Transcript PPT - LSU Physics & Astronomy

b
Physics 2102
a
Jonathan Dowling
Physics 2102
Lecture 11
DC Circuits
Incandescent light bulbs
(a)
(b)
(c)
(d)
(e)
(f)
Which light bulb has a smaller resistance: a 60W, or a 100W one?
Is the resistance of a light bulb different when it is on and off?
Which light bulb has a larger current through its filament: a 60W one, or a
100 W one?
Would a light bulb be any brighter if used in Europe, using 240 V outlets?
Would a US light bulb used in Europe last more or less time?
Why do light bulbs mostly burn out when switched on?
EMF devices and single loop circuits
b
The battery operates as a “pump” that moves
positive charges from lower to higher electric
potential. A battery is an example of an
“electromotive force” (EMF) device.
a
These come in various kinds, and all transform one source of energy into electrical
energy. A battery uses chemical energy, a generator mechanical energy, a solar cell
energy from light, etc.
i
- +
d
b c
The difference in potential energy that the
a
device establishes is called the EMF
i
and denoted by E.
E
= iR
iR
E
Va
a
b
c
d=a
Circuit problems
Given the emf devices and resistors in a circuit,
we want to calculate the circulating currents.
Circuit solving consists in “taking a walk” along
the wires. As one “walks” through the circuit (in
any direction) one needs to follow two rules:
When walking through an EMF, add +E if you flow with the current or -E
otherwise. How to remember: current “gains” potential in a battery.
When walking through a resistor, add -iR, if flowing with the current or +iR
otherwise. How to remember: resistors are passive, current flows “potential down”.
Example:
Walking clockwise from a: + E-iR=0.
Walking counter-clockwise from a: - E+iR=0.
Ideal batteries vs. real batteries
If one connects resistors of lower and lower value of R to get higher and higher
currents, eventually a real battery fails to establish the potential difference E, and
settles for a lower value.
One can represent a “real EMF device” as an ideal one attached to a resistor,
called “internal resistance” of the EMF device:
E –i r - i R=0  i=E/(r+R)
Etrue = E –i r
The true EMF is a function of current: the more
current we want, the smaller Etrue we get.
Resistors in series and parallel
An electrical cable consists of 100 strands of fine wire, each having 2 W resistance. The same potential
difference is applied between the ends of all the strands and results in a total current of 5 A.
(a)
(b)
(c)
What is the current in each strand?
Ans: 0.05 A
What is the applied potential difference?
Ans: 0.1 V
What is the resistance of the cable?
Ans: 0.02 W
Assume now that the same 2 W strands in the cable are tied in series, one after the other, and the 100
times longer cable connected to the same 0.1 Volts potential difference as before.
(d)
What is the potential difference through each strand?
Ans: 0.001 V
(e)
What is the current in each strand?
Ans: 0.0005 A
…
(f)
What is the resistance of the cable?
Ans: 200 W
(g)
Which cable gets hotter, the one with strands in parallel or the one with strands in series?
Ans: each strand in parallel dissipates 5mW (and the cable dissipates 500 mW);
each strand in series dissipates 50 mW (and the cable dissipates 5mW)
DC circuits: resistances in series
Two resistors are “in series” if they are connected such that the
same current flows in both.
The “equivalent resistance” is a single imaginary resistor that can
replace the resistances in series.
In the circuit with the
equivalent resistance,
“Walking the loop” results in :
E –iReq=0  i=E/Req
E –iR1-iR2-iR3=0  i=E/(R1+R2+R3)
Thus,
n
Req =  R j
j =1
Multiloop circuits: resistors in parallel
Two resistors are “in parallel” if they are
connected such that there is the same
potential drop through both.
The “equivalent resistance” is a single
imaginary resistor that can replace the
resistances in parallel.
“Walking the loops” results in :
E –i1R1=0, E –i2R2=0, E –i3R3=0
The total current delivered by the battery
is i = i1+i2+i3 = E/R1+ E/R2+ E/R3.
In the circuit with the equivalent resistor,
i=E/Req. Thus,
n
1
1
=
Req j =1 R j
Resistors and Capacitors
Resistors
Key formula: V=iR
Capacitors
Q=CV
In series: same current
Req=∑Rj
same charge
1/Ceq= ∑1/Cj
In parallel: same voltage
1/Req= ∑1/Rj
same voltage
Ceq=∑Cj
Example
Bottom loop: (all else is irrelevant)
12V
8W
i=
V 12V
=
= 1.5 A
R 8W
Which resistor gets hotter?
Example
a) Which circuit has the
largest equivalent
resistance?
b) Assuming that all
resistors are the
same, which one
dissipates more
power?
c) Which resistor has
the smallest potential
difference across it?
Example
Find the equivalent resistance between points
(a) F and H and
(b) F and G.
(Hint: For each pair of points, imagine that a battery
is connected across the pair.)
Monster Mazes
If all resistors have a
resistance of 4W, and all
batteries are ideal and
have an emf of 4V, what
is the current through
R?
If all capacitors have a
capacitance of 6mF, and
all batteries are ideal
and have an emf of 10V,
what is the charge on
capacitor C?