Paper 1 Conservation Laws in Physics Answers
| Q | Answer | Reason |
|---|
| 1 | A | System boundary determines what is conserved. |
| 2 | B | Momentum is conserved when resultant external impulse is zero or negligible over the interaction. |
| 3 | C | Current continuity follows from charge conservation. |
| 4 | D | Energy is transferred or transformed but not created or destroyed. |
| 5 | B | Nucleon or mass numbers are the upper numbers. |
| 6 | C | Proton or nuclear-charge numbers are the lower numbers. |
| 7 | A | Mass defect appears as energy. |
| 8 | D | Initial total momentum is zero, so the final vector sum is zero. |
| 9 | A | Kinetic energy can transform to internal energy. |
| 10 | B | Kirchhoff’s first law is charge conservation at a junction. |
| 11 | C | Kirchhoff’s second law is energy conservation per unit charge around a loop. |
| 12 | A | Boundary mistakes invalidate conservation claims. |
| 13 | B | Momentum has direction and is a vector. |
| 14 | D | Energy has no direction and is a scalar. |
| 15 | A | Mechanical energy can be dissipated to thermal energy outside chosen mechanical store. |
| 16 | B | Total charge is constant for an isolated system. |
| 17 | A | One nucleon remains one nucleon. |
| 18 | C | The loop rule is energy accounting per unit charge. |
| 19 | A | Choose system and check external interactions. |
| 20 | D | Internal transfers redistribute a conserved quantity without changing the system total. |