Revision notes · Electricity
Energy transfers
Power4.2.4.1
| Equation | Units |
|---|---|
| P = V × I | P in W, V in V, I in A |
| P = I² × R | P in W, I in A, R in Ω |
Power loss (as heat) in a component is proportional to the square of the current through it and to its resistance — this is why the National Grid transmits electricity at a high potential difference and low current: for the same power transferred, a lower current means much less power is wasted heating the cables.
Energy transfers in everyday appliances4.2.4.2
Everyday electrical appliances transfer energy electrically from batteries or the mains to other, more useful stores — for example, a motor transfers electrical energy mainly to a kinetic energy store, and a kettle transfers electrical energy mainly to a thermal energy store.
| Equation | Units |
|---|---|
| E = P × t | E (energy transferred) in J, P (power) in W, t (time) in s |
| E = Q × V | E (energy transferred) in J, Q (charge) in C, V (potential difference) in V |
The National Grid4.2.4.3
- •Step-up transformers increase the potential difference (and correspondingly decrease the current) between the power station and the transmission cables.
- •Step-down transformers decrease the potential difference again, from the National Grid to a safer level for consumers.
Since power = potential difference × current (P = VI), transmitting power at a very high potential difference keeps the current low for the same power delivered. Because power lost as heat in the cables depends on the square of the current (P = I²R), a lower current dramatically reduces the energy wasted heating the cables over long transmission distances.
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