electrostatics
Chapter-1: <ctrie chavgcs and electie Fill
Electie charge: charg is
mottr due to whieh it oduces ad exeriences electrie
and mmagmetie et.
The electte cherge is 'g
There are tuoo tes chargs, a RosItine a-d a
gatie charg
Aroton is positag charged outs cle , haing a -27
+ 1.6 x03 an has maS S
A meutron is a meutral þartiele ,i.e, ta
a netron is erO.
ngatig chargd partide
An elechvom
charge
is
- 1.6 x16
C
avd has a mas S havig
3
Te S.I. unt electrie chor Coulob (c)
6
1 Coulomb charg 6 25 x10
electroms
electro
charg
4
1. e
,16
1 e 1.6 ×\oC
,Condctovs ! Those
Th ohich readily allouos ta passa
4hem are callel Conduetovs .
throug
.4, silvey, coer , ete.
9nsulators: Those substamees whick o s hih resistanee
to asag cdetrittg CAre called insulatovs .
ylastieoe., ebe.
t is Cauied by he tranler eleethas.
frictiowal £lectiity'
eroherties o} electie charge.
9t means a sgtm couststs n chag's
than tohal char
wil be
4,t,v,
are discrete
uanti tation of charge 9t mean S charges
and not Contimuous.
charg body
cohene n z 0, , 2,3,
1.6 x\O
and e' is electronie charge
means +hat tke totaI
i) ConServation charg Coser
an isolated sytem is aloag
Coulomb's Lass
, The electoshate loree betwen twe oit chorgs is
betwen two
dectly ortio ndl to e roduct of thel maguitude.
dargs and imetrscl, oianal to the Sauare o e
distance thei
between ceutres.
F
2
cohen Nm?
ohore, is obsalute ermitiihy d ree sae
2
or Valuum
E.8. 85 10
¬ s absolute medium.
Also,
Here, or k s relatine gemA
te medium anol is also kuown as Atelecie
Comshaut.
1 Coulomb i 1 Coulomb is that whieh when laced
1m grom an
eana amd Similar eharge in
Vacuum (or al) mels it witt a
Chapter-1: <ctrie chavgcs and electie Fill
Electie charge: charg is
mottr due to whieh it oduces ad exeriences electrie
and mmagmetie et.
The electte cherge is 'g
There are tuoo tes chargs, a RosItine a-d a
gatie charg
Aroton is positag charged outs cle , haing a -27
+ 1.6 x03 an has maS S
A meutron is a meutral þartiele ,i.e, ta
a netron is erO.
ngatig chargd partide
An elechvom
charge
is
- 1.6 x16
C
avd has a mas S havig
3
Te S.I. unt electrie chor Coulob (c)
6
1 Coulomb charg 6 25 x10
electroms
electro
charg
4
1. e
,16
1 e 1.6 ×\oC
,Condctovs ! Those
Th ohich readily allouos ta passa
4hem are callel Conduetovs .
throug
.4, silvey, coer , ete.
9nsulators: Those substamees whick o s hih resistanee
to asag cdetrittg CAre called insulatovs .
ylastieoe., ebe.
t is Cauied by he tranler eleethas.
frictiowal £lectiity'
eroherties o} electie charge.
9t means a sgtm couststs n chag's
than tohal char
wil be
4,t,v,
are discrete
uanti tation of charge 9t mean S charges
and not Contimuous.
charg body
cohene n z 0, , 2,3,
1.6 x\O
and e' is electronie charge
means +hat tke totaI
i) ConServation charg Coser
an isolated sytem is aloag
Coulomb's Lass
, The electoshate loree betwen twe oit chorgs is
betwen two
dectly ortio ndl to e roduct of thel maguitude.
dargs and imetrscl, oianal to the Sauare o e
distance thei
between ceutres.
F
2
cohen Nm?
ohore, is obsalute ermitiihy d ree sae
2
or Valuum
E.8. 85 10
¬ s absolute medium.
Also,
Here, or k s relatine gemA
te medium anol is also kuown as Atelecie
Comshaut.
1 Coulomb i 1 Coulomb is that whieh when laced
1m grom an
eana amd Similar eharge in
Vacuum (or al) mels it witt a
