DC circuits
Physics 122
10/16/13
Lecture X
1
Skills
• Solve problems on parallel and series
connections in DC circuits
• RC circuits
10/16/13
Lecture X
2
1
Symbols
• Circuits can be
rearranged:
– Wires with negligible
resistance can be
– Stretched
– Bended
– Collapsed to a point
10/16/13
Lecture X
3
Electric battery
•
•
•
•
For idealized battery emf – supplied voltage
Real life batteries have internal resistance r
Terminal voltage (supplied to the circuit)
Vab=emf-Ir
10/16/13
Lecture X
4
2
Skiing ßà electric circuit
a
i li
ft
b
Batt
ery
Sk
c
Cannot stop at b, must get to c –
ski lift:
V=V1+V2 - Net voltage drop in a
circuit is always equal to the
supplied voltage (e.g. battery)
10/16/13
Lecture X
5
Series connection
10/16/13
• Charge conservation:
– I=I1=I2=I3
• Ohm’s law
– V1=IR1; V2=IR2; V3=IR3
• Energy conservation:
– qV=qV1+qV2+qV3
– V=V1+V2+V3
• IReq=IR1+IR2+IR3
• Req=R1+R2+R3
Lecture X
6
3
Parallel connection
1
1 1
1
= + +
Req R1 R2 R3
• Charge conservation: I=I1+I2+I3
• Energy conservation: V=V1=V2=V3
• Ohm’s law: I1=V/R1; I2=V/R2; I3=V/R3
V
V V V
= + +
Req R1 R2 R3
10/16/13
Lecture X
7
Capacitor connections
No DC current
through capacitor,
Just store charge.
• Parallel connection:
•
• Same voltage – V1=V2=V3=V •
• Different charges:
•
– Q1=C1V Q2=C2V
Q3=C3V
– Q=Q1+Q2+Q3=V(C1+C2+C3)
Series connection:
Same charge (QA=0 à -Q1+Q2=0)
Different voltages V=V1+V2+V3
Q
Q Q Q
= +
+
Ceq C1 C2 C3
– Ceq=C1+C2+C3
10/16/13
Lecture X
1
1
1
1
= +
+
Ceq C1 C2 C3
8
4
RC circuit
• RC circuit contains at least one capacitor (C ) and at
least one resistor (R ).
I=
dQ
dt
VR = IR
VC = Q / C
VR + VC = Vbattery = const
+Q
dQ Q
R
+ =V
dt C
RCQ '+Q = CV
C
-Q
Q = CV (1 − e −t /τ )
τ = RC
10/16/13
Lecture X
9
DC circuits
•
•
•
•
Series connection
I=I1=I2=I3
V=V1+V2+V3
Req=R1+R2+R3
10/16/13
•
•
•
•
Parallel connection
I=I1+I2+I3
V=V1=V2=V3
1
1 1
1
= + +
Req R1 R2 R3
Lecture X
10
5
Series vs parallel - Req
• R1=R2=R3=R
• Req=3R
• R1=R2=R3=R
• Req=R/3
>
Equivalent resistance is larger in series connection.
10/16/13
Lecture X
11
Series vs parallel - I
•
•
•
•
R1=R2=R3=R
Req=3R
I=V/(3R)
I1=I2=I3=I=V/(3R)
<
<
•
•
•
•
R1=R2=R3=R
Req=R/3
I=3V/R
I1=I2=I3=I/3=V/R
Total current and individual currents are smaller in series connection.
10/16/13
Lecture X
12
6
Series vs parallel - P
P1=I2R
Pnet=IV
Brightness
proportional
to power
•
•
•
•
R1=R2=R3=R
Req=3R
I=V/3R à Pnet=V2/3R
I1=V/3Rà P1=V2/9R
<
<
•
•
•
•
R1=R2=R3=R
Req=R/3
I=3V/R à Pnet=3V2/R
I1=V/R à P1=V2/R
Total and individual power consumptions are smaller in series connection.
Light bulbs are brighter in parallel connection.
10/16/13
Lecture X
13
Safety and grounding
• Usually V is fixed
• To reduce I – increase R
• Dry surface
– 1mA – “feel”
• Insulating sole
– 10mA – muscle contraction
• Insulating floor
– 70 mA – “ventricular fibrillation”
– ~1A – hearts stops (not as harmful)• To avoid high V • Ground the case
– >10A – “fry”
(3prong plug) 14
10/16/13
Lecture X
• Voltage does not kill.
• Current kills
7
Kirchhoff’s rules
• Junction rule (charge conservation):
– At any junction point the sum of all current entering the
junction must equal the sum of all currents leaving the
junction
• Do not disregard signs!
• Assign initial signs based on your best guess – if you were wrong the
currents will turn to be negative (opposite to initial guess)
• Loop rule (energy conservation):
– The sum of the changes in potential around any closed path of
a circuit must be zero.
•
•
•
•
•
Choose a direction in which you circle the loop (random)
For resistor Vab=-IR – negative if current along the loop direction
For resistor Vab=+IR – positive if current opposite the loop direction
For battery Vab – positive if the direction is from – to +
For battery Vab –negative if the direction is from + to -
10/16/13
Lecture X
15
Series vs parallel - Req
• R1=Rà2R
• Req=3Rà4R
R2=R3=R
• R1=Rà2R
R2=R3=R
• Req=R/3=2R/6à2R/5
If any of R’s increased the equivalent resistance will increase
in both parallel and series connection.
10/16/13
Lecture X
16
8
Series vs parallel - I
•
•
•
•
R1=Rà2R
R2=R3=R
Req=3Rà4R
I=V/Req=V/3RàV/4R
I1=I2=I3=I
10/16/13
•
•
•
•
•
R1=Rà2R
R2=R3=R
Req=R/3=2R/6à2R/5
I=V/Req=6V/2Rà5V/2R
I1=V/R1=V/RàV/2R
I2=I3=V/R – the same
Lecture X
17
Test problem
• For resistors connected in series, which of the
following will be the same for each of the
resistors?
• A
The current through.
• B
The potential difference across.
• C
The resistance of.
• D
The power dissipated by.
10/16/13
Lecture X
18
9
Test problem
• For resistors connected in parallel, which of the
following will be the same for each of the
resistors?
• A
The current through.
• B
The potential difference across.
• C
The resistance of.
• D
The power dissipated by.
10/16/13
Lecture X
19
10