Reason (R): When we insert a dielectric between the plates of a capacitor, the induced charges tend to draw in the dielectric into the field (just as neutral objects are attracted by charged objects due to induction). We resist this force while slowly inserting the dielectric, and thus do negative work on the system, removing electrostatic energy from the system.
Solution:
When a dielectric is inserted into a disconnected charged capacitor, the charge \( Q \) remains constant. The capacitance \( C \) increases to \( kappa C_0 \), where \( \kappa \) is the dielectric constant. The energy stored is \( U = \frac{Q^2}{2C} \). Since \( C \) increases, \( U \) decreases. The external agent does negative work, as the dielectric is pulled in by electrostatic forces. This decrease in energy is explained by the work done by the field.
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