact me anytime with emails or IM's and I'll do my best to get back to you in a timely fashion.
Ah, BTW, a hint for the blogs. Equations are good =)
Physics Day 2 (02/25/2009)
Well, if you weren't in class, you missed out on your chance to purchase a notebook from Kara. You will need one for our upcoming project to record your daily progress and what have you. (Make sure it has graphing paper in it.) Kara will have them in class Monday, otherwise, get one for $1.80 at Staples.
During class we followed along pages 9 through 16 (1.6 to 2.9) in our 101 page packet. Yeah, I counted (three times, actually). Do you need a special stapler to use those INDUSTRIAL SIZED staples? hmmm...
Anywho... most important concept of the day was electric potential which can, in many ways, relate to gravitational potential energy. Electric fields are, indeed, conservative and therefore work done by an electric field is INDEPENDENT of the path taken. (This is key, folks)
Then we remembered that the only thing we love more than integrating, is integrating from inifinty. Yes, integrating FROM infinity. Remember how we used this trick for gravity? Yeah, now we use it to find the electric potential at a distance r from a point charge by integrating from inifinty to r. Remember, the electric (and gravitationa) potentials at inifinity are ZERO.
One last thing: When dealing with electrons and protons in an atom, we found their gravitational attraction to be SO small as compared to their electrical attraction, it is NEGLIGIBLE.
Now a little inspiration:
Somebody said that it couldnt be done,
But he with a chuckle replied
That "maybe it couldnt," but he would be one
Who wouldnt say so till hed tried.
So he buckled right in with the trace of a grin
On his face. If he worried he hid it.
He started to sing as he tackled the thing
That couldnt be done, and he did it.
With that being said, lets all get an A this semester!!!
Monday, February 23, 2009
Physics 4B Day 1
Best thing about Day 1: WE GET TO SET THINGS ON FIRE!!!
Worst thing about Day 1: We don't get to do that till later in the semester.
Anyways, first things first, we all received a MASSIVE GIANTIC SUPER HUMONGOUS PACKET that we will (assumedly) complete by the next
After Mr. Mason introduced himself and told us his life story, we got to start working on our MASSIVE GIANTIC SUPER HUMONGOUS PACKET. After he organized everyone into six different groups of 3 people each, we began working. So, we went got ourselves some scotch tape, a rod stand, glass/plastic rod, a patch of fur, and a piece of silk, and we used them to answer the questions in the packet by performing little experiments. Then we learned about Coulomb's Law.
Now we get to a good part... ELECTROCUTING PETER!!!
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Well... not really... more like having him conduct various experiments on a Van de Graaf generator.
First, Peter attached strips of paper all around the metal ball on the generator. When the generator was turned on, the ends of the strips lifted into the air. This happens because the strips all acquire the same charge and repel each other.
Second, Peter touched a flourescent light to the metal ball on the generator. The flourescent light glowed from the point it touched the generator to the point Peter's hand was holding. The charge induced on the light caused it to glow, and the charge flowed through the light to Peter.
Third, Peter placed a pie tin filled with paper confetti ontop of the generator. When the generator was turned on, the paper confetti flew out of the tin. Both the paper and the tin acquired the same charge, so the paper was repeled from the tin and flew out of it.
Fourth and lastly, Peter blew bubbles (after a failed first attempt haha) at the generator. The bubbles fly towards the generator then are repeled from it once they get close. Because the bubbles are uncharged, they are attracted to the charged metal ball, but once they become charged by touching the ball, they are repeled.
Afterward, for some obscure reason, Mr. Mason put the metal ball from the Van de Graaf inside a microwave. Unfortunately, nothing happened. Then Mr. Mason put aluminum foil inside the microwave, and we all watched it FRY or rather get electrocuted. Visually, it was like lightning trapped in a box.
For the rest of class, we worked on the packet until we had finished up to section 1.5.
At the end of class, Mr. Mason gave us the class syllabus and Mastering Physics homework.
In short, today's theme was:
Welcome to Physics 4B
Tonight you need to do your first mastering physics assignment:
(www.masteringphysics.com)
You also need to read the syllabus, find at least two mistakes and then email me those mistakes.
