The Maxwell-Ampere Law Can Be Written As $\oint \vec { B } \cdot d \vec { s } = \mu _ { 0 } I + \mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }$

The Maxwell-Ampere Law can be written as $\oint \vec { B } \cdot d \vec { s } = \mu _ { 0 } I + \mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }$ . The term in the equation that does not contribute to the theoretical description of the propagation of an electromagnetic wave pulse is

A) $\oint \vec { B } \cdot d \vec { s }$
B) $\mu _ { 0 } I$
C) $\mu _ { 0 } \varepsilon _ { 0 } \frac { d \Phi _ { E } } { d t }$
D) No term in this equation is related to the propagation of the electromagnetic wave pulse.