Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current...
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Transcript of Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current...
![Page 1: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/1.jpg)
Lecture 7 Circuits Ch. 27
• Cartoon -Kirchhoff's Laws• Warm-up problems• Topics
– Direct Current Circuits– Kirchhoff's Two Rules– Analysis of Circuits Examples– Ammeter and voltmeter– RC circuits
• Demos– Three bulbs in a circuit
– Power loss in transmission lines– Resistivity of a pencil– Blowing a fuse
![Page 2: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/2.jpg)
Transmission line demo
![Page 3: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/3.jpg)
Direct Current Circuits
1. The sum of the potential drops around a closed loop is zero. This follows from energy conservation and the fact that the electric field is a conservative force.
2. The sum of currents into any junction of a closed circuit must equal the sum of currents out of the junction. This follows from charge conservation.
![Page 4: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/4.jpg)
Example (Single Loop Circuit)
No junction so we don’t need that rule.
How do we apply Kirchoff’s rule?
Must assume the direction of the current – assume clockwise.
Choose a starting point and apply Ohm’s Law as you go around the circuit.
a. Potential across resistors is negative
b. Sign of E for a battery depends on assumed current flow
c. If you guessed wrong on the sign, your answer will be negative
Start in the upper left hand corner.
21321
21
1132221 0
rrRRR
EEi
irEiRirEiRiR
++++−
=
=−+−−−−−
![Page 5: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/5.jpg)
21321
21
rrRRR
EEi
++++−
=
Now let us put in numbers.
VE
VE
rr
RRR
5
10
1
10
2
1
21
321
==
Ω==Ω===Suppose:
325
11101010510 =
Ω++++−= Vi amp
VE
VE
10
5
2
1
==Suppose:
325
32)105( −=
Ω−= Vi amp
We get a minus sign. It means our assumed direction of current must be reversed.
Note that we could have simply added all resistors and get the Req. and added the EMFs to get the Eeq. And simply divided.
32
5
)(32
)(5
R .e
.=
Ω==
VEi
q
eqamp
Sign of EMF
Battery 1 current flows from - to + in battery +E1
Battery 2 current flows from + to - in battery -E2
In 1 the electrical potential energy increases
In 2 the electrical potential energy decreases
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Example with numbers
Quick solution:
AE
I
R
VVVVE
q
eq
i
i
i
i
16
10
R
16
102412
.e
.
6
1
3
1
==
Ω=
=+−=
∑
∑
=
=
Question: What is the current in the circuit?
AampsVi
iV
625.0625.01610
0)311551()2412(
==Ω
=
=Ω+++++−+−+
Write down Kirchoff’s loop equation.
Loop equation
Assume current flow is clockwise.
Do the batteries first – Then the current.
![Page 7: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/7.jpg)
Example with numbers (continued)
Question: What are the terminal voltages of each battery?
V375.111A625.0V12irV =Ω⋅−=−=εV375.11A625.0V2irV =Ω⋅−=−=εV625.41A625.0V4irV =Ω⋅+=−=ε
2V:4V:
12V:
![Page 8: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/8.jpg)
Multiloop Circuits
Kirchoff’s Rules1. in any loop
2. at any junction
0=∑i
iV
∑∑ =outinii
Find i, i1, and i2
Rule 1 – Apply to 2 loops (2 inner loops)
a.
b.
Rule 2
a.
045203412
12
1
=+−−=−−iiii
21iii +=
We now have 3 equations with 3 unknowns.
024503712
0)(3412
21
211
21
=−+−=−−
=+−−
iiii
iii
061215061424
21
21
=−+−=−−ii
ii
AiAi
Ai
i
0.25.0
5.12639
02639
2
1
1
==
==
=−
multiply by 2multiply by 3
subtract them
Find the Joule heating in each resistor P=i2R.
Is the 5V battery being charged?
![Page 9: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/9.jpg)
Method of determinants for solving simultaneous equations
524012043
0
21
1
21
=−+−=+−−
=−−
iiiiiii
Cramer’s Rule says if :
3332313
2322212
1312111
dicibiadicibiadicibia
=++=++=++
Then,
333
222
111
333
222
111
1
cbacbacba
cbdcbdcbd
i =
333
222
111
333
222
111
2
cbacbacba
cdacdacda
i =
333
222
111
333
222
111
3
cbacbacba
dbadbadba
i =
![Page 10: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/10.jpg)
i =
0 −1 −1
−12 −4 0
5 +4 −2
1 −1 −1
−3 −4 0
0 +4 −2
=
0−4 0
4 −2
⎛⎝⎜
⎞⎠⎟−1
0 −12
−2 5
⎛⎝⎜
⎞⎠⎟−1
−12 −4
5 4
⎛⎝⎜
⎞⎠⎟
1−4 0
4 −2
⎛⎝⎜
⎞⎠⎟−1
0 −3
−2 0
⎛⎝⎜
⎞⎠⎟−1
−3 −4
0 4
⎛⎝⎜
⎞⎠⎟
=24 + 48 −20
8 + 6 + 12=
52
26=2A
You try it for i1 and i2.
See inside of front cover in your book on how to use Cramer’s Rule.
For example solve for i
Method of determinants using Cramers Rule and cofactorsAlso use this to remember how to evaluate cross products of two vectors.
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Another example
Find all the currents including directions.
21
121
1
358023380
234480
iiiii
iiVVV
−−=−−−=
−−−++=
012120010166
0246
1
12
12
=+−=−+−
=++−
iii
ii0)1(246 2 =++− Ai
Loop 1
Loop 2
Ai 11 =
Ai
Ai
2
12
==
Loop 1
Loop 2
i i
i
i
i1i2
i2
21iii +=
024612=++− ii
Multiply eqn of loop 1 by 2 and subtract from the eqn of loop 2
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Rules for solving multiloop circuits
1. Replace series resistors or batteries with their equivalent values.
2. Choose a direction for i in each loop and label diagram.
3. Write the junction rule equation for each junction.
4. Apply the loop rule n times for n interior loops.
5. Solve the equations for the unknowns. Use Cramer’s Rule if necessary.
6. Check your results by evaluating potential differences.
![Page 13: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/13.jpg)
3 bulb question
The circuit above shows three identical light bulbs attached to an ideal battery. If the bulb#2 burns out, which of the following will occur?
a) Bulbs 1 and 3 are unaffected. The total light emitted by the circuit decreases.b) Bulbs 1 and 3 get brighter. The total light emitted by the circuit is unchanged.c) Bulbs 1 and 3 get dimmer. The total light emitted by the circuit decreases.d) Bulb 1 gets dimmer, but bulb 3 gets brighter. The total light emitted by the circuit is
unchanged.e) Bulb 1 gets brighter, but bulb 3 gets dimmer. The total light emitted by the circuit is
unchanged.f) Bulb 1 gets dimmer, but bulb 3 gets brighter. The total light emitted by the circuit
decreases.g) Bulb 1 gets brighter, but bulb 3 gets dimmer. The total light emitted by the circuit
decreases.h) Bulb 1 is unaffected, but bulb 3 gets brighter. The total light emitted by the circuit
increases.i) None of the above.
![Page 14: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/14.jpg)
When the bulb #2 is not burnt out:
R23
2RRR eq =+=
R3V2
RVI
231 ==
RIP,Power 2=RVI =
For Bulb #1
For Bulb #2
For Bulb #3
RV44.
R9V4RIP
22211 ===
R3V
2I
I 12 ==
RV11.
R9VRIP
22222 ===
R3V
2I
I 13 == R
V11.R9
VRIP22
233 ===
1I
2I
I 12 = 2
II 1
3 =
![Page 15: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/15.jpg)
R2RRR eq =+=
R2VI1 =
RIP,Power 2=RVI =
For Bulb #1
For Bulb #2
For Bulb #3
RV25.
R4VRIP
22211 ===
0I2 = 0RIP 222 ==
R2VII 13 == R
V25.R4
VRIP22
233 ===
1I
13 II =
So, Bulb #1 gets dimmer and bulb #3 gets brighter. And the total power decreases.
f) is the answer.
Before total power was R
V66.R
VRVP
2
23
2
eq
2
b ===
RV50.
R2V
RVP
22
eq
2
a ===After total
power is
When the bulb #2 is burnt out:
![Page 16: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/16.jpg)
How does a capacitor behave in a circuit with a resistor?
Charge capacitor with 9V battery with switch open, then remove battery.
Now close the switch. What happens?
![Page 17: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/17.jpg)
Discharging a capacitor through a resistor
V(t)
Potential across capacitor = V =
just before you throw switch at time t = 0.
Potential across Resistor = iR
at t > 0.
RC
QiRi
C
Q ooo
o=⇒=
C
Qo
What is the current I at time t?
RC)t(Q
)t(i =
RCQi =or
![Page 18: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/18.jpg)
dtdQi but ,
RCQi ,So −==
RCdt
QdQ
RCQ
dtdQ
=−
=−
Integrating both the sides
∫ ∫=−RCdt
QdQ
ARC
tQln +=−
ARCtA
RCt
eeeQ ,So −−−−==
ARC
tQln −−=
At t=0, Q=Q0
RCt
0eQQ −
=⇒
Time constant =RC
Q
0Q
RCt =
7.2Q
eQ =
t
What is the current I at time t?
AARC0
0 eeQ ,So −−−==
![Page 19: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/19.jpg)
RCt
0eQQ−
=
dtdQi = Ignore -
sign
i
tRC
RV0
What is the current?
RCt
0RCt
0 eRV
eRCQ −−
−=−=
![Page 20: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/20.jpg)
How the charge on a capacitor varies with time as it is being charged
What about charging the capacitor?
t
Q
i
t
00 QCV =
Same as before
)e1(CVQ RCt
0
−−=
γ−
=t
0 eRV
i
Note that the current is zero when either the capacitor is fully charged or uncharged. But the second you start to charge it or discharge it, the current is maximum.
![Page 21: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/21.jpg)
Instruments
Galvanometers: a coil in a magnetic field that senses current.
Ammeters: measures current.
Voltmeter: measures voltage.
Ohmmeters: measures resistance.
Multimeters: one device that does all the above.
Galvanometer is a needle mounted to a coil that rotates in a magnetic field. The amount of rotation is proportional to the current that flows
through the coil.
Symbolically we write
gRUsually when Ω=20Rg
milliAmp5.00Ig →=
![Page 22: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/22.jpg)
Ohmmeter
gs RRRVi
++= Adjust Rs so when R=0 the
galvanometer read full scale.
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Ammeter
V10A5 Ω2
gI
gR
sR
sI
A5I = A5I =≡
A5III sg =+=
ssgg RIRI =The idea is to find the value of RS that will give a full
scale reading in the galvanometer for 5A
A5A0005.A5I So, ,A105.0I and 20R s3
gg ≈−=×=Ω= −
Ω=Ω×==−
002.0)20(A5
A105.0RI
IR ,So
3
gs
gs
Ammeters have very low resistance when put in series in a circuit.
You need a very stable shunt resistor.
Very small
![Page 24: Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Warm-up problems Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples.](https://reader035.fdocuments.in/reader035/viewer/2022081519/56649ca85503460f9496b50b/html5/thumbnails/24.jpg)
Voltmeter
Use the same galvanometer to construct a voltmeter for which full scale reading in 10 Volts.
≡V10 Ω2
sR
gRI
Ω=×= −
20R
A105.0I
g
3g
What is the value of RS now?
)RR(IV10 gsg +=
A105V10
IV10RR
4g
gs −×==+
Ω=+ 000,20RR gs
Ω= 980,19Rs
So, the shunt resistor needs to be about 20KΩ
Note: the voltmeter is in parallel with the battery.
We need