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F on q 2
by q1
kq1q2
r2ˆ r
E caused
by q1
kq1
r2ˆ r
Ufrom q1and q 2
kq1q2
r
Vfrom q1k
q1
r
Baseball Diamond Heuristicof Electrostatics Equations
E caused
by q1
kq1
r2ˆ r
Ufrom q1and q 2
kq1q2
r
Vfrom q1point charge
kq1
r
F on q 2
by q1
q2
E from q1
Won q 2 q2V
(Usually find with Gauss’s Law.)
(Remember: V, the electric potential, has units of energy per unit charge.)
F
U
xˆ x
U
yˆ y
U
zˆ z
U(r ) U0
F d
s
r 0
r
E
V
xˆ x
V
yˆ y
V
zˆ z
V (r ) V0
E d
s
r 0
r
(scalar)
(scalar)
(vector)
(The change of electric potential a particle experiences moving from one position to another can be used to find the change in its kinetic energy via the “work-energy theorem”: K = W.)
(The potential energy stored in having 2charges at a distance r from each other.)
(The force between 2 charges at a distance r from each other.)
t
Vmotor
t
Vresistor
T
t1 t2
Vmotor,on
Vresistor,on
on on on onoff off off offoff
on on on onoff off off offoff
t (sec) V (Volts)0
0.0010.0030.0050.0070.0090.0110.0130.0150.0170.0190.0210.0230.025
t (sec) V1 (Volts) V2 (Volts)
00.0030.0060.0090.0120.015
200
100
red 1
red 2(channelinverted)
black(middleground)
+
-
200
100
red 1
black(bottomground)
red 2
+
-
I
I
I
current direction
always the same (so
is force on wire)
DC Power Supply+ -
these wiresfixed
brushesallow goodcontact as
loop rotates
Pulses let through by the diode move speaker withfrequency of desired audio wave.
Quantum mechanical turn-on voltage of diode.
Modulate Wave Transmitted by Diode to Speaker
RFModulator
IN GROUND
VariableCapacitor
SpeakerDio
de
(This is just to provide a ground.)external antenna
+
-
-
+{upward}
{outward}
“{upward}” and “{outward}” describewhich way the electron is deflected.
- +
{accelerated}
Vd,y Volts
0 Volts
d
w
z
y
coordinates
vf,z
vf,y
y
-
-
+
+
Va L
y’Dy
accelerationin z-direction
accelerationin y-direction
while crossingdeflection plates
constant motionwhile crossing
remaining distanceto screen
Energy (eV)
Momentum
Generic Plot of Energy Bands for Semiconductor
conduction band(empty)
valence band(filled with electrons)
E is called Band Gap Energy
Algebraic Equation Differential Equation
y+3 = 2
dy(t)
dt2y(t)
(involves a function y(t)and it’s parameter t)
(involves coordinate y)
y = -1(solution is a point/number) (solution is a function of t)
y(t) e2t
(-1)+3 = 2 …True!
(check solution by plugging point into original algebraic equation)
(check solution by plugging function into original differential equation)
d e2t dt
2e2t …True!