Title: Winter wk 3
1Winter wk 3 Thus.20.Jan.05
- Ch.24 Voltage and electric field
- Ch.26 Current and resistance
- Solar applications
- Ch.27 Circuits
Energy Systems, EJZ
2Equipotential surfaces and E fields
Equipotential constant voltage Conductors are
equipotentials, in electrostatics Potential
difference ? Electric field dV/dx -E or,
equivalently, Practice Ch.24 Q5,8
(p.646), P3, 4, 6, 35
3Ch.24 4
4Ch.24 6
5Ch.24 35
6Electrostatics (d/dt0) charges ? fields ?
forces, energy
- Charges make E fields and forces
- charges make scalar potential differences dV
- E can be found from V
- Electric forces move charges
- Electric fields store energy (capacitance)
F q E m a
W qV, C q/V
7Ch.26 Currents and Resistance
- Current rate of flow of charge
- I dq/dt
- Units amps coulombs/sec
- Current density J current/area n e v
- Ch.26 Q1, 2, P.1, 8
- Water flow Electricity flow
- pressure voltage V
- volume/time current I
-
8Ch.26 Q1, 2, P.1, 8
9Resistance
- Resistance resistivity area/length
- R r A/L
- Which conductor has the greatest resistivity?
- Ch.26 Q3
10Ohms law
- In many substances, for a given resistance R, the
stronger the driving voltage, the greater the
current that flows - Voltage current resistance
- V I R
- Ch.26 Q5, P.17
11Power in electric circuits
- Power rate of energy xfr voltagecurrent
- P V I
- units Watts volts amps
- Recall that work qV. Units J CV
- Solve for V(J,C)
- Then voltsamps ____C/s ______
- If VIR, find P(I,R) P(R,V)
- Ch.26 35, 64
12Ch.27 Circuits
- Battery pumps electricity ? current flows
http//hyperphysics.phy-astr.gsu.edu/hbase/electri
c/watcir.htmlc1
13Voltage emf
- DVoltage potential difference
- Electromotive force e DV dW/dq work done per
unit charge - de/dx -E electric field
14Emf e and electric field E
- de/dx -E electric field
- Using the fundamental theorem of calculus, we can
derive another of Maxwells eqns
15Ch.27 Practice with simple circuits
16Solar applications
- Storms from the Sun
- p.13 If a CME travels at 1 million miles per
hour, how long does it take to reach Earth? - p.16 The 2 May 1994 event dumped 4600 GW-hr of
electricity into Earths upper atmosphere. How
much energy is that in Joules? - p.16 If the Earths mean magnetic field is
B00.5 Gauss, and one Tesla104 Gauss, by what
percent does 2000 nanoTesla change Earths field? - p.54 For the CME of 1 Sept 1859 calculate its
speed v, if it took 18 hours to reach Earth.
17more Solar applications
- Storms from the Sun
- p.77 If Rsun 100 REarth, then find the ratio
of their volumes, Vsun/VEarth - p.77 If m5 millions tons of mass is converted
to energy (Emc2) each second, calculate the
power (P) produced by the Sun. - p.82 If the Suns mass is M2x1030 kg, and it
keeps losing dm/dt 5 million tons per second,
how long (T) can the Sun last? - p.83 If the solar wind pours I1 million amps
into Earths magnetosphere, how much charge (Q) is
that per day?
18Extra solar applications
- p.13 Calculate vthermal from Tsolar wind.
Compare to vflow. - p.16 Derive the altitude for a geosynchronous
orbit - p.77 If the Suns core temperature is about
T107K, calculate the thermal speed vth of
protons in the core.