Ohm’s Law: V = IR Power dissipated (Joule heating) = P = I 2 R = IV.

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Ohm’s Law: V = IR Power dissipated (Joule heating) = P = I 2 R = IV
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Transcript of Ohm’s Law: V = IR Power dissipated (Joule heating) = P = I 2 R = IV.

Ohm’s Law: V = IR

Power dissipated (Joule heating) =

P = I2R = IV

Kirchoff’s Loop equation:

Kirchoff’s junction rule:

Resistors in series: Req = R1 + R2 + …

Resistors in parallel: Req-1 = R1

-1 + R2-1 +…

Capacitors in series: Ceq-1 = C1

-1 + C2-1 + …

Capacitors in parallel: Ceq = C1 + C2 + …

0iclosed loop

V

/0ientering leaving junction

I

Group Problems1. R combo – all 100

a) Find I from the battery

b) Find I through each R

2. a) Find equivalent R (in terms of R)

b) Find the battery

current if R = 100

R4

R2R1

R5

R325V

R

R

10V

R

R

Simple RC Series circuit

• Discharging: Q(t) = Qoexp(-t/RC)

and I(t) = Ioexp(-t/RC)

0

0.2

0.4

0.6

0.8

1

0 10 20 30 40 50 60

time (ms)

No

rmal

ize

d Q

or

I

When t = RC = 1 time constant, then Q = Qoexp(-1) = 0.37Qo

Microscopic Picture of Electric Current

• E field in wire produces forces on free electrons leading to a net drift velocity: vdrift = a, where a is

the acceleration (a = F/m = eE/m = e(V/L)/m where V is the applied voltage across the wire of length L) and is the mean-

free time between collisions • Solving for the charge drifting by allows us to

compute the current I: I=[(ne2/m)(A/L)]V = [1/R]V = GV, where n is the free charge density, e is the electron charge, A is the wire cross-sectional area, R is the wire’s resistance and G is its conductance

• We can also introduce intrinsic parameters: conductivity, = ne2/m and resistivity, = 1/ to write R = L/A

IC INa IK IL

outside

inside

C

VNa VK VL

GNa GK GL

Cell body

axon

Myelin sheath

dendrites

Terminal endings

retinal “starburst” cell (red) found in visual processing network, Courtesy of Thomas Euler, Max Planck Institute for Medical Research, Heidelberg

I (pA)

Time (ms)

0

1

Time (ms)

I (pA)

V (mV)