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Registered Member #1062
Joined: Tue Oct 16 2007, 02:01AM
Location:
Posts: 1529
1: That would be difficult, the best i can think of is thinking of the cone as stacked cylinders. "resistance (Rt, Omega/cm2) is derived from the following equations (1) Rt = 1/S = rho L/(pi (r/2)2 F) where rho is copper resistivity (1.67 × 10-6 Omega cm), L is wire length (3.6 × 10-3 cm), r is cross-sectional diameter of copper wires …."
Registered Member #2099
Joined: Wed Apr 29 2009, 12:22AM
Location: Los Altos, California
Posts: 1716
wylie wrote ...
I can't shake the feeling that that's some sort of homework......
Me too, esp. as first post by a newcomer. Problem #1 needs a bit of calculus or cleverness, unlike #2. How 'bout if we all let this rest a week before contributing answers?
[edit] Came back to report an attitude adjustment. * Would not frown on prompt homework help, if OP says it's homework. * Giving answers is inappropriate, esp. when OP does not show any effort. But giving hints (Dr Slack beat me to it) is what teachers, parents, and 4hvers do.
Registered Member #2474
Joined: Fri Nov 20 2009, 01:22AM
Location:
Posts: 4
Its sort of 2 question i found out in a book but without explaination and answer..... thats y i tried to post and ask it..... thanks for all the suggestion. will look into it.
Registered Member #2099
Joined: Wed Apr 29 2009, 12:22AM
Location: Los Altos, California
Posts: 1716
Rodney wrote ...
Hi, Thanks for all the help I have successgully done question number 1... Can anyone help me check whether i did it correctly or not?
Hi Rodney. Looks pretty good, but I got a different answer (unreviewed) by doing just a single integration along the length. Hint: try, early on, replacing r(x) with x * r1/x1. (I am using x instead of lowercase l for typographic clarity).
Then where you get the factor 0.9 after integrating r^-2 from 1 to 10, I integrated x^-2 and got the very similar form R = (0.9 * x1)/(sigma*pi*r1^2) = (0.1 * L)/(sigma * pi * r1^2 ). Solving for R = 50 ohms, I got L = 3 * a power of 10 * pi meters. Want to try matching that? Be careful with centimeter/meter conversion.
If the real conductivity of copper were used, I think the length of 50 ohm tapered bar would be roundly geodetic. Could be wrong!
You did so well, how can problem 2 be a problem after Dr Slack's hint? [edit]If you can visualize the drawing in 3 dimensions, think about applying the principle of symmetry. Valuable in current spreading problems. Don't be deterred by infinite current density & voltage drop at point sources; they are nicely behaved everywhere else.
Registered Member #1792
Joined: Fri Oct 31 2008, 08:12PM
Location: University of California
Posts: 527
I think for the second problem they are expecting you to assume that the current density will spread out evenly across the sphere as the cross-section expands, in which case it becomes a simple matter of geometry.
But I don't think that that is what would actually happen if you were to actually solve the problem, I suspect that the current will be bunched up more at the center of the half-sphere. I think a full solution would need to solve the differential equation presented by div(J)=0, using image theory where you can replace the (presumably perfect conductor) at the base of the half-sphere with the mirror image, i.e. make it a whole sphere. Then you define dot(normal, J) = 0 on the sphere's surface, as no current flows outward, except at the top and bottom where you have a point source J = 50A. Sounds to me a like a very tricky problem to solve analytically, but probably not too bad numerically.
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