Grasp the complexities of electrodynamics with these structured notes. From electric fields to electromagnetic induction, this guide offers detailed explanations and practical examples for easy learning.
Contains many examples and diagrams making learning easy.
fodnatuofjpnd
" the direction of the force on a current -
carrying
SINGLE LOOP OF WIRE
T Force ( F)
i Recurrent
"
magnetic.ci
.
SOLENOID
ion
"
ELECTROMAGNET
-
on
.÷÷E⇐÷i÷÷
FACTORS AFFECTING THE SHE
RRCE
O ON THE
" " " " " " " " "" "" "
÷÷÷÷÷:÷÷÷÷÷÷÷i÷ .
=
, DC MOTOR
convert electrical energy into mechanical energy
CLOCKWISE
@ F-
Ts
E¥tFtF¥
N
/
y s
#
x
. . a-
-
g-
N S Function of a split ring commutator in
ambo for
T④④ • reverse the direction of the current in the
↳#
every half revolution ( 180
-
coil rev )
SPLIT RING me
dinette
• Ensures the coil continues to spin
I
,
-1 COMMUTATOR
SOURCE #
Nt#
DC
s
a-
-
ELECTROMAGNETIC INDUCTION
Wb AREA
-
Q = BA cos O
marine mi:*.
age;¥:*;
"
= ,
Flux through SA of coil M ( count field lines )
t
as the magnet approaches the coli
&
t
f
µq
changing induces an em
Ifa't
→ slope
-
'
.
induced a current -
Magnetic flux density ( B) is a representation of
¥
the magn 8 direction of MF
" E
.
- -
'
t
µ
FARADAY 'S LAW
.
induced
eme.in#iIOin:nn..e
Dt
. ..
its E its ⇐ its
Cmf
0 Max o
ft EI Efts
o max
current induced Is proportional to RATE OF CHANGE OF FLUX
NOT magnitude of flux
If
a. in:*.is :* : ::i:::::i: inanimate
" ""
.mn .
LENZ 'S LAW
induced current flows direction so as to
The in a set up a
magnetic
field to oppose the the change in the magnetic flux
C- = IR
I = E
a
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