Coulomb's Law - Vector form 1
Description:
.fraction {
display: inline-block;
vertical-align: middle;
margin: 0 0.2em 0.4ex;
text-align: center;
}
.fraction > span {
display: block;
padding-top: 0.15em;
}
.fraction span.fdn {border-top: thin solid black;}
.fraction span.bar {display: none;}
.sy {
position: relative;
text-align: center;
}
.oncapital, .onsmall {
position: absolute;
top: -1.2em;
left: -1px;
width: 100%;
font-size: 70%;
text-align: center;
}
.onsmall {
top: -1em;
}
We know that force in q vector quantity, so it will have magnitude as well as directon.
F = 14πεo q1q2r2
This equation gives only magnitude.
Notation for direction
Consider the direction q1 to q2
‘r’ is the displacement between them. So, displacement in the vector form can be written as −
(r21→ denotes, displacement upto point 2 from point 1)
Now, Vector r21→ can be written as −
r21→ = r̂21 |r21|→
Here −
‘r21’ is a full vector
‘r̂21’ is a unit vector
|r21|→ is the magnitude
Coulumb Force Vector
Coulumb Force is always along the straight line going the two charges.
Let,
Both the charges are similar.
Q2 is experiencing force due to q1. So, force vector can be written as −
F21→
F21→ represents, force on charge q2 due to charge q1.
So, Vector equation of coulomb force can be written as −
Format 1 − F21→ = 14πεo q1q2r2 r̂21 .....(1)
(Unit vector r̂21, its magnitude is always equal to 1. So, it doesn’t charges value, it only gives the direction)
We know that r̂21 = r21→r .....(2)
Putting (2) in (1) we get −
Format 2 − F21→ = 14πεo q1q2r3r21→