4.7.3.4b - Transformer Power, Current and Transmission

4.7.3.4b - Transformer Power, Current and Transmission

A transformer can change potential difference, but an ideal transformer does not create extra electrical power. This Higher-tier physics-only lesson uses that idea to calculate currents and to explain why the National Grid transmits electricity at high potential differences. The key pattern is simple but powerful: for the same power transfer, a larger potential difference means a smaller current.

Ideal Transformer Power

A real transformer always wastes some energy, usually by heating the coils and core. In the AQA GCSE model for this lesson, we often start with an ideal transformer: a transformer that is 100% efficient.

Ideal Transformer

An ideal transformer is a transformer that is 100% efficient, so its electrical power output equals its electrical power input.

A brief reminder of the mechanism: an alternating current in the primary coil produces a changing magnetic field in the core, and that changing field induces a potential difference across the secondary coil.

If a transformer is 100% efficient, the power in the primary coil is equal to the power in the secondary coil:

power input=power output\text{power input} = \text{power output}

Electrical power in a coil is found from potential difference multiplied by current, so:

Ideal Transformer Power Equality

VpIp=VsIsV_p I_p = V_s I_s

where VpV_p is the potential difference across the primary coil, IpI_p is the current in the primary coil, VsV_s is the potential difference across the secondary coil, and IsI_s is the current in the secondary coil.

[DIAGRAM: asset_name: ideal_transformer_power_and_current - diagram 1; asset_slug: 112_4_7_3_4b_transformer_power_current_and_transmission_diagram1; file: diagram_assets/112_4_7_3_4b_transformer_power_current_and_transmission_diagram1.png; recommended_method: image_gen; description: Built-in Codex Image Gen transformer schematic showing a primary coil, iron core and secondary coil, with the secondary coil drawn with clearly more turns for a step-up transformer. The example labels show Vp=230 VV_p = 230\text{ V}, Ip=10 AI_p = 10\text{ A}, Vs=2300 VV_s = 2300\text{ V}, Is=1.0 AI_s = 1.0\text{ A}, and equal powers VpIp=VsIs=2300 WV_pI_p = V_sI_s = 2300\text{ W}. The visual teaches that stepping up potential difference lowers current for the same ideal power transfer. Generated with built-in Codex Image Gen; nearby prose states the exact relationships for accessibility.]
Diagram

The equation is given on the Physics equation sheet. The exam skill is choosing it, identifying primary and secondary values, rearranging it correctly, and using watts for power.

Current Changes with Potential Difference

The ideal transformer equation shows that current changes in the opposite direction to potential difference when the power transfer is the same.

For a step-up transformer, the secondary potential difference is greater than the primary potential difference. In an ideal transformer, the secondary current must therefore be smaller than the primary current. The transformer has not made extra power; it has transferred roughly the same power at a higher potential difference and a lower current.

For a step-down transformer, the secondary potential difference is smaller than the primary potential difference. In an ideal transformer, the secondary current is therefore larger than the primary current.

This is the common AQA trap: "step-up" describes the potential difference, not the current. A step-up transformer steps up VV and steps down II. A step-down transformer steps down VV and steps up II, assuming ideal power transfer.

Worked example: an ideal transformer has Vp=25 VV_p = 25\text{ V}, Ip=4.0 AI_p = 4.0\text{ A}, and Vs=100 VV_s = 100\text{ V}. Calculate the secondary current.

VpIp=VsIsV_p I_p = V_s I_s 25×4.0=100×Is25 \times 4.0 = 100 \times I_s 100=100Is100 = 100I_s Is=1.0 AI_s = 1.0\text{ A}

The potential difference has increased by a factor of 4, so the current has decreased by a factor of 4.

Input Current Calculations

AQA specifically expects you to calculate the current drawn from the input supply to provide a particular power output. The phrase "current drawn from the input supply" means IpI_p, the primary current.

If the output power is given directly, use:

Pin=PoutP_\text{in} = P_\text{out}

for an ideal transformer, then:

Pin=VpIpP_\text{in} = V_p I_p

so:

Ip=PoutVpI_p = \frac{P_\text{out}}{V_p}

[DIAGRAM: asset_name: input_current_from_output_power - diagram 2; asset_slug: 112_4_7_3_4b_transformer_power_current_and_transmission_diagram2; file: diagram_assets/112_4_7_3_4b_transformer_power_current_and_transmission_diagram2.png; recommended_method: deterministic_drawn; description: Exact deterministic worked-equation flow showing an output device needing 60 W60\text{ W}, an ideal transformer, an input supply of 230 V230\text{ V}, and the calculation Ip=Pout/Vp=60/230=0.26 AI_p = P_\text{out}/V_p = 60/230 = 0.26\text{ A}. The visual teaches how to identify input current from output power without confusing primary and secondary values. Deterministic drawing is required because the values, equation layout and labels are assessed.]
Diagram

Worked example: an ideal transformer supplies a 60 W60\text{ W} output device. The input supply is 230 V230\text{ V}. Calculate the current drawn from the input supply.

Pin=Pout=60 WP_\text{in} = P_\text{out} = 60\text{ W} Pin=VpIpP_\text{in} = V_p I_p 60=230×Ip60 = 230 \times I_p Ip=60230=0.26 AI_p = \frac{60}{230} = 0.26\text{ A}

The current drawn from the input supply is 0.26 A0.26\text{ A} to 2 significant figures.

If a question gives secondary values instead of output power, calculate output power first:

Pout=VsIsP_\text{out} = V_s I_s

then use Pin=PoutP_\text{in} = P_\text{out} for the ideal transformer.

Continue this lesson.

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