Transcript Lecture 4

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What was
the plan?
What did
I do?
What
were my
results?
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Clear
figures
Clear
tables
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What
does it
mean?
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Wrap it
up.
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EMF and Terminal Voltage (Ch 26)
An Electric circuit needs a battery or generator to
produce current – these are called sources of emf.
(electromotive force, ε)
A battery is a nearly constant voltage source, but
does have a small internal resistance, which
reduces the actual voltage from the ideal emf:
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EMF and Terminal Voltage
This resistance behaves as though it were in
series with the emf.
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EMF and Terminal Voltage
Example : Battery with internal resistance.
A 65.0-Ω resistor is
connected to the
terminals of a battery
whose emf is 12.0 V and
whose internal
resistance is 0.5 Ω.
Calculate
(a)the current in the circuit,
(b) the terminal voltage of the battery, Vab, and
(c) the power dissipated in the resistor R and in
the battery’s internal resistance r.
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Resistors in Series and in Parallel
A series connection has a single path from
the battery, through each circuit element in
turn, then back to the battery.
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Resistors in Series and in Parallel
The current through each resistor is the
same; the voltage depends on the
resistance. The sum of the voltage
drops across the resistors equals the
battery voltage:
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Resistors in Series and in Parallel
From this we get the equivalent resistance (that
single resistance that gives the same current in
the circuit):
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Resistance Limits:
Open and Short Circuits
• Short Circuit: A wire! R=0, V=0 for any i.
– Particularly bad for any voltage source
• Open circuit: A break! R→, i=0 for any V.
– Particularly bad for current source
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Series Resistors and the Voltage Divider Rule
For N resistors in series:
Same current through each resistor – so voltage is split
according to their resistance
Voltage Divider:
R1
v1 
(1.5V)
REQ
R
v2  2 (1.5V)
REQ
v3 
R3
(1.5V)
REQ
R3
Resistors in Series and in Parallel
A parallel connection splits the current; the
voltage across each resistor is the same:
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Resistors in Series and in Parallel
The total current is the sum of the currents
across each resistor:
,
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Resistors in Series and in Parallel
This gives the reciprocal of the equivalent
resistance:
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Resistors in Series and in Parallel
An analogy using water
may be helpful in
visualizing parallel
circuits. The water
(current) splits into two
streams; each falls the
same height, and the total
current is the sum of the
two currents. With two
pipes open, the resistance
to water flow is half what
it is with one pipe open.
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Parallel Resistors and the Current Divider Rule
For N resistors in parallel:
Current is split according to the inverse of their resistance
(more current through a wider (lower resistance) pipe)
v REQ
iS
Current Divider: i1  
R1
R1
REQ
v
i2 

iS
R2
R2
v REQ
i3 

iS
R3
R3
Resistors in Series and in Parallel
Example: Series or parallel?
(a) The lightbulbs in the figure are identical.
Which configuration produces more light?
(b) Which way do you think the headlights of a
car are wired?
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Resistors in Series and in Parallel
Example: Circuit with series and parallel
resistors.
How much current is drawn from the
battery shown?
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