Gauss Law = q,enclosed/eplsillon not. We divided a couple of charges into different enclosed areas, s1, s2, s3 and drew the flux lines from each charge.
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We had q1 be negative( top right), q2 and q3 are the positives one. Flux lines are going towards q1. The flux for each S (surface), s1 ,s2 ,s3 can be counted by having flux lines going out - flux lines going in. If the net result is positive then more flux went in the surface, if net result is negative more flux went out of the surface. |
Another picture demonstrating flux.
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Electric field only effects the normal of a surface. |
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Flux inside is zero in this enclosed surface. |
Prof. Mason then asked us what would be the best answer if one was in a lighting storm. Our answer was to stay inside the car. It would act like a Faraday cage.
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The white board Prof. Mason picked out. |
We then explained the demonstration of a lighter in the microwave. And when to use the right symbol for E calculations.
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We explained the plasma and also E = sigma/Epsilon not. And when to use lambda, sigma or rho in our E calculations. We also explained what the fork did in the microwave. |
We then derived the volume of a sphere and integrated in terms of r + dr.
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The white board Prof. Mason showed as example. |
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Our work of the same thing. dr to the powers of 2 and 3 are small so they go to zero. Only 4pir^2dr is left and is useful. |
We then did some Active Physics questions that asked to find Q if the r's are different. The final answer was 1/8Q.
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We set the lesser r on top and the bigger r on bottom. Did some canceling and was left with 1/8Q. |
We then did use Gauss law to find E.
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E = q/e0, the 4pi and e0 turns into K. E then becomes E= Kq/r^2. Similar to Coulomb's law. |
Prof. Mason then pleased us by showing us what different types of things do when they are put inside a microwave. We did some prediction for some.
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Fork, our prediction was the fork would cause sparks. Nothing happened. |
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Cd, our prediction we would see sparks. Sparks happened. |
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The damage to the Cd by the sparks caused by the small layer of aluminum coating on it. |
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Our prediction of Soap. Did not work, but the soap would become foam. |
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Picture of something. |
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Picture of soap. |
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Very beautiful colors when microwaved. Melted a whole through it. |
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Picture. |
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Our predticion was that it would expand and blow up. It did not but showed a light blue glow. |
We then moved on to answer some Active Physics demo and questions. The first was a slew of questions about flux.
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All questions answered. Used Gauss law to find flux. Which was 40,00N/C. Flux in a smaller radius is zero. The charge is 2.39*10^4 C/m^3. Rho*V is equal to E is = 45,000 N/C. |
Prof. Mason then asked us to E for a cylinder. Sa = 2pirL + 2pir^2. Lambda = q/l.
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We plugged in the numbers to the equation and got E = 4.798 N/C for the cylinder. Used q/L. The second term goes to zero since the is no perpendicular flux going through it. |
For got to mention the graph we found from E(r). E field grows as the radius grows.
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The E is greates when little r is equal to R. After little r becomes greater then R, E drops by 1/r^2. E(r) = qnotr/R^3. |
Summary:
We found Gauss law to be useful in finding E. Flux inside different S have different flux depending on the q inside and the q outside of the S. Flux is = integral EdA. The usefulness of 4pir^2dr found for spheres. Changes in r could effect Q greater then one would think. Gauss laws is similar to Coulomb's law.
Microwaved a whole bunch of things.
Learned that little r inside of big R stores different Flux. Found the graph of E versus R.
Found the Surface area for a cylinder Sa = 2pirL + 2pir^2. Lambda = q/L.
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