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Let's do your simple example first. Just a DC circuit with a resistor. To be more realistic we take into account also the self-inductance of the system. We can describe it as a series of an ideal resistor and a ideal coil. Then we use the equations for circuits, which are nothing else than a quasistationary approximation of Maxwell's equations.
The differential equation describing this system is then given by
[tex]L \dot{i}+R i=U(t),[/tex]
where [itex]L[/itex] is the self-inductance, [itex]R[/itex] the resistance, [itex]i[/itex] the current, and [itex]U(t)[/itex] the battery. Being switched on at [itex]t_0=t[/itex], we have
[tex]U(t)=U_0 \Theta(t).[/tex]
Now we simply solve this equation with the initial condition [itex]i(0)=0[/itex]. We get for [itex]t>0[/itex]
[tex]i(t)=\frac{U_0}{R} \left [1-\exp \left(-\frac{R}{L} t \right ) \right ].[/tex]
Now we calculate the total power for [itex]t>0[/itex]
[tex]P(t)=U(t) i(t)[/tex]
and the total amount of work done at time [itex]t[/itex]
[tex]E_{\text{tot}}(t)=\int_0^t \mathrm{d}t' P(t')=\frac{U_0^2}{R} t+\frac{L U_0^2}{R^2} \left[1-\exp \left(-\frac{R}{L} t \right) \right].[/tex]
The amount of work converted into heat is given by the Ohm loss
[tex]E_{\text{loss}}(t)=\int_0^{t} \mathrm{d} t' R i^2(t')=\frac{U_0^2}{2 R} \left
[2 R t -3L - L\exp \left(-\frac{2 R t}{L} \right )+4 L \exp \left (-\frac{R t}{L} \right ) ) \right ].[/tex]
The reminder is used to build up the magnetic field
[tex]E_{\text{mag. field}}(t)=\frac{L U_0^2}{2 R^2} \left [1-\exp \left (-\frac{R t}{L} \right ) \right ]^2=\frac{L}{2}i^2(t).[/tex]
The only work done on the charges obviously is the Ohmian loss, which is not due to the magnetic field built up and counteracting the builtup of the current (Lenz's Law).
In the stationary limit, one has the asymptotic behaviour
[tex]E_{\text{tot}}(t) \simeq \frac{L U_0^2}{2 R^2}+\frac{U_0^2}{R} t = \frac{L i_{\infty}^2}{2} + U_0 i_{\infty} t.[/tex]
Of course the total energy is conserved (heat + magnetic-field energy) and comes from the battery.
The differential equation describing this system is then given by
[tex]L \dot{i}+R i=U(t),[/tex]
where [itex]L[/itex] is the self-inductance, [itex]R[/itex] the resistance, [itex]i[/itex] the current, and [itex]U(t)[/itex] the battery. Being switched on at [itex]t_0=t[/itex], we have
[tex]U(t)=U_0 \Theta(t).[/tex]
Now we simply solve this equation with the initial condition [itex]i(0)=0[/itex]. We get for [itex]t>0[/itex]
[tex]i(t)=\frac{U_0}{R} \left [1-\exp \left(-\frac{R}{L} t \right ) \right ].[/tex]
Now we calculate the total power for [itex]t>0[/itex]
[tex]P(t)=U(t) i(t)[/tex]
and the total amount of work done at time [itex]t[/itex]
[tex]E_{\text{tot}}(t)=\int_0^t \mathrm{d}t' P(t')=\frac{U_0^2}{R} t+\frac{L U_0^2}{R^2} \left[1-\exp \left(-\frac{R}{L} t \right) \right].[/tex]
The amount of work converted into heat is given by the Ohm loss
[tex]E_{\text{loss}}(t)=\int_0^{t} \mathrm{d} t' R i^2(t')=\frac{U_0^2}{2 R} \left
[2 R t -3L - L\exp \left(-\frac{2 R t}{L} \right )+4 L \exp \left (-\frac{R t}{L} \right ) ) \right ].[/tex]
The reminder is used to build up the magnetic field
[tex]E_{\text{mag. field}}(t)=\frac{L U_0^2}{2 R^2} \left [1-\exp \left (-\frac{R t}{L} \right ) \right ]^2=\frac{L}{2}i^2(t).[/tex]
The only work done on the charges obviously is the Ohmian loss, which is not due to the magnetic field built up and counteracting the builtup of the current (Lenz's Law).
In the stationary limit, one has the asymptotic behaviour
[tex]E_{\text{tot}}(t) \simeq \frac{L U_0^2}{2 R^2}+\frac{U_0^2}{R} t = \frac{L i_{\infty}^2}{2} + U_0 i_{\infty} t.[/tex]
Of course the total energy is conserved (heat + magnetic-field energy) and comes from the battery.