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GRADE 8 · WORK AND CURRENT POWER

Thermal effect of current and safety

Joule-Lenz law, heaters, short circuits and protection.

24 minutes5 theory cards
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Understanding step by step

One device works normally, but after several are connected the same wire becomes hot. Why does current affect the released energy more strongly than a simple doubling might suggest?

Small currentTwice the currentless energymore energySame R and tHeating rises faster than current
Identical conductors with unchanged resistance are compared over the same time. Doubling current releases more energy; blue arrow lengths are in the ratio 1:2. Red waves symbolise heat generation, not a temperature scale.

Why a wire heats up

The field does work on moving charges; they interact with the conductor's material and transfer energy to it. In a resistive section, electrical energy becomes internal energy: this is Joule heating. The released energy Q is measured in joules. It may stay in the conductor or leave for the surroundings. A heating element can therefore keep releasing energy even after its temperature stops rising.

Energy transfer in an interactione⁻Electrical energy→ conductor's internal energy
Electrons and particles of the conductor are shown schematically. Electrons interact with the material; the field's energy becomes the conductor's internal energy. Blue shows an electron's motion; red shows energy transfer to the material. The electron does not disappear during the interaction.

Joule–Lenz law

A resistor converts electrical power UI into heating. Substitute U = IR: over time t, the Joule–Lenz law gives Q = I²Rt for constant I and R. Units А²·Ом·с give joules. The square arises because increasing current at the same R also requires more voltage. At zero current, Joule heating is zero; twice the time gives twice the energy. Q is energy, not a number of degrees.

Q = I² · R · tFor constant I and RIamperesRohmstsecondsthe result is joulesreleased energy,not temperature
For constant I and R, multiply current squared by resistance and time. Units: А²·Ом·с = Дж. This is released energy; temperature change also depends on mass, heat capacity and heat exchange with the surroundings.

Why large current is dangerous

Double the current in one wire while keeping resistance and time unchanged. The formula contains (2I)² = 4I², so four times the energy is released. Increasing the load on shared wiring can therefore quickly increase heating. Keep comparison conditions clear: at fixed current, greater R gives more Q; at fixed voltage, current changes and Q = U²t/R. Resistances cannot be compared without stating what the source maintains.

Same R and time tRIQR2I4QSame R and t: Q ∝ I²Energy is released in the resistance
The comparison uses identical unchanged R and equal time t. Blue arrows show I and 2I; red arrows show energy transfer; rectangles on the right show Q and 4Q with areas in the ratio 1:4. Q = I²Rt determines released energy, not temperature.

What sets the temperature

Does four times Q mean four times the temperature? No: there is an initial temperature, and its change depends on mass and heat capacity. For an ideal thermally insulated conductor without a phase change, ΔT = Q/(cm). Real wire also transfers energy to air and supports. Temperature can become constant when release balances losses. If R changes during heating, one constant R cannot be used over the whole interval either.

Same Q, c and initial TQQm2mΔTΔT/2Same energy, different massHeat losses ignored here
Two objects of the same material receive equal Q. Initial temperatures and specific heat capacities are equal; heat losses and phase changes are ignored. A mass 2m has half the temperature rise of m: ΔT = Q/(cm). Cooling by the surroundings also affects a real wire.

Short circuit

A short circuit creates an unintended very low-resistance path between circuit points at different potentials, for example bypassing a load. Total current rises sharply; real resistance in the source, contacts and wires prevents it from becoming infinite. These parts release energy and may overheat. Low resistance in the shorting path therefore does not mean no dangerous heating elsewhere: the current has changed greatly.

+−rdeviceLarge IShort circuitr — sourceand wiresBefore protection trips
Damage creates the red low-resistance path in parallel with the device, increasing total current. Source and wire resistances are grouped schematically as r; they limit current so it is not infinite. The diagram shows the moment before protection disconnects the circuit. Never build this fault circuit as a school experiment.

Overload protection

A fuse or circuit breaker is selected to suit the wiring's current rating. Excess current makes it open the circuit, limiting the duration of energy release and reducing overheating risk. But a current dangerous to a person may be below its trip threshold. A normal breaker therefore mainly protects wiring; it does not guarantee protection when someone touches a live part. Never change its rating yourself just to stop it tripping.

After the breaker trips+−BreakerLoadI = 0Protect wiring from overload
The circuit after a correctly selected breaker trips: contacts inside its case are open and current has stopped everywhere. The breaker protects wiring against excess current. Its presence does not guarantee protection from every electric shock.

Safe behaviour

Damaged insulation may allow current to pass through a person; wet hands often lower contact resistance. Do not touch bare wires or damaged devices, or handle electrical appliances with wet hands. If you find damage, stop using the device and tell an adult. School experiments use a purpose-designed low-voltage source and a checked circuit. Understanding heating explains the rules; it does not make dangerous contact an acceptable experiment.

Three things to avoidbarewirewethandsdamageddeviceDamage? Tell an adult
Do not touch bare wires or damaged devices, or handle them with wet hands. If a device is damaged, stop using it and tell an adult.

Different protective devices

Protection has different roles. Insulation prevents contact with a conductor. Protective earthing provides an intended fault-current path and helps disconnection after a fault. A residual-current device detects a difference between outgoing and returning currents, which may indicate leakage. These measures reduce particular risks, but do not permit touching live parts. Specialists check their condition and correct use.

Different protective rolesInsulationBarrierto contactEarthingCurrent pathduring a faultRCDLeakage →disconnectionDo not touch live parts
Insulation prevents contact with live parts. Protective earthing provides a fault-current path after insulation damage and works with disconnecting devices. A residual-current device (RCD) responds to outgoing/returning current imbalance caused by leakage; a standard RCD does not replace overload protection. No protection permits touching live parts.

Resistor heating

A constant 2 A flows through a 5 ohm resistor for 60 s. Find the energy released.

+−R = 5 ОмI = 2 Аt = 60 сQ — ?Energy released in the resistor
A constant current I = 2 А flows through R = 5 Ом for t = 60 с. The red arrow shows current from source positive to negative through the external circuit. Find the energy Q released in the resistor.

Worked example · 1

We need the resistor's released energy; current and resistance are constant. Use Q = I²Rt.

+−R = 5 ОмI = 2 Аt = 60 сI and R constant for all 60 сQ = I² · R · t
Treat the current of 2 A and resistance of 5 ohms as constant throughout the 60 s. We can therefore calculate released energy directly with Q = I²Rt. These conditions belong to the chosen resistor and current model.

Worked example · 2

The current is squared: 2² = 4. Thus Q = 4·5·60 = 1200 Дж. The release rate is 20 W; over 60 s this gives the same 1200 J.

+−R = 5 ОмI = 2 Аt = 60 сQ = (2 А)² · 5 Ом · 60 сQ = 1200 Дж
For the same resistor and interval, first square the current: (2 А)² = 4 А². Then Q = 4 А² · 5 Ом · 60 с = 1200 Дж. Resistance, current and duration stay unchanged throughout the calculation.

Worked example · 3

This is not a temperature answer. For temperature, we need mass, heat capacity, initial temperature and energy exchange with the surroundings.

+−R = 5 ОмI = 2 Аt = 60 сQ = 1200 Дж — energyFor temperature change we needmass, heat capacity and losses
The same resistor releases 1200 J. To find its temperature rise, we need mass, specific heat capacity and information about cooling and possible phase changes. Final temperature also requires initial temperature. Q alone does not determine temperature.

Check the result

1200 J. Each second, 20 J was released; some may have transferred to surrounding objects.

Key idea · 1

Q = I²Rt explains quadratic growth in released energy as current rises with R and t unchanged.

Key idea · 2

Temperature also depends on energy accumulation and removal; a short circuit changes current throughout the real circuit.

Key idea · 3

Different protective devices serve different purposes; touching live parts remains unacceptable.

What comes next

Current not only heats a conductor: it creates a magnetic field. We will study its effects next.

Basic Concepts

3 concepts

Joule-Lenz law

The energy released by the current in the resistance during time t is equal to Q = I²Rt, if the current I and resistance R are constant.

At the same R and t, doubling the current quadruples the released energy. Temperature also depends on mass, heat capacity, and cooling; its growth does not have to be fourfold. Some of the energy can be transferred to surrounding bodies.

Short circuit

An unintended very low-resistance path between circuit points with a voltage difference; it may cause excessive current.

The actual current is limited by the resistance of the source, wires and contacts. A properly selected and functioning fuse or circuit breaker will cut off excessive current, reducing the risk of wiring overheating. Such a device does not guarantee human protection upon any touch.

Electrical safety

Safe operation requires proper insulation, grounding, protective devices and no contact with live parts.

Wet skin conducts better, so electrical appliances should not be used with wet hands or near water without protection.

Physical quantities

1 magnitude

Energy released by current

Q

The energy released when current passes through a resistance; it can remain in the conductor or be transmitted to the environment.

Unit: joule · \mathrm{Дж}

Lesson formulas

1 formula

Joule-Lenz law

Q = I^2Rt

The energy released by the current in the resistance is equal to the square of the current multiplied by the resistance and time.

Conditions: I and R are constant over time t. The released energy does not necessarily remain entirely in the conductor: some may escape into the environment; The temperature is determined by a separate heat balance.

Related formulas

The same formulas in the reference, with symbols and units.

Problems on this topic

Statements, answer options and the walkthrough.