31 January 2006
Solution to first homework: a ring of charge
Please let me know if you have questions about the solution, or if you think / don't think similar exercises would be helpful in future.
27 January 2006
Question: E=V/d or V=-Ed? (to minus or not to minus)
I was wondering why the notes from class say that for uniform Electric fields E=V/d, while the textbook and WebTA say that V=-Ed. Why is there no negative sign in the one case, but the negative is included in the other?
That is a very good question. I can first tell you that the reason my formula and the formula in the book are the same is that I copied mine out of the book. ;) I can also say that Prof. Altounian's notes are correct.
To get to the heart of this matter, really we have to think about what V is and what E is. The electric potential, V, is a scalar quantity. That is, it has a magnitude at a particular point in space, but no direction associated with it. But the electric field, E, is a vector quantity. This means it has both a magnitude and a direction. So if we look at a simple formula for the electric field, like E=V/d, we have to think this isn't the full story... how do we relate a vector and a scalar?? where is the direction part of E??? Well, it isn't there. Really all we get is the magnitude of E. So, whether you stick a negative sign there or not, you have to determine the direction of the electric field in another way (by determing where a high potential is and where a low potential is).
So, why did the text book (and myself) bother putting a negative sign there? Well, it comes from the calculus relation between E and V. If you have a map of V over an area, the electric field points downhill, so when you look at it from within a differential formalism you need the negative sign (so I'm used to seeing it that way).
In any case, I mean to change my webTA pages to agree with the class notes on this point. And the moral of the story is that since E is a vector you have to determine the direction as well as the magnitude.
26 January 2006
Server unavailable Jan 27 05:00-07:00
please be advised that tomorrow (friday) the webserver (and its filesystem) will be unavailable between 05:00 and 07:00.
This will effect the webTA home (site with all examples etc), but not the blog site.
25 January 2006
Posting questions
Also, I think everyone is getting the idea about asking questions by posting comments. Don't worry if they don't appear right away, I have to clear them first. I would prefer, unless you are having a problem with the site, that you don't email me with questions. It's just easier to have them all in one place on the blog, and possibly helpful to others that might have been wondering the same thing.
Thanks everyone for your continued participation, so far I think this is working out quite well. :)
Question: 2 Charges Dropped in an Electric Field (Chapter 17, #68)
I am confused on what the equation for conservation of energy should be for this problem....Should we consider potential energy due to the height?
For example I assumed the equation to be: mgh(before)+PE(before)=KE(after)
The question states: "Near the surface of the Earth there is an electric field of about 150V/m which points downward. Two identical balls with mass m=0.540kg are dropped from at height of 2.00m, but one of the balls is positively charged with q1=650μC, and the second is negatively charged with q2=-650μC. Use conservation of energy to determine the difference in the speed of the two balls when they hit the ground."
Whoo-ee! That's a nice problem, it incorporates several different ideas, just the kind I hated as a student, and see the value of now when I teach. :)
Your energy equation is mostly correct, but we need to figure out the signs of the energies.
Let's first draw a diagram, because I find that problem a mouth full. (I will put in the electrostatic forces, but not gravitational... we all know that points downward anyway).
So we have the positive charge (drawn on the left) experiencing a downward force due to the electric field, thus as it falls (down) it's electric potential energy will be decreasing, just as it's gravitational potential energy will be decreasing. However, for the negative charge (drawn on the right), the electrostatic force is pointing upward, opposing the falling motion, so it's electric potential will increase as it falls.
We will have to look at the conservation of energy each charge separately. Let's start with the positive charge:
PE(electric)+PE(gravitational)=KE
qEh+mgh=(1/2)mv12
(note that I used h for the distance the charge travels through the electric field).
Now let's look at the negative charge:
PE(gravitational)=KE+PE(electric)
mgh=(1/2)mv22+qEh
When plugging in the numbers, disregard the sign of the charge. I have included it already by determing whether the electric potential energy increases or decreases. Alternatively you could have used the energy equation for the first charge and plugged in the sign of the charge to get the same thing. Personally, to avoid confusion with signs, I think it's better to work through the logic of what's going on than to plug in signs, but that doesn't make the other way wrong.
So, using the energy equations for each ball, you can solve for the final velocities. I have confidence that you can all plug in numbers, so I will leave it at that. Hope this helps, and if you have any further questions feel free to post a comment.
Question: Increase plate separation, increase energy stored in capacitor
If two plates of a capacitor with constant charge have their separation doubled, the energy stored also doubles. I'm confused as to why this happens, since I thought E-stored was related to C, and C decreased as distance of separation increased. I'm looking at the equation Energy Stored = 0.5CV^2.
You are right that the energy stored in a capacitor if related to C, the capacitance. However, you have to consider what is being held constant as the separation doubles. If you look at the equation: U=(1/2)CV2, you will notice that U is proportional to C, however you have a factor of V2 that changes in a way you can't determine directly. If instead, you re-write the equation substituting in V=Q/C, so that you have: U=(1/2)Q2/C, then you know that Q is a constant, so we can talk about U being proportional to 1/C. Thus, as C decreases, U increases.
It might help you to look at the example I posted on this if you haven't already: Chapter 17, #50. Note also that since the amount of energy stored in the capacitor is increased, work must be done to increase the separation between the plates.
24 January 2006
First homework: a ring of charge
If you're interested you can get to it from the homework page.
Good luck, I will post an answer in a few days or so.
Topic open: Resistance and Resistivity
The following topic is now open for questions: Resistance and Resistivity.
To pose a question, please post a comment to this post by clicking on the comments link below.
I realize you may still have questions regarding capacitors, feel free to continue asking questions on old topics (by posting comments to the appropriate topic post).
23 January 2006
Popups?!?
If anyone has seen this happen on the blog, or the static tutorial page, please let me know and I will remove the counter immediately.
Thanks, and my appologies to anyone experiencing these popups.
Edit: I have removed the webstats4u counter and replaced it with another that claims it will not put ads on the sites that use it. Still, let me know if anything strange happens. (2:14 PM Jan 23 2006)
Question: Capacitor miscellany
here are my questions about capacitor:
1 #51 b)Why doubling?
The energy stored in a capacitor is given by:
U=(1/2)QV=(1/2)CV2=(1/2)Q2/C.
In Ch. 17, #51 (b) we are told that the amount of charge on each plate is doubled (ie. Q is doubled), and the capacitor remains connected to a battery (ie. V is held constant). So, we can look at an initial energy, U0, and a new energy after the charge is doubled, U':
U0=Q0V
U'=Q'V=(2Q0)V
The ratio of the new energy to the old is then:
U'/U0=Q'V/Q0V=2
So, indeed if the charge on the capacitor is doubled, the energy stored in the capacitor is doubled.
2 Say, we have 2+Q on the left plate and 2 -Q on the rite, can I just add 1 +Q to the left and add nothing to the rite? Or it is a must for me to add the same amount of charges to both sides?
You must add the same amount of charge to both sides. (Check out the Ch. 17 summary on where it describes a capacitor.) If you added more of one charge to one side than the other, the net charge of the capacitor would be non-zero. I'm not sure what exactly would happen, but it wouldn't be a simple capacitor anymore and wouldn't follow the behaviour we've been discussing. Sorry I can't give a better explanation than that.
3 If I added 1 +Q to left and 1 -Q to rite, the total charge should be +2Q, rite?
Well, the net charge would be zero, the total amount of charge would be |2Q| (those || are to show we are talking magnitude/absolute value and disregarding the signs), but the charge on the capacitor (the "Q" you use in the capacitor equation) would be 1Q. The measure of charge that matters in a capacitor is how much you have separated off to each plate, so it is this charge you consider.
4 #77b) what i did was PE/2=1/2*m*v^2, what is wrong with my solution( i know it must be wrong -_-||)?
I had a student ask this question last year, I think the answer given there will help you also. Check out electrostatics: previous student questions, it is the second item on the page.
I believe your problem lies in the factor of 1/2 you are using for the potential energy... I'm not sure where this comes from, and I'm pretty sure it isn't necessary. ;)
Good Luck, hope this helps. As always you can ask follow-up questions.
18 January 2006
Topic open: Anything Capacitor
To pose a question, please post a comment to this post by clicking on the comments link below.
Question: Back-to-Back Capacitors (Ch 17, #41)
One student asks: "I was able to find the number of charges using Q=CV...but I have no clue how to solve the question."
Another asks: "I figured out the total charge after charging to batteries, but I dunt understand why they made "the positive plates connected to each and the negative plates connected to each other" and I cannot get the answer either. Another question from #41: they said "the potential difference across reach". Does it have the same meaning of the voltage of a battery?"
The question states: "A 2.50-μF capacitor is charged to 857V and a 6.80-μF capacitor is charged to 652V. These capacitors are then disconnected from their batteries. Next the positive plates are connected to each other and the negative plates are connected to each other. What will be the potenial difference across each and the charge on each? [Hint: charge is conserved]"
Ok, so it seems there is some degree of confusion about this question and how to handle it. The first step is to calculate the charge on each isolated capacitor using: Q=CV, as suggested by the first student. The total charge when they are put together will be the sum of these two charges. You will have:
Q1=(2.5e-6)(875)
Q2=(6.8e-6)(652)
Qtotal=Q1+Q2
The second question here actually holds a key part of the answer, and again, it is about interpreting the wording of a question. What does it mean when they say "the postive plates are connected to each other and the negative plates are connected to each other"? Let's draw this situation...
Notice that by connecting the terminals of the capacitors with like charge we have essentially placed them in parallel. So, we can treat them like parallel capacitors and find the equivalent capacitance of this arrangement. For capacitors in parallel, we have: Ceq=C1+C2.
Now we know the total charge on the two capacitors, and the equivalent capacitance of the two. We can now treat them as one capacitor with the total charge Qtotal and equivalent capacitance Ceq to find the new voltage across both (note that the voltage across things in parallel is always equal).
Qtotal=CeqVnew
Vnew=Qtotal/Ceq
To address the second student's last question regarding the potential difference, the potential difference here is somewhat similar to the voltage across a battery. A battery's job is to raise the potential energy of charges passing through it, it puts more positive charge on one side and more negative charge on the other. The same is happening here, on one side of the two capacitors there is more negative charge and on the other there is more positive charge. So, we say there is a potential difference or a voltage across the two capacitors.
Hope this is helpful, if you have any follow-up questions please post a comment.
17 January 2006
Question: One charge, E-field and force
Hi, I was wondering how to calculate both a force and an electric field when you're only given one charge. For example, if I have a positive test charge q, and a positive charage Q1 r distance away from the test charge... I'm confused on how I can calculate the force vector (resultant) in order to set up a triangle and find the x and y components of the force (same for electric fields).
If you are given only one charge, and no electric field anywhere due to some other arrangement of charges, then all you can do is calculate the electric field due to that one charge. In this case, you can determine the electric field at a point some distance (r) away. The direction of the electric field will be the same as a force would be on a positive charge if you put one there, but the magnitude of this test charge (q) is divided out (E=F/q). Remember that for a point charge, the electric field points radially outward/inward from the positive/negative charge. This makes sense if you think about putting a positive test charge anywhere around the charge you are given, as the force between the two will be along the direction of the separation.
You might also be asked about a charge in an electric field (usually a uniform one, since that's easiest to deal with). In this case you can determine the force on the charge due to this external electric field by making use of the definition of electric field: E=F/q. Flip this around, and you have: F=Eq, which can be very useful. Let's say you have an electron in a 1 V/m (N/C) uniform electric field pointing north. The magnitude of the force on the electron will be: F=(1N/C)(1.6e-19C)=1.6e-19N. The direction of the force will be south, since the electron is negatively charged and the direction of E is defined as the direction of force on a positive charge.
I hope this helps, please follow-up if I haven't answered your question here.
sorry!
Edit: I will also be notified by email now whenever a comment needs to be cleared, so I shouldn't miss out on your questions again!
Question: Charge transfered between plastic balls (Ch 16, #22)
i have an r, an F and constant k....im not sure how to go about this, but i solve for Q1*Q2, and then not sure where to go from there. if the first ball is uncharged , does that mean Q1 is 0 coulombs?
The question states: "A charge Q is transferred from one ball to an identical ball 12 cm away. The force of attraction is then 17 mN. How many electrons were transferred from one ball to the other?"
So, the key thing to pick up on here is that the balls are initially uncharged (Q1=Q2=0). This means that after charge is transferred between the two balls the net charge, Q1+Q2, will be zero. If we use this fact, we can see that Q1=-Q2. So, since a charge is transferred from one ball to the other each now has an equal but opposite charge, let's call it Δq. So, we can say that Q1 now has a charge of +Δq (a positive charge), and Q2 now has a charge of -Δq (a negative charge).
Now we can use the equation for the electrostatic force between two point charges to solve for Δq as you suggest.
It is worth noting that there were two ways we could have determined that the balls had opposite charge from what is given in the question. We used the fact that the balls are uncharged, telling us that the net charge after transfer is zero. We could also have used the fact that the force is attractive to determine that the balls are oppositely charged. But... we still would have needed to know that the magnitude of the charge on each was equal from the zero net charge. Often though, the wording of a question contains more information than you might suspect at first glance, so it is worth looking for hints like this.
You might also find the following posted example helpful: Chapter 16, #21 which also involves two charged spheres. The only difference is that in this example the net charge of the two sphere is not zero.