A charge q is moving slowly with a uniform velocity . Obtain an expression for the vector potential and the magnetic field at a distance r from it.
solution
we are considering charge is moving with uniform velocity V in direction +X axis.the charge is at origine at time t=0.at any instant t
its position are x=vt, y=z=0
then retarded time
t'=t - r'/c ................eq.1
where r' is distance to the point A from charge q at retarded time.
at the erlier time the charge was at position
x=vt'
therefore
"r'=\\sqrt{(x-vt')^2+y^2+z^2}" ........eq.2
using equation 1 and 2
"r'^2=c^2(t-t')^2=(x-vt')^2+y^2+z^2"
"(v^2-c^2)t^2-2(xv-c^2t)t'+x^2+y^2+z^2-c^2t^2=0"
this is the quadratic equation in t'
its solution can be found using shridhar aacharya formula.and
value of t' putting in equation 1
we get
r' = c(t - t') ........eq.3
scaler potential can be written for a charge q which is moving with velocity v is given by
"\\phi(x,y,z,t)=\\frac{q}{4\\pi\\in_0(r'-v.r'\/c)}"
"\\phi(x,y,z,t)=\\frac{q}{4\\pi\\in_0(\\sqrt{(x-vt)^2+(1-v^2\/c^2)(y^2+z^2)}}"
"\\phi(x,y,z,t)=\\frac{q}{4\\pi\\in_0\\sqrt{(1-v^2\/c^2)}(\\sqrt{((x-vt)\/(\\sqrt(1-v^2\/c^2))^2+(y^2+z^2)}}"
relation between vector potential and scaler potential is
"A=\\frac{v\\phi}{c^2}"
for a charge q at a time t and position (vt,0,0)
then vector potential is given by
"A_x=\\frac{q}{4\\pi\\in_0\\sqrt{(1-v^2)}(\\sqrt{(x-vt)^2\/((1-v^2)+(y^2+z^2)}}" ...eq.4
and Ay=Az=0 because we are considering that charge q is moving in +ve x direction.
now
megnetic field for charge q which is moving with unnifonrm velocity v is
"B=\\nabla\\times A"
putting the value of Ax , Ay , Az then magnetic field will be
"\\fcolorbox{red}{aqua}{$B=\\frac{\\mu_0 \\space qv\\times r}{4\\pi c^2\\space r^3}$}"
this magnetic field must be in z direction because Electric field E,manetic field B and velocity v are perpendicular to each other.
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