The resistor cube problem

C

Chris Carlen

Guest
Hi:

Guy Macon wrote:

"Here is a classic that really shows the difference between algebraic
and RPN: calculate the resistance between points (a) and (b) using
only a calculator - no drawings or equations on paper.


(a)-- *----------- ONE OHM -------------* V1
|\ |\
| O O O
| N N N
| E E E
| |
| O O O
O H H H
N M M M
E \ V2 | \
*---- ONE OHM --------------------* V6
O | | |
H O | O
M N | N
| W | E
| | | |
| O | |
| H | O
| M | N
| V3 | | E
*----- ONE OHM -------------------* V4
\ | \ O
O | O H
N | N M
E | E |
| |
O | O |
H | H |
M | M |
\| V5 \|
*------------ ONE OHM ------------*--(b)"


I found this intriguing because it seemed silly that I could spend all
weekend studying Fourier transforms and "advanced" stuff like that, and
then be put off by a simple resistor problem. So I gave it a try...

I am thogroughly impressed by any folks who can solve this by eye, using
just the calculator's "arithmetic" capabilities whether it be RPN or
algebraic input.

I had to resort to pencil and paper and came up with the following
matrix solution for the node voltages for attaching a 1V source to
terminal A and ground to terminal B:

[ V1 ] [ 3 0 0 -1 0 -1 ]^-1 [ 1 ] [ 0.6 ]
[ V2 ] [ 0 3 0 0 -1 -1 ] [ 1 ] [ 0.6 ]
[ V3 ] [ 0 0 3 -1 -1 0 ] [ 1 ] [ 0.6 ]
[ V4 ] = [-1 0 -1 3 0 0 ] * [ 0 ] = [ 0.4 ]
[ V5 ] [ 0 -1 -1 0 3 0 ] [ 0 ] [ 0.4 ]
[ V6 ] [-1 -1 0 0 0 3 ] [ 0 ] [ 0.4 ]


Thus, R= V / Ib = 1 / (3*0.4/1) = 1/1.2 = 0.8333 ohms

Confirmed in LTSpice.

Fun problem. Wasn't what I had originally planned for my first hour of
the day.

Clues as to the "by eye" solution would be appreciated. I am no genius,
so usually must resort to methodical techniques such as writing out the
node voltage equations which is what I did after puzzling over it for 30
minutes. I thought a lot about superposition approaches, and re-wrote
the circuit in a planar form with one source applied to one of the three
branches attached to "a" with the other two grounded. There are some
symmetries that become more apparent after planarizing that could lead
to some further superposition approaches from that point. But is all
seems like more of a pain in the butt and more prone to error than
writing the node voltage eqns. So while a keen eye might come up with
an elegant solution, sometimes the brute force method delivers a result
long before that spark of insight hits, usually in the shower at the end
of the day (or week).


Good day!





--
____________________________________
Christopher R. Carlen
Principal Laser/Optical Technologist
Sandia National Laboratories CA USA
crcarle@sandia.gov
 
Oops, here's the corrected version of my post:

In article <C.D.H.Williams-8F6022.19003924052004@news.ex.ac.uk>,
Charles DH Williams <C.D.H.Williams@exeter.ac.uk> wrote:

In article <c8ta9v0183o@news4.newsguy.com>,
Chris Carlen <crcarle@BOGUS.sandia.gov> wrote:
Clues as to the "by eye" solution would be appreciated.

The symmetry of the problem allows you to assert that
VX = V1 = V2 = V3 and VY = V4 = V5 = V6 so you can join the
points at equal potential by piece of wire and not change anything.
This leaves you with three resistors in parallel from a to X,
six from X to Y, and 3 from Y to b, i.e 1/3 + 1/6 + 1/3 ohms.

Charles.
 
Charles DH Williams wrote:
Oops, here's the corrected version of my post:

In article <C.D.H.Williams-8F6022.19003924052004@news.ex.ac.uk>,
Charles DH Williams <C.D.H.Williams@exeter.ac.uk> wrote:


In article <c8ta9v0183o@news4.newsguy.com>,
Chris Carlen <crcarle@BOGUS.sandia.gov> wrote:

Clues as to the "by eye" solution would be appreciated.

The symmetry of the problem allows you to assert that
VX = V1 = V2 = V3 and VY = V4 = V5 = V6 so you can join the
points at equal potential by piece of wire and not change anything.
This leaves you with three resistors in parallel from a to X,
six from X to Y, and 3 from Y to b, i.e 1/3 + 1/6 + 1/3 ohms.

Charles.

Yes of course, just stick wires between the equal V points! I had
gotten to the point of seeing that there were two groups of three equal
voltage points before doing any math, but just didn't make the next
mental leap before bailing out to what I'm comfortable with: writing
equations.

I realize it is sometimes a disadvantage to brute force stuff, cause you
can miss the elegant solutions.

Part of the price to pay of trying to do too many things reasonably
well, instead of mastering one thing, I suppose.

I'd like to redraw and solve the resistor cube just for fun with some
additional diagonal resistors connected from the corners, and passing
through the interior of the cube.

How about a 4 dimensional resistor cube!?!?

Ok, back to work...

Good day!



--
____________________________________
Christopher R. Carlen
Principal Laser/Optical Technologist
Sandia National Laboratories CA USA
crcarle@sandia.gov
 
In article <c8ta9v0183o@news4.newsguy.com>,
Chris Carlen <crcarle@BOGUS.sandia.gov> wrote:
I had to resort to pencil and paper and came up with the following
matrix solution for the node voltages for attaching a 1V source to
terminal A and ground to terminal B:
Change it to a 1 amp current source and think about it that way.

Mark Zenier mzenier@eskimo.com Washington State resident
 
Chris Carlen <crcarle@BOGUS.sandia.gov> writes:

Hi:

Guy Macon wrote:

"Here is a classic that really shows the difference between algebraic
and RPN: calculate the resistance between points (a) and (b) using
only a calculator - no drawings or equations on paper.


(a)-- *----------- ONE OHM -------------* V1
|\ |\
| O O O
| N N N
| E E E
| |
| O O O
O H H H
N M M M
E \ V2 | \
*---- ONE OHM --------------------* V6
O | | |
H O | O
M N | N
| W | E
| | | |
| O | |
| H | O
| M | N
| V3 | | E
*----- ONE OHM -------------------* V4
\ | \ O
O | O H
N | N M
E | E |
| |
O | O |
H | H |
M | M |
\| V5 \|
*------------ ONE OHM ------------*--(b)"


I found this intriguing because it seemed silly that I could spend all
weekend studying Fourier transforms and "advanced" stuff like that,
and then be put off by a simple resistor problem. So I gave it a
try...

You know that the cube is symmetrical, and the two points a and b are
at opposite corners. So there is no "preferred" route from a to b. The
currents from a to V1, V2 and V3 will be equal by symmetry. Therefore
the voltage drop will be equal too. So the voltages V1,2,3 are
equal. There is therefore no difference between this circuit and one
with V1,2,3 connected together. In which case the 3 resistors
connected to a are in parallel and the resistance is 1/3 ohm.

You can make the identical argument from the "b" end, so another 1/3
ohm appears.

Finally we now have the remaining 6 resistors V3-5, V2-5, V1-4, V1-6,
V2-5, V2-6. But these are all in parallel too since we connected
V1,2,3 and V4,5,6. So we have a final 1/6 of an ohm giving a total of
1/3+1/3+1/6 = 5/6.


--
John Devereux
 
Chris Carlen <crcarle@BOGUS.sandia.gov> says...

So while a keen eye might come up with an elegant solution,
sometimes the brute force method delivers a result long
before that spark of insight hits, usually in the shower
at the end of the day (or week).
The fist time I saw this I looked at it for roughly one minute,
came up with a much simpler way to solve it and did the math in
my head. It turns out that that's the point of the problem - to
see if you can find the (obvious to me) simplification.


--
Guy Macon, Electronics Engineer & Project Manager for hire.
Remember Doc Brown from the _Back to the Future_ movies? Do you
have an "impossible" engineering project that only someone like
Doc Brown can solve? My resume is at http://www.guymacon.com/
 
"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...
Fun problem. Wasn't what I had originally planned for my first hour of
the day.
Your next assignment is the dodecahedron ;)

--
Thanks, Frank.
(remove 'x' and 'invalid' when replying by email)
 
Guy Macon wrote:
Chris Carlen <crcarle@BOGUS.sandia.gov> says...


So while a keen eye might come up with an elegant solution,
sometimes the brute force method delivers a result long
before that spark of insight hits, usually in the shower
at the end of the day (or week).


The fist time I saw this I looked at it for roughly one minute,
came up with a much simpler way to solve it and did the math in
my head. It turns out that that's the point of the problem - to
see if you can find the (obvious to me) simplification.


Yes indeed.


--
____________________________________
Christopher R. Carlen
Principal Laser/Optical Technologist
Sandia National Laboratories CA USA
crcarle@sandia.gov
 
Frank Bemelman wrote:
"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...

Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)

If you can draw it, I'll solve it.



--
____________________________________
Christopher R. Carlen
Principal Laser/Optical Technologist
Sandia National Laboratories CA USA
crcarle@sandia.gov
 
Chris Carlen says...
Frank Bemelman wrote:

"Chris Carlen" schreef...

Fun problem. Wasn't what I had originally planned for
my first hour of the day.

Your next assignment is the dodecahedron ;)

If you can draw it, I'll solve it.
I would like to see someone draw a ASCII resistor dodecahedron
that's anywhere near as clear as my ASCII resistor cube was...

I don't think I can manage it.


--
Guy Macon, Electronics Engineer & Project Manager for hire.
Remember Doc Brown from the _Back to the Future_ movies? Do you
have an "impossible" engineering project that only someone like
Doc Brown can solve? My resume is at http://www.guymacon.com/
 
On Mon, 24 May 2004 15:22:14 -0700, Chris Carlen
<crcarle@BOGUS.sandia.gov> wrote:

Frank Bemelman wrote:
"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...

Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)


If you can draw it, I'll solve it.
Consider the infinite plane grid of 1 ohm resistors with nodes on
the coordinates with integer values, such as (1,1), (2,2), (1,2) etc.
None of the resistors is diagonally connected, as between (1,1) and
(2,2). All the horizontally adjacent and vertically adjacent nodes
have a 1 ohm resistor connected.

What is the resistance between the points (1,1) and (1,2)?

What is the resistance between the points (1,1) and (1,2)?
 
"The Phantom" <phantom@aol.com> wrote in message
news:ra35b09jojkea7158uuduie1l4r1eltgsm@4ax.com...
| On Mon, 24 May 2004 15:22:14 -0700, Chris Carlen
| <crcarle@BOGUS.sandia.gov> wrote:
|
| >Frank Bemelman wrote:
| >> "Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
| >> news:c8ta9v0183o@news4.newsguy.com...
| >>
| >>>Fun problem. Wasn't what I had originally planned for my first
hour of
| >>>the day.
| >>
| >>
| >> Your next assignment is the dodecahedron ;)
| >
| >
| >If you can draw it, I'll solve it.
|
| Consider the infinite plane grid of 1 ohm resistors with nodes on
| the coordinates with integer values, such as (1,1), (2,2), (1,2) etc.
| None of the resistors is diagonally connected, as between (1,1) and
| (2,2). All the horizontally adjacent and vertically adjacent nodes
| have a 1 ohm resistor connected.
|
| What is the resistance between the points (1,1) and (1,2)?
|
| What is the resistance between the points (1,1) and (1,2)?

The same as the resistance between points (1,1) and (1,2)

Do I get a sweety darling?

DNA
 
The Phantom wrote:
On Mon, 24 May 2004 15:22:14 -0700, Chris Carlen
crcarle@BOGUS.sandia.gov> wrote:


Frank Bemelman wrote:

"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...


Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)


If you can draw it, I'll solve it.


Consider the infinite plane grid of 1 ohm resistors with nodes on
the coordinates with integer values, such as (1,1), (2,2), (1,2) etc.
None of the resistors is diagonally connected, as between (1,1) and
(2,2). All the horizontally adjacent and vertically adjacent nodes
have a 1 ohm resistor connected.

What is the resistance between the points (1,1) and (1,2)?
Yes, this is another category of interesting resistor problems. Don't
give me any hints. Though I am not sure when I will try it. It has
been in the back of my mind since seeing it here a few times.

What is the resistance between the points (1,1) and (1,2)?
Don't you mean some other points?


Good day!



--
_____________________
Christopher R. Carlen
crobc@earthlink.net
Suse 8.1 Linux 2.4.19
 
"Chris Carlen" <crcarle@BOGUS.sandia.gov> wrote in message
news:c8tsim13152@news3.newsguy.com...
Frank Bemelman wrote:
"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...

Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)


If you can draw it, I'll solve it.
/------------------- 1 ohm ------------------------------\
/ \
K-- 1 ohm --L-------- 1 ohm --------O-- 1 ohm --Q-- 1 ohm --S
| | | | |
| | | | |
| 1 ohm 1 ohm | |
| | | | |
| | | | |
1 ohm C-- 1 ohm --E-- 1 ohm --G 1 ohm |
| | | | | |
| | | | | |
| 1 ohm | 1 ohm | |
| | | | | |
| | | | | |
A-- 1 ohm --B 1 ohm I-- 1 ohm --J 1 ohm
| | | | | |
| | | | | |
| 1 ohm | 1 ohm | |
| | | | | |
| | | | | |
1 ohm D-- 1 ohm --F-- 1 ohm --H 1 ohm |
| | | | |
| | | | |
| 1 ohm 1 ohm | |
| | | | |
| | | | |
M-- 1 ohm --N-------- 1 ohm --------P-- 1 ohm --R-- 1 ohm --T
\ /
\------------------- 1 ohm ------------------------------/


One pair of "opposite corners" is A and I.
 
On 24 May 2004 20:11:54 +0100, John Devereux <jd1@devereux.me.uk> wrote:

(snip O/P stuff re 1R cube)

You know that the cube is symmetrical, and the two points a and b are
at opposite corners. So there is no "preferred" route from a to b. The
currents from a to V1, V2 and V3 will be equal by symmetry. Therefore
the voltage drop will be equal too. So the voltages V1,2,3 are
equal. There is therefore no difference between this circuit and one
with V1,2,3 connected together. In which case the 3 resistors
connected to a are in parallel and the resistance is 1/3 ohm.

You can make the identical argument from the "b" end, so another 1/3
ohm appears.

Finally we now have the remaining 6 resistors V3-5, V2-5, V1-4, V1-6,
V2-5, V2-6. But these are all in parallel too since we connected
V1,2,3 and V4,5,6. So we have a final 1/6 of an ohm giving a total of
1/3+1/3+1/6 = 5/6.
John and Mark have put their respective fingers on the elegant solution
approach. Symmetry is the key, and using a current source helps visualise the
volt drop across each thrid of the mesh.

BTW, we had this as a problem in high school physics. Several of us gave the
answer "by eye", without resort to pencil/paper. And the slide rule probably
wouldn't have helped ....
 
The Phantom <phantom@aol.com> says...

Consider the infinite plane grid of 1 ohm resistors with nodes on
the coordinates with integer values, such as (1,1), (2,2), (1,2) etc.
None of the resistors is diagonally connected, as between (1,1) and
(2,2). All the horizontally adjacent and vertically adjacent nodes
have a 1 ohm resistor connected.

What is the resistance between the points (1,1) and (1,2)?

What is the resistance between the points (1,1) and (1,2)?
You mean (2,2) don't you?


The answers are in the rec.puzzles archive.

Don't read any farther unless you want to know the answers

References:
http://rec-puzzles.org/
http://rec-puzzles.org/physics.html
http://rec-puzzles.org/sol.pl/physics/resistors

resistors
What is the resistance between various pairs of vertices on a
lattice of unit resistors in the shape of a

1. Cube,

2. Platonic solid,

3. N dimensional Hypercube,

4. Infinite square lattice, and

5. between two small terminals on a continuous sheet?

------------------------------------------------------------------------------

Solution to the /physics/resistors problem

Cube
The key idea is to observe that if you can show that two points in a circuit
must be at the same potential, then you can connect them, and no current will
flow through the connection and the overall properties of the circuit remain
unchanged. In particular, for the cube, there are three resistors leaving the
two "connection corners". Since the cube is completely symmetrical with respect
to the three resistors, the far sides of the resistors may be connected
together. And so we end up with:
|---WWWWWW---| |---WWWWWW---| |---WWWWWW---|
| | |---WWWWWW---| | |
*--+---WWWWWW---+-+---WWWWWW---+-+---WWWWWW---+---*
| | |---WWWWWW---| | |
|---WWWWWW---| |---WWWWWW---| |---WWWWWW---|
|---WWWWWW---|

This circuit has resistance 5/6 times the resistance of one resistor.
Platonic Solids
Same idea for 8, 12 and 20, since you use the symmetry to identify
equi-potential points. The tetrahedron is a hair more subtle:
*---|---WWWWWW---|---*
|\ /|
W W W W
W W W W
W W W W
| \ / |
\ || |
\ | /
\ W /
\ W / <-------
\ W /
\|/
+

By symmetry, the endpoints of the marked resistor are equi-potential. Hence
they can be connected together, and so it becomes a simple:
*---+---WWWWW---+----*
| |
+-WWW WWW-+
| |-| |
|-WWW WWW-|

Hypercube
Think of injecting a constant current I into the start vertex. It splits (by
symmetry) into n equal currents in the n arms; the current of I/n then splits
into I/n(n-1), which then splits into I/[n(n-1)(n-1)] and so on till the
halfway point, when these currents start adding up. What is the voltage
difference between the antipodal points? V = I x R; add up the voltages along
any of the paths: n even:
(n-2)/2
V = 2{I/n + I/(n(n-1)) + I/(n(n-1)(n-1)) + ... + I/(n(n-1) )}


n odd:
(n-3)/2
V = 2{I/n + I/(n(n-1)) + I/(n(n-1)(n-1)) + ... + I/(n(n-1) )} (n-1)/2
+ I/(n(n-1)
)

And R = V/I i.e. replace the Is in the above expression by 1s.
For the 3-cube: R = 2{1/3} + 1/(3x2) = 5/6 ohm
For the 4-cube: R = 2{1/4 + 1/(4x3)} = 2/3 ohm

This formula yields the resistance from root to root of two (n-1)-ary trees of
height n/2 with their end nodes identified (-when n is even; something similar
when n is odd). Coincidentally, the 4-cube is such an animal and thus the
answer 2/3 ohms is correct in that case. However, it does not provide the
solution for n >= 5, as the hypercube does not have quite as many edges as were
counted in the formula above.

The Infinite Plane
For an infinite lattice: First inject a constant current I at a point; figure
out the current flows (with heavy use of symmetry). Remove that current. Draw
out a current I from the other point of interest (or inject a negative current)
and figure out the flows (identical to earlier case, but displaced and in the
other direction). By the principle of superposition, if you inject a current I
into point a and take out a current I at point b at the same time, the currents
in the paths are simply the sum of the currents obtained in the earlier two
simpler cases. As in the n-cube, find the voltage between the points of
interest, divide by I and voila`!
As an illustration, in the adjacent points case: we have a current of I/4 in
each of the four resistors:

^ |
| v
<--o--> -->o<--
| ^
v |
(inject) (take out)

And adding the currents, we have I/2 in the resistor connecting the two points.
Therefore V=(1 ohm) x I/2 and effective resistance between the points = 1/2
ohm.
We do not derive it, but the equivalent resistance between two nodes k diagonal
units apart is (2/pi)(1+1/3+1/5+...+1/(2k-1)); that, plus symmetry and the
known equivalent resistance between two adjacent nodes, is sufficient to derive
all equivalent resistances in the lattice.

Continuous sheet
I think the answer is (rho/dz)log(L/r)/pi where rho is the resistivity, dz is
the sheet thickness, L is the separation, r is the terminal radius.
cf. "Random Walks and Electric Networks", by Doyle and Snell, published by the
Mathematical Association of America.


--
Guy Macon, Electronics Engineer & Project Manager for hire.
Remember Doc Brown from the _Back to the Future_ movies? Do you
have an "impossible" engineering project that only someone like
Doc Brown can solve? My resume is at http://www.guymacon.com/
 
On Mon, 24 May 2004 17:15:07 -0700, Chris Carlen
<crobc@BOGUS_FIELD.earthlink.net> wrote:

The Phantom wrote:
On Mon, 24 May 2004 15:22:14 -0700, Chris Carlen
crcarle@BOGUS.sandia.gov> wrote:


Frank Bemelman wrote:

"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...


Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)


If you can draw it, I'll solve it.


Consider the infinite plane grid of 1 ohm resistors with nodes on
the coordinates with integer values, such as (1,1), (2,2), (1,2) etc.
None of the resistors is diagonally connected, as between (1,1) and
(2,2). All the horizontally adjacent and vertically adjacent nodes
have a 1 ohm resistor connected.

What is the resistance between the points (1,1) and (1,2)?

Yes, this is another category of interesting resistor problems. Don't
give me any hints. Though I am not sure when I will try it. It has
been in the back of my mind since seeing it here a few times.

What is the resistance between the points (1,1) and (1,2)?
Yes, of course; typos happen, eh?

What is the resistance between the points (1,1) and (2,2)?

Don't you mean some other points?


Good day!
 
On Mon, 24 May 2004 17:57:01 -0700, Richard Henry wrote:

"Chris Carlen" <crcarle@BOGUS.sandia.gov> wrote in message
news:c8tsim13152@news3.newsguy.com...
Frank Bemelman wrote:
"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...

Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)


If you can draw it, I'll solve it.



/------------------- 1 ohm ------------------------------\
/ \
K-- 1 ohm --L-------- 1 ohm --------O-- 1 ohm --Q-- 1 ohm --S
| | | | |
| | | | |
| 1 ohm 1 ohm | |
| | | | |
| | | | |
1 ohm C-- 1 ohm --E-- 1 ohm --G 1 ohm |
| | | | | |
| | | | | |
| 1 ohm | 1 ohm | |
| | | | | |
| | | | | |
A-- 1 ohm --B 1 ohm I-- 1 ohm --J 1 ohm
| | | | | |
| | | | | |
| 1 ohm | 1 ohm | |
| | | | | |
| | | | | |
1 ohm D-- 1 ohm --F-- 1 ohm --H 1 ohm |
| | | | |
| | | | |
| 1 ohm 1 ohm | |
| | | | |
| | | | |
M-- 1 ohm --N-------- 1 ohm --------P-- 1 ohm --R-- 1 ohm --T
\ /
\------------------- 1 ohm ------------------------------/

One pair of "opposite corners" is A and I.
Is that *really* a dodecahedron flattened out? Where's Bucky when I
need him?
--
Best Regards,
Mike
 
The Phantom wrote:
On Mon, 24 May 2004 17:15:07 -0700, Chris Carlen
crobc@BOGUS_FIELD.earthlink.net> wrote:

The Phantom wrote:
On Mon, 24 May 2004 15:22:14 -0700, Chris Carlen
crcarle@BOGUS.sandia.gov> wrote:


Frank Bemelman wrote:

"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...


Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)


If you can draw it, I'll solve it.


Consider the infinite plane grid of 1 ohm resistors with nodes on
the coordinates with integer values, such as (1,1), (2,2), (1,2) etc.
None of the resistors is diagonally connected, as between (1,1) and
(2,2). All the horizontally adjacent and vertically adjacent nodes
have a 1 ohm resistor connected.

What is the resistance between the points (1,1) and (1,2)?

Yes, this is another category of interesting resistor problems. Don't
give me any hints. Though I am not sure when I will try it. It has
been in the back of my mind since seeing it here a few times.

What is the resistance between the points (1,1) and (1,2)?

Yes, of course; typos happen, eh?

What is the resistance between the points (1,1) and (2,2)?


Don't you mean some other points?


Good day!
The cube of 1 ohm resistors, a resistor on each edge, whit the
question as to the value of resistance across the internal body diagnal
can be made more interesting:
State at least three completely differnt ways of solving this problem
and give the electrical and/or mathematical reasons for each step if the
solutions.
For extra credit, state how many different ways there are to solve
that problem - with a brief description of each method (so we know you
are not cheating).
 
The Phantom wrote:
On Mon, 24 May 2004 17:15:07 -0700, Chris Carlen
crobc@BOGUS_FIELD.earthlink.net> wrote:

The Phantom wrote:
On Mon, 24 May 2004 15:22:14 -0700, Chris Carlen
crcarle@BOGUS.sandia.gov> wrote:


Frank Bemelman wrote:

"Chris Carlen" <crcarle@BOGUS.sandia.gov> schreef in bericht
news:c8ta9v0183o@news4.newsguy.com...


Fun problem. Wasn't what I had originally planned for my first hour of
the day.


Your next assignment is the dodecahedron ;)


If you can draw it, I'll solve it.


Consider the infinite plane grid of 1 ohm resistors with nodes on
the coordinates with integer values, such as (1,1), (2,2), (1,2) etc.
None of the resistors is diagonally connected, as between (1,1) and
(2,2). All the horizontally adjacent and vertically adjacent nodes
have a 1 ohm resistor connected.

What is the resistance between the points (1,1) and (1,2)?

Yes, this is another category of interesting resistor problems. Don't
give me any hints. Though I am not sure when I will try it. It has
been in the back of my mind since seeing it here a few times.

What is the resistance between the points (1,1) and (1,2)?

Yes, of course; typos happen, eh?

What is the resistance between the points (1,1) and (2,2)?


Don't you mean some other points?


Good day!
There are a number of ways the "cube" problem can be solved, and one
of the simplist methods takes a few seconds from the first view of the
problem to the correct method, then one or two seconds more to an
*exact* solution, as compared to the calculator method (approximate)
first given.
 

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