Stored inductor energy grows with current squared, so the ceiling can be safe at low current, exactly reached, and exceeded by the next row. With 2 H, currents 1, 2, and 3 A store 1, 4, and 9 J against a 4 J ceiling exactly for the ideal inductor model; real inductors add saturation, winding resistance, core loss, thermal limits, ripple, current-sense tolerance, and energy measurement uncertainty.

The square-current energy ledger is checked against an energy ceiling. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

1 A energy row

Inductance stays 2 H. Current 1 A stores 1 J against a 4 J ceiling, so margin is 3 J.

E=1 J,m=3 J⇒passE=1\ \text{J},\quad m=3\ \text{J}\Rightarrow\text{pass}
Stored-energy ceiling boundaryThe current square law is checked before the limit.L 2 HI 1 AE 1 JI0 0 AE0 0 JdE 1 J

2 A energy row

Inductance stays 2 H. Current 2 A stores 4 J against a 4 J ceiling, so margin is 0 J.

E=4 J,m=0 J⇒passE=4\ \text{J},\quad m=0\ \text{J}\Rightarrow\text{pass}
Stored-energy ceiling boundaryThe current square law is checked before the limit.L 2 HI 2 AE 4 JI0 0 AE0 0 JdE 4 J

3 A energy row

Inductance stays 2 H. Current 3 A stores 9 J against a 4 J ceiling, so margin is negative 5 J.

E=9 J,m=−5 J⇒failE=9\ \text{J},\quad m=-5\ \text{J}\Rightarrow\text{fail}
Stored-energy ceiling boundaryThe current square law is checked before the limit.L 2 HI 3 AE 9 JI0 0 AE0 0 JdE 9 J