Maxwell-s modified form of Ampere-s circuital law isdisplaystyleoint-displaystyle s-vec-B-vec-dl-mu-0Idisplaystyleoint-displaystyle s-vec-B-vec-ds-0displaystyleoint-displaystyle s-vec-B-vec-dl-mu-0I-frac-I-varepsilon-o-frac-dq-dt-displaystyleoint-displaystyle s-vec-B-vec-dl-mu-0I-mu-0varepsilon-ofrac-dphi-E-dt-

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Toppr Admin · Accepted Answer

Answer-x2212- DTreating all charges on the same footing -disregarding whether they are bound or free charges- the generalized Amp-xE8-re-apos-s equation- also called the Maxwell-x2013-Amp-xE8-re equation- is in integral form-

Maxwell's modified form of Ampere's circuital law is
$\oint_{s} \to B . \to d l = μ_{0} I$
$\oint_{s} \to B . \to d s = 0$
$\oint_{s} \to B . \to d l = μ_{0} I + \frac{I}{ε_{o}} \frac{d q}{d t}$
$\oint_{s} \to B . \to d l = μ_{0} I + μ_{0} ε_{o} \frac{d ϕ_{E}}{d t}$

$A n s w e r : -$ D
Treating all charges on the same footing (disregarding whether they are bound or free charges), the generalized Ampère's equation, also called the Maxwell–Ampère equation, is in integral form.

Maxwell's modified form of Ampere's circuital law is∮s→B.→dl=μ0I∮s→B.→ds=0∮s→B.→dl=μ0I+Iεodqdt∮s→B.→dl=μ0I+μ0εodϕEdt

Answer:− DTreating all charges on the same footing (disregarding whether they are bound or free charges), the generalized Ampère's equation, also called the Maxwell–Ampère equation, is in integral form.

Maxwell's modified form of Ampere's circuital law is
$\oint_{s} \to B . \to d l = μ_{0} I$
$\oint_{s} \to B . \to d s = 0$
$\oint_{s} \to B . \to d l = μ_{0} I + \frac{I}{ε_{o}} \frac{d q}{d t}$
$\oint_{s} \to B . \to d l = μ_{0} I + μ_{0} ε_{o} \frac{d ϕ_{E}}{d t}$

$A n s w e r : -$ D
Treating all charges on the same footing (disregarding whether they are bound or free charges), the generalized Ampère's equation, also called the Maxwell–Ampère equation, is in integral form.