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Chapter 18 Notes College Physics by Giambattista et al. Basic DC ...

Chapter 18 Notes College Physics by Giambattista et al. Basic DC ...

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<strong>Chapter</strong> <strong>18</strong> <strong>Notes</strong><br />

<strong>College</strong> <strong>Physics</strong> <strong>by</strong> <strong>Giambattista</strong> <strong>et</strong> <strong>al</strong>.<br />

<strong>Basic</strong> <strong>DC</strong> Circuit:<br />

“V – C – R”<br />

+<br />

voltage LOAD<br />

source<br />

–<br />

Voltage Sources:<br />

1) Batteries: chemic<strong>al</strong> electric<strong>al</strong><br />

2) Solar cells: light electric<strong>al</strong><br />

3) Generators: magn<strong>et</strong>ism electric<strong>al</strong><br />

4) Thermocouples: heat electric<strong>al</strong><br />

5) Piezoelectric cryst<strong>al</strong>: pressure electric<strong>al</strong><br />

Emf E – “electromotive force”<br />

theor<strong>et</strong>ic<strong>al</strong>, ide<strong>al</strong> voltage difference<br />

voltage difference when source is not in use<br />

Electric Current I<br />

n<strong>et</strong> flow of charge<br />

convention<strong>al</strong> vs. electron flow<br />

ac vs. dc<br />

I<br />

q<br />

<br />

t<br />

SI unit: ampere (A) = coulomb/sec<br />

Resistance R<br />

measure of how well a device conducts electricity, e.g. high R low I<br />

depends on:<br />

1) materi<strong>al</strong> 3) length<br />

2) temperature 4) width (thickness)<br />

For a wire,<br />

R <br />

L<br />

A<br />

SI unit: ohm (Ω)<br />

ρ is the resistivity in Ω-m, Table <strong>18</strong>.1, p.646<br />

Resistors<br />

have a fixed resistance<br />

may be purchased commerci<strong>al</strong>ly<br />

regulate voltage and current, essenti<strong>al</strong> to every circuit<br />

John B. Ross, Ph.D.<br />

IUPUI <strong>Physics</strong> Dept.


<strong>Chapter</strong> <strong>18</strong> <strong>Notes</strong><br />

<strong>College</strong> <strong>Physics</strong> <strong>by</strong> <strong>Giambattista</strong> <strong>et</strong> <strong>al</strong>.<br />

Ohm’s Law: ΔV = IR for resistors only!<br />

Termin<strong>al</strong> Voltage V t<br />

voltage difference b<strong>et</strong>ween the termin<strong>al</strong>s of a power supply when it’s in use<br />

V t = E<br />

V t = E – Ir<br />

V t = E + Ir<br />

when not in use<br />

when energy leaves battery (to power circuit)<br />

when energy enters battery (“charging”)<br />

Electric Power<br />

rate of electric<strong>al</strong> energy transfer<br />

U<br />

E qV<br />

P P = IΔV in gener<strong>al</strong> Note: watt = amp*volt!<br />

t<br />

t<br />

For resistors, ΔV = IR <br />

P = I 2 R<br />

or<br />

2<br />

V<br />

P <br />

R<br />

Joule heat formulas<br />

Question:<br />

What are you being billed for <strong>by</strong> the electric company??<br />

Energy measured in kilowatt-hours = (kilowatts)(hours) = PΔt<br />

In the SI,<br />

joules = (watts)(sec)<br />

Resistor Combinations<br />

I. Series – like a train, same current<br />

R 1 R 2 R 3 R eq = Σ R i<br />

<br />

E<br />

When one goes out, they <strong>al</strong>l go out – “open circuit”<br />

II. Par<strong>al</strong>lel – like a ladder, same voltage difference<br />

1 1<br />

<br />

R eq<br />

R i<br />

E R 1 R 2 R 3<br />

John B. Ross, Ph.D.<br />

IUPUI <strong>Physics</strong> Dept.


<strong>Chapter</strong> <strong>18</strong> <strong>Notes</strong><br />

<strong>College</strong> <strong>Physics</strong> <strong>by</strong> <strong>Giambattista</strong> <strong>et</strong> <strong>al</strong>.<br />

<br />

<br />

<br />

When one goes out, the rest stays on.<br />

More paths, more current to flow potenti<strong>al</strong> hazard!<br />

discuss fuses, circuit-breakers<br />

Short circuit – illeg<strong>al</strong> par<strong>al</strong>lel connection, path of least resistance<br />

Solving <strong>DC</strong> Circuits: Two M<strong>et</strong>hods<br />

M<strong>et</strong>hod#1 – Resistor Combinations<br />

M<strong>et</strong>hod #2 – Kirchhoff’s Rules<br />

Junction Rule: Σ I in – Σ I out = 0 at any single junction<br />

Loop Rule: Σ V rise – Σ V drop = 0 around any closed loop<br />

Solving Multiloop Circuits Using KR:<br />

1) Draw and label currents I 1 , I 2 , I 3 in each branch.<br />

2) Write termin<strong>al</strong>s on each device:<br />

3) Pick a junction and apply the Junction Rule.<br />

4) Apply the Loop Rule to two different loops.<br />

5) You have 3 equations, 3 unknowns – solve for I 1 , I 2 , I 3 .<br />

RC Circuits<br />

Have you ever used an expensive camera with a flashbulb that needs to charge before you<br />

snap the picture?<br />

I. Charging Circuit<br />

S V C (t) = E(1 – e –t/τ ) τ = RC<br />

I(t) = (E/R)e –t/τ<br />

E C<br />

max<br />

R 0 t<br />

II. Discharging Circuit<br />

S V C (t) = Ee –t/τ τ = RC<br />

I(t) = (E/R)e –t/τ<br />

R C<br />

max<br />

0 t<br />

John B. Ross, Ph.D.<br />

IUPUI <strong>Physics</strong> Dept.

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