Download I I-i1 i1 i2 I-i2 i1

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Lumped element model wikipedia , lookup

CMOS wikipedia , lookup

Integrated circuit wikipedia , lookup

Mathematics of radio engineering wikipedia , lookup

Power electronics wikipedia , lookup

Test probe wikipedia , lookup

Wien bridge oscillator wikipedia , lookup

Switched-mode power supply wikipedia , lookup

Power MOSFET wikipedia , lookup

Index of electronics articles wikipedia , lookup

Valve RF amplifier wikipedia , lookup

Multimeter wikipedia , lookup

Schmitt trigger wikipedia , lookup

Regenerative circuit wikipedia , lookup

Charlieplexing wikipedia , lookup

Opto-isolator wikipedia , lookup

Surge protector wikipedia , lookup

Two-port network wikipedia , lookup

Operational amplifier wikipedia , lookup

TRIAC wikipedia , lookup

Resistive opto-isolator wikipedia , lookup

Electrical ballast wikipedia , lookup

Rectiverter wikipedia , lookup

Ohm's law wikipedia , lookup

RLC circuit wikipedia , lookup

Current mirror wikipedia , lookup

Current source wikipedia , lookup

Network analysis (electrical circuits) wikipedia , lookup

Transcript
Physics 7B, Lecture 001, Spring 2012 (Xiaosheng Huang)
Mid-term 2 – Problem 2 solution
Method 1:
Using Kirchoff’s current law, we can label the current flowing through each
resistor. i1 and i2 are unknown currents that have been introduced.
I-i1
R
A
I-i2
i1-i2
i1
R
R
R
B
R
i2
C
I
ε
Three loops have also been drawn in the above diagram. Using Kirchoff’s
voltage law, we know that the voltage drop around any loop must sum to 0.
Loop A:
R*i1 + R*(i1-i2) – R*(I-i1) = 0
 3i1 – i2 = I
Loop B:
R*(i1-i2) + R*(I-i2) – R*(i2) = 0
 I = 3i2 – i1
If we equate the “I” in both equations:
3i1 – i2 = 3i2 – i1
i1 = i2
Subbing them back into our “I” equations would tell us that
i1 = i2 = I/2
Loop C:
R*i1 + R*i2 – ε = 0
ε = R*( i1 + i2) = R*I
since
i1 = i2 = I/2
We also know that the EMF is equal to the total potential drop in the circuit
ε = V = Reff * I
Hence we immediately see that Reff = R
Method 2:
By redrawing the circuit, we can easily see that the circuit has a symmetry
we can exploit to solve the problem.
Va
I2
I1
R
I
R
I
I3
R
R
R
I4
I5
Vb
Now the clever trick is to flip the diagram upside-down.
Vb
I5
I4
R
I
R
I
I3
R
R
R
I1
I2
Va
But after the reflection, the assembly of these 5 resistors looks exactly the
same as before. Hence they are the same circuit.
We see that the direction of the current through the middle resistor (I3) is
flipped, so the only way to ensure that both circuit are equivalent is for I3=0
We could have also argued that by symmetry Va=Vb. There is no voltage
drop across the middle resistor hence no current flows through it.
Since there is no current through the middle resistor, its removal will not
affect our circuit.
R
R
R
R
The effective resistance can be found by summing the resistors in the above
diagram, which gives:
Reff = R
An aside:
Symmetry also tells us that I1=I4 and I2=I5. Together with Kirchoff’s junction
rule, we can quickly deduce that I1= I2= I4= I5=I/2 with minimal algebra.
The lesson is that symmetry is a powerful tool and should be exploited
whenever possible!