RuukkilabraUpper secondary physics
FY6 · Chapter 15

Electrical safety at home and at work

Why does the kitchen fuse trip when many devices are on at the same time, even though none of them is broken?

Prior knowledge

  • Electric power is $P = UI$, and a conductor produces thermal power $P = RI^2$chapter Electric power and the heating of a resistor
  • In a parallel connection every branch has the same voltage and the currents of the branches add upchapter Resistors in series and in parallel
  • An insulator withstands an electric field only up to its dielectric strengthchapter The capacitor and its energy

Core path: follow the steps in order. Tasks marked Optional give extra practice. Optional tasks: 3.

Think about it

On a Saturday morning in the kitchen, coffee is brewing, the kettle is boiling water for tea, the toaster is on and porridge is heating in the microwave oven. After a moment the kitchen goes dark: one circuit breaker in the fuse board has tripped. No device is broken.

Why did the circuit breaker trip, and does the same fuse also protect a person from electric shock?

Optional Recall: the current of a device
The power of a kettle is $2000\,\text{W}$, and it is plugged into a $230\,\text{V}$ socket. How large a current does the kettle draw?

Predict

Make your predictions before investigating 2 questions

Prediction 1: fuse or residual current device?

A person touches the live frame of a faulty device, and a current of $0.1\,\text{A}$ flows through them to the ground. The circuit has a $10\,\text{A}$ fuse and a $30\,\text{mA}$ residual current device (RCD).What cuts off the current?

Prediction 2: a bird on a conductor

A bird sits on a bare $20\,\text{kV}$ conductor and does not get an electric shock. Which explanation is correct?

Investigate

Which devices fit in the same circuit?

Made-up example data · Invented example data: typical powers of home appliances, not a measurement.

The sockets of a kitchen are on the same circuit, which is protected by a $10\,\text{A}$ fuse. The mains voltage is $230\,\text{V}$, and the devices are connected in parallel.

device $P$
kettle $2000\,\text{W}$
coffee maker $1000\,\text{W}$
microwave oven (input power) $1200\,\text{W}$
toaster $900\,\text{W}$
refrigerator $100\,\text{W}$

Calculate the current of each device, $I = P : U$. Then find which combinations of two devices fit in the circuit without exceeding the rated current of the fuse, and how large a current would flow if all the devices were on at the same time.

How large a current flows in the circuit cable when the kettle and the microwave oven are on at the same time?

A
Hint 1: a guiding question

The devices are in parallel. How do the currents of devices in parallel combine in the circuit cable?

Hint 2: what is the connection

The current in the circuit cable is the sum of the currents of the devices, that is, the total power divided by the voltage.

Hint 3: an intermediate step

$I = (2000\,\text{W} + 1200\,\text{W}) : 230\,\text{V}$.

Show the solution

Given

power of the kettle $P_1 = 2000\,\text{W}$, input power of the microwave oven $P_2 = 1200\,\text{W}$, voltage $U = 230\,\text{V}$

Find

the current $I$ in the circuit cable in amperes

Principle

The devices are connected in parallel, so the voltage across each is $230\,\text{V}$ and their currents add up in the circuit cable. The total current is therefore obtained from the total power of the devices.

Formula

$I = \dfrac{P_1 + P_2}{U}$

Conversions

None needed: $1\,\text{W} : 1\,\text{V} = 1\,\text{A}$.

Substitution

$I$$= \dfrac{2000\,\text{W} + 1200\,\text{W}}{230\,\text{V}}$
$= \dfrac{3200\,\text{W}}{230\,\text{V}}$
$= 13.91\,\text{A}$

Answer

$14\,\text{A}$

Two significant figures like the power $1200\,\text{W}$. The current is larger than the rated current of the fuse, $10\,\text{A}$, so the circuit is overloaded.

Reasonableness

The currents of the devices are $8.7\,\text{A}$ and $5.2\,\text{A}$, and their sum is the same $13.9\,\text{A}$. Each device fits in the circuit alone, but not together. All five devices together would draw $5200\,\text{W} : 230\,\text{V} \approx 23\,\text{A}$.

Dry or wet skin?

Made-up example data · Invented example data: the resistances of the current path are indicative orders of magnitude. The effect limits are approximate values for the effects of current described in the standard IEC 60479-1.

A person touches the frame of a faulty device whose voltage relative to the ground is $230\,\text{V}$. A current flows from the hand through the body to the feet and the ground. The table gives the resistance of the whole current path in three situations. The first row holds only if the shoes and the floor are dry and undamaged and the person does not touch anything earthed at the same time, such as a tap.

situation $R$
dry hands, rubber-soled shoes, dry floor $200\,\text{k}\Omega$
dry hands, bare feet on a dry floor $20\,\text{k}\Omega$
wet hands, bare feet on a wet floor $1.0\,\text{k}\Omega$

Calculate the current through the body in each situation, in milliamperes. Compare the currents with the approximate effect limits: a current of about $0.5\,\text{mA}$ can be felt, with about $10\,\text{mA}$ you may not be able to let go, and from about $50\,\text{mA}$ upward the danger of ventricular fibrillation of the heart increases.

How large a current flows through the body in wet conditions? Answer in milliamperes.

mA
Hint 1: a guiding question

The body is part of the circuit. Which law gives the current when the voltage and the resistance are known?

Hint 2: what is the connection

$I = U : R$ when the resistance is in ohms: $1.0\,\text{k}\Omega = 1000\,\Omega$.

Hint 3: an intermediate step

$I = 230\,\text{V} : 1000\,\Omega$, and $1\,\text{A} = 1000\,\text{mA}$.

Show the solution

Given

touch voltage $U = 230\,\text{V}$, resistance of the current path in wet conditions $R = 1.0\,\text{k}\Omega$

Find

the current $I$ through the body in milliamperes

Principle

The body is part of the circuit between the frame of the device and the ground, so the current through it is obtained from Ohm's law with the resistance of the whole current path.

Formula

$U = RI$, so $I = \dfrac{U}{R}$

Conversions

$R$$= 1.0\,\text{k}\Omega$
$= 1.0 \cdot 1000\,\Omega$
$= 1000\,\Omega$

$1\,\text{A} = 1000\,\text{mA}$.

Substitution

$I$$= \dfrac{230\,\text{V}}{1000\,\Omega}$
$= 0.23\,\text{A}$
$= 230\,\text{mA}$

Answer

$230\,\text{mA}$

Two significant figures like the resistance $1.0\,\text{k}\Omega$.

Reasonableness

The current is more than four times the limit for the danger of ventricular fibrillation, $50\,\text{mA}$. With rubber-soled shoes the current would be $230\,\text{V} : 200\,\text{k}\Omega = 1.15\,\text{mA}$ and with bare feet on a dry floor $11.5\,\text{mA}$; in wet conditions the resistance becomes $200$ times smaller, so the current grows $200$-fold. Shoes reduce the current like this only if they are undamaged and dry, the floor is dry and the person does not touch a tap or an earthed device at the same time; otherwise the current bypasses the shoes, and shoes must not be relied on as protection.

Conclusion: what protects the cable, what protects a person?

Write, on the basis of the calculations in the tables: why does the fuse trip even though no device is broken, and why does the same fuse not protect a person? Why does wet skin make an electric shock more dangerous?

Theory summary

Key idea

A fuse protects the cable from overheating

The electricity of a home is divided into circuits in the fuse board. Each circuit has its own circuit cable and its own fuse, usually $10\,\text{A}$ or $16\,\text{A}$. The sockets and lights of one circuit are connected in parallel, so the voltage across each device is $230\,\text{V}$ and the currents of the devices add up in the circuit cable (chapter Resistors in series and in parallel). The fuse is at the start of the circuit cable, so the current of the whole circuit flows through it. A single device can be in working order, but many devices together exceed the rated current of the fuse.

$230\,\text{V}$
$\text{fuse}$
$I$
$P_1$
$I_1$
$P_2$
$I_2$
$P_3$
$I_3$
$I = I_1 + I_2 + I_3$

The conductors of the circuit cable have a small resistance, and they produce thermal power $P = RI^2$ (chapter Electric power and the heating of a resistor): when the current doubles, the thermal power of the cable becomes four times as large. The size of the fuse is chosen according to the cable: the cable determines how large a current the fuse may let through. If the current is larger for a long time, the cable and its connections heat up, the insulation is damaged and a fire can start. The fuse cuts off the current before that happens. A small overload can continue for a long time, but the larger the overcurrent, the faster the fuse acts; in a short circuit the current is cut off in a fraction of a second. In a screw-in fuse a thin wire melts from its own heating, whereas a circuit breaker trips and is switched back on. A blown fuse is never replaced with a larger one.

Earthing leads the fault current away from the person

The two holes of a socket take the line conductor L and the neutral conductor N. An earthed socket also has protective earth contacts PE, which are connected to the ground with a yellow-green protective earth conductor. The colours of the insulation of the conductors are well established in Finland: in new installations the line conductor is usually brown, the neutral conductor blue and the protective earth conductor yellow-green. In old installations the colours may differ, and you must never conclude from the colour of a conductor that it is not live.

$\text{socket}$
$\text{PE}$
$\text{PE}$
$\text{cable}$
$\text{line}\ \text{L}$
$\text{neutral}\ \text{N}$
$\text{earthing}\ \text{PE}$

The conductive metal frame of a washing machine or a kettle is connected to protective earth through the plug. If the insulation of the line conductor wears and the conductor touches the frame, a large fault current flows along the protective earth conductor, and the fuse cuts off the current quickly. Without earthing, the frame would stay live, and a current would flow to the ground through a person touching the frame. For this reason the earth contact must not be bypassed, and an earthed plug must not be connected to a socket without earthing by means of an extension cord or an adapter.

$\text{no earthing}$
$\text{protectively earthed}$
$\text{fault}$
$I$
$\text{fault}$
$I_\text{E}$
$\text{current through the person}$
$\text{the fuse trips}$

Protection classes tell how a device protects the user

The rating plate of a device has the sign of its protection class. A protection class I device has a conductive frame that is protectively earthed, and its plug has earth contacts. A protection class II device has no earthing: the live parts are separated from the user by double or reinforced insulation, and the plug is often flat. A protection class III device works at a protective extra-low voltage, at most $50\,\text{V}$ alternating voltage or $120\,\text{V}$ direct voltage, which comes from a safety transformer or a battery. In ordinary conditions, touching it does not cause a dangerous current.

$\text{class I}$
$\text{earthing}$
$\text{washing machine}$
$\text{class II}$
$\text{double insulation}$
$\text{hair dryer}$
$\text{class III}$
$\text{extra-low voltage}$
$\text{cordless drill}$

The residual current device protects a person

A fuse does not notice a current through a person: its rated current is amperes, but a current of just tens of milliamperes through the body can be life-threatening. A fuse protects a person only together with protective earthing, when a fault causes an earth fault. The small current through a person is cut off by a residual current device (RCD). It compares the current going to the device in the line conductor with the current returning in the neutral conductor. In an intact circuit they are equal. If part of the current gets to the ground through a fault, for example through a person, the returning current is smaller. When the difference exceeds the tripping current, usually $30\,\text{mA}$, the device cuts off the current in a fraction of a second. In new installations the socket circuits are protected with an RCD, and its test button should be pressed regularly.

$230\,\text{V}$
$\text{L}$
$\text{N}$
$\text{residual current device}$
$\text{fuse}$
$I_\text{L}$
$I_\text{N}$
$\text{device}$
$R_\text{body}$
$I_\text{E}$
$I_\text{L} - I_\text{N} = I_\text{E}$
A white four-pole residual current device on a black background: a yellow TEST button, a black lever and screw terminals along the top and bottom; its side is marked with the voltage, the tripping current and the rated current.
A residual current device. The marking $I_{\Delta n} = 0.03\,\text{A}$ means that it cuts the current when the currents in the phase and neutral conductors differ by $30\,\text{mA}$. The yellow TEST button is used to check regularly that the device works. Photo: Raimond Spekking, CC BY-SA 4.0

An RCD does not prevent all shocks. If a person touches the line conductor and the neutral conductor at the same time, the current returns along the neutral conductor, and there is no difference between the currents of the line and neutral conductors. For this reason live parts are never touched, even if the circuit has an RCD.

The dielectric strength of an insulator

The plastic sheath of cables, the body of a plug and the insulators of high-voltage lines separate the live parts from people. Every insulator, however, withstands only an electric field of a certain size. When the field exceeds the dielectric strength of the insulator, the insulator starts to conduct and a spark discharges through it (chapter The capacitor and its energy). In a uniform field, an insulating layer of thickness $d$ withstands a voltage $E_\text{max} d$. A larger voltage therefore needs a thicker insulator or a longer air gap, and the insulator must be intact: a crack, moisture or dirt weakens the insulation.

High-voltage lines and step voltage

Electricity is transmitted from power plants at a high voltage, in the national grid as much as $400\,\text{kV}$, because for the same power a high voltage means a small current and thus small thermal losses $RI^2$ in the lines. High-voltage conductors are bare, and they are insulated by the surrounding air. The dielectric strength of air is about $3\,\text{MV/m}$, so you do not need to touch a conductor to get a shock: an electric arc can jump from the conductor to an object brought near it, such as the boom of a crane, a fishing rod or the string of a kite. The voltage of the overhead line of trains is $25\,\text{kV}$, so you must not climb on the roof of the carriages.

A bird can sit on a bare conductor because both its feet are at the same potential: there is no voltage between the feet, and no current flows through the bird. The danger arises when a body connects two points at different potentials, for example a conductor and the ground.

If a conductor falls to the ground, the current spreads into the ground. The potential of the ground is greatest at the point of contact and decreases with distance, so there is a voltage between different points. The voltage between a person's feet is called the step voltage: it is the larger, the closer to the point of contact you are and the longer your step is. You move away from a fallen conductor with short steps, feet together, or by hopping with both feet together; you do not approach the conductor, and you report the damage to the emergency number $112$.

$U_\text{step}$
$U \approx 0$
$\text{potential decreases}$
A yellow triangular warning sign with a black border and a black lightning arrow, on a white surface.
The lightning-arrow sign warns of dangerous voltage. It is found, for example, on the cover of a fuse box: behind the cover are live parts that must not be touched. Photo: Pittigrilli, CC BY 4.0

Safe action at home and at work

In Finland, electrical installation work may be done only by electrical professionals, and the company doing the work must be in the register of the Finnish Safety and Chemicals Agency Tukes as an electrical contractor. A layperson may do only simple jobs: for example, replace a fuse and a lamp, reset a tripped circuit breaker or residual current device (RCD), repair an extension cord or replace its plug, and connect a light fitting in a dry space with a lighting connector. An up-to-date list of the electrical work allowed for laypersons is on the website of Tukes. Before work, the current is switched off and you make sure that there is no voltage at the site.

At workplaces such as building sites, extension cords and devices are inspected, in damp places an RCD or a protective extra-low voltage is used, and a damaged device is taken out of use. If a device smells of burning, gets hotter than usual or gives small electric shocks, its plug is pulled out and the device is taken for repair. If someone is stuck to a live part, the current is switched off first, before the person is touched, and the emergency number $112$ is called.

Current of a circuit and touch current

The devices of a circuit are in parallel at the same voltage, so the current of each device is $I_k = P_k : U$, and the sum of them flows in the circuit cable and the fuse:

$$I = \frac{P_1 + P_2 + P_3 + \dots}{U}$$

where $I$ is the total current of the circuit cable ($\text{A}$), $P_1, P_2, \dots$ are the powers of the devices that are on at the same time ($\text{W}$) and $U$ is the mains voltage $230\,\text{V}$. The mains voltage is the rms value of the alternating voltage, so the power of a heating device is calculated with it as with a direct voltage. The circuit is not overloaded when $I$ is at most the rated current of the fuse $I_\text{f}$. The total power of the devices may therefore be at most $230\,\text{V} \cdot 10\,\text{A} = 2300\,\text{W}$ in a $10\,\text{A}$ circuit and $230\,\text{V} \cdot 16\,\text{A} = 3680\,\text{W}$ in a $16\,\text{A}$ circuit.

The current through the body

When a person touches a live part and the ground at the same time, their body is part of the circuit. The current through the body is obtained from Ohm's law (chapter Resistance and Ohm's law):

$$I = \frac{U}{R}$$

where $I$ is the current through the body ($\text{A}$), $U$ is the touch voltage, that is, the voltage between the points of contact ($\text{V}$), and $R$ is the resistance of the whole current path ($\Omega$): the resistances of the skin, the inside of the body, and the shoes and the floor, in series.

The resistance of the body is not constant. Most of it is in the skin, and it depends on the moisture of the skin, the size of the contact area, the path of the current and the voltage. With dry skin and insulating shoes, the resistance of the current path can be hundreds of kilohms. Wet or sweaty skin, a large contact area and bare feet on a wet floor reduce it to about a kilohm, and then a touch voltage of $230\,\text{V}$ gives a current of $230\,\text{V} : 1\,\text{k}\Omega \approx 230\,\text{mA}$. The resistance of the inside of the body is only of the order of hundreds of ohms.

Shoes reduce the current only if they are undamaged and dry, the floor is dry and the person does not touch anything else earthed at the same time, such as a tap or an earthed device: then the current flows past the shoes. Shoes must not be regarded as equipment that protects against electric shock.

$I$ (approx.) effect
$0.5\,\text{mA}$ the current can be felt
$10\,\text{mA}$ the grip does not release
$30\,\text{mA}$ breathing becomes difficult
over $50\,\text{mA}$ danger of ventricular fibrillation

About $0.5\,\text{mA}$ is the threshold of perception. A current of about $10\,\text{mA}$ cramps the muscles so that you may not be able to let go: this is the let-go threshold. A current of over $50\,\text{mA}$ can cause ventricular fibrillation of the heart if it lasts about a second; a shorter shock needs a larger current.

The table applies to the $50\,\text{Hz}$ alternating current of a home. The usual tripping current of an RCD, $30\,\text{mA}$, has been chosen so that the device usually cuts off the current before it has time to cause ventricular fibrillation. The values are indicative, and they are based on the effects of current on an adult described in the international standard IEC 60479-1. The effect also depends on the duration and path of the current and on the person, and no current can be regarded as certainly safe.

$I\ (\text{mA})$
$0.1$
$1$
$10$
$100$
$1000$
$0.5\,\text{mA}\ \ \text{the current can be felt}$
$10\,\text{mA}\ \ \text{the grip does not release}$
$30\,\text{mA}\ \ \text{breathing becomes difficult}$
$50\,\text{mA}\ \ \text{danger of fibrillation}$

Common misconception

Many people think that a fuse protects a person from electric shock. A fuse protects the cables: its rated current is $10\,\text{A}$ or $16\,\text{A}$, whereas a current of only about $50\,\text{mA}$ through the body can cause ventricular fibrillation of the heart. A fuse does not notice so small a current through a person at all. It protects a person only together with protective earthing: in an earth fault, protective earthing leads a large fault current along the conductor, and the fuse cuts it off. The small current through a person is cut off by the residual current device (RCD), which trips at a fault current of about $30\,\text{mA}$.

Another mistake is to think that a large voltage alone is dangerous or that a small voltage is always safe. The harm is done by the current through the body, which depends on both the voltage and the resistance of the current path. A bird sits safe on a $20\,\text{kV}$ conductor because there is no voltage between its feet, but wet skin can make even a smaller voltage dangerous.

Summary

  • The devices of one circuit are in parallel, so the current through the fuse is their total current $I = (P_1 + P_2 + \dots) : U$. A fuse protects the cable from overheating, because the thermal power of the cable is $RI^2$.
  • Protective earthing leads the fault current along the yellow-green conductor to the ground, and then the fuse cuts off the current. The protection classes are I (earthing), II (double insulation) and III (protective extra-low voltage).
  • A residual current device (RCD) compares the currents of the line and neutral conductors and cuts off the current when the difference exceeds about $30\,\text{mA}$.
  • The current through the body is $I = U : R$. Wet skin reduces the resistance, and a current of just tens of milliamperes can be life-threatening.
  • An insulator withstands a field only up to its dielectric strength; from a high-voltage line an electric arc can jump through the air without contact. Near a conductor that has fallen to the ground, the step voltage is dangerous.
  • In Finland, electrical installation work belongs to professionals; a layperson may do only simple jobs, such as replacing a fuse or repairing an extension cord.
Optional Return to your predictions

Compare your predictions with the theory and the currents you calculated. Then return to the opening question: why did the kitchen circuit breaker trip, and what protects a person?

    Would you change your prediction?

    Apply

    Worked example

    Problem

    A kitchen socket circuit is protected by a $16\,\text{A}$ fuse. In the morning a kettle ($2.2\,\text{kW}$), a coffee maker ($1.0\,\text{kW}$) and a microwave oven with an input power of $1.3\,\text{kW}$ are on at the same time. How large a current flows in the circuit cable, and is the rated current of the fuse exceeded?

    Step 1/7

    Given and asked. $P_1 = 2.2\,\text{kW}$, $P_2 = 1.0\,\text{kW}$, $P_3 = 1.3\,\text{kW}$, $U = 230\,\text{V}$, rated current of the fuse $I_\text{f} = 16\,\text{A}$. We are asked for the current $I$ in the circuit cable and whether $I > I_\text{f}$.

    Step 2/7

    Principle. The devices are connected in parallel on the same circuit, so the voltage across each is $230\,\text{V}$ and their currents add up in the circuit cable and the fuse. The total current is therefore calculated from the total power of the devices.

    Step 3/7

    Formula solved.

    $$I = \frac{P_1 + P_2 + P_3}{U}$$

    Step 4/7

    Unit conversions.

    $P_1 + P_2 + P_3$$= 2.2\,\text{kW} + 1.0\,\text{kW} + 1.3\,\text{kW}$
    $= 4.5\,\text{kW}$
    $= 4.5 \cdot 1000\,\text{W}$
    $= 4500\,\text{W}$

    Step 5/7

    Substitution. $$\begin{aligned} I &= \frac{P_1 + P_2 + P_3}{U} \\ &= \frac{4500\,\text{W}}{230\,\text{V}} \\ &= 19.6\,\text{A} \end{aligned}$$

    Step 6/7

    Result. A current of about $20\,\text{A}$ flows in the circuit cable, two significant figures like the powers. It is larger than the rated current of the fuse, $16\,\text{A}$, so the circuit is overloaded. Such a small overcurrent does not cut off the current at once, but the fuse trips if the load continues long enough. It is worth using the devices in turn.

    Step 7/7

    Reasonableness. The currents of the devices are $9.6\,\text{A}$, $4.3\,\text{A}$ and $5.7\,\text{A}$, and their sum is the same $19.6\,\text{A}$. The estimate $4500\,\text{W} : 200\,\text{V} \approx 22\,\text{A}$ is slightly larger, because the divisor is smaller. No single device exceeds $16\,\text{A}$ alone; only the common current does.

    Find the error

    A student checks whether a kettle ($2000\,\text{W}$) and a toaster ($900\,\text{W}$) can be used at the same time in a $10\,\text{A}$ circuit:

    $$\begin{aligned} I_1 &= \frac{2000\,\text{W}}{230\,\text{V}} \approx 8.7\,\text{A} \\ I_2 &= \frac{900\,\text{W}}{230\,\text{V}} \approx 3.9\,\text{A} \end{aligned}$$

    “Each current is below $10\,\text{A}$, so the devices can be on at the same time.” Where is the error?

    Apply to a new situation

    On a building site, a site heater ($2.0\,\text{kW}$) and an angle grinder ($1.4\,\text{kW}$) are connected to a $16\,\text{A}$ circuit through the same extension cord. The total resistance of the two conductors of the extension cord is $0.60\,\Omega$. Assume that the currents of the devices are the same as when they are connected directly to a $230\,\text{V}$ socket.

    How large a thermal power is produced in the extension cord?

    W
    Hint 1: a guiding question

    The current of both devices flows through the extension cord. How large is it?

    Hint 2: what is the connection

    $I = (2000\,\text{W} + 1400\,\text{W}) : 230\,\text{V}$. The thermal power produced in the cord depends on the resistance of the cord and the current.

    Hint 3: an intermediate step
    $P$$= RI^2$
    $= 0.60\,\Omega \cdot (14.8\,\text{A})^2$
    Show the solution

    Given

    powers $P_1 = 2.0\,\text{kW}$ and $P_2 = 1.4\,\text{kW}$, voltage $U = 230\,\text{V}$, resistance of the extension cord $R = 0.60\,\Omega$

    Find

    the thermal power $P_\text{c}$ produced in the extension cord

    Principle

    The devices are in parallel at the end of the extension cord, so the sum of their currents flows through the cord, and it is obtained from the total power. In the resistance of the cord, electrical energy is transformed into internal energy at the rate $RI^2$. By the assumption, the small voltage drop in the cord does not change the currents of the devices.

    Formula

    $I = \dfrac{P_1 + P_2}{U}$ and $P_\text{c} = RI^2$, so

    $P_\text{c}$$= R\left(\dfrac{P_1 + P_2}{U}\right)^2$

    Conversions

    $P_1 + P_2$$= 2.0\,\text{kW} + 1.4\,\text{kW}$
    $= 3.4\,\text{kW}$
    $= 3.4 \cdot 1000\,\text{W}$
    $= 3400\,\text{W}$

    Substitution

    $I$$= \dfrac{3400\,\text{W}}{230\,\text{V}}$
    $= 14.78\,\text{A}$
    $P_\text{c}$$= 0.60\,\Omega \cdot (14.78\,\text{A})^2$
    $= 131.1\,\text{W}$

    Answer

    $130\,\text{W}$

    Two significant figures like the resistance $0.60\,\Omega$ and the powers.

    Reasonableness

    The current $14.8\,\text{A}$ is below $16\,\text{A}$, so the fuse does not trip, but the cord heats with a power of $130\,\text{W}$. The voltage across the cord is $0.60\,\Omega \cdot 14.8\,\text{A} \approx 8.9\,\text{V}$, small compared with $230\,\text{V}$, so the assumption holds. Wound on a reel, a cord cannot cool, so on a building site the cord is unwound from the reel completely.

    Check your understanding

    Exit ticket

    Answer on your own first and only then open the answer.

    1. A blown $10\,\text{A}$ fuse is replaced with a $16\,\text{A}$ fuse. Why is that dangerous even though the electricity works?
      Answer

      The circuit cable is dimensioned for a current of $10\,\text{A}$. A larger fuse lets through a current of up to $16\,\text{A}$, and then the thermal power of the conductors, $P = RI^2$, is $(16 : 10)^2 \approx 2.6$ times as large. The cable and the connections can overheat, the insulation can be damaged and a fire can start.

    2. May a layperson install a new socket in a wall in Finland? Name two electrical jobs that a layperson may do themselves.
      Answer

      No: electrical installation work belongs to electrical professionals. A layperson may, for example, replace a fuse and a lamp, reset a tripped circuit breaker or residual current device (RCD) and repair an extension cord. An up-to-date list is on the website of Tukes.

    1. Step voltage

    A high-voltage conductor has fallen to the ground in a storm. Why do you move away from it with short steps, feet together?

    Suggestion: one answer does not show everything you can do, but review the theory summary and do the core exercises.

    2. The sign of a protection class

    The rating plate of a hair dryer has a sign that tells that the device has double or reinforced insulation and is not earthed.Which sign is it?

    Suggestion: one answer does not show everything you can do, but review the theory summary and do the core exercises.

    Optional 3. Explain protective earthing

    Inside a washing machine the insulation of the line conductor has worn, and the conductor touches the metal frame of the machine. Explain how protective earthing and the fuse protect a person who touches the machine.

    Why is earthing not needed in a protection class II device?

    Exercises

    Level 1 · basic practice 5 exercises

    One formula or one step of reasoning. Core exercises first, the rest is extra practice.

    1. Exercise 15-1Core

      The heating power of a fan heater is $1500\,\text{W}$, and it is plugged into a $230\,\text{V}$ socket. How large a current does the heater draw?

      A
      Answer

      $6.5\,\text{A}$

      Show the solution

      Given

      power $P = 1500\,\text{W}$, voltage $U = 230\,\text{V}$

      Find

      the current $I$ in amperes

      Principle

      Electric power is voltage times current. The mains voltage $230\,\text{V}$ is the rms value of the alternating voltage, so the power of a heating device is calculated with it as with a direct voltage.

      Formula

      $P = UI$, so $I = \dfrac{P}{U}$

      Conversions

      None needed: $1\,\text{W} : 1\,\text{V} = 1\,\text{A}$.

      Substitution

      $I$$= \dfrac{1500\,\text{W}}{230\,\text{V}}$
      $= 6.522\,\text{A}$

      Answer

      $6.5\,\text{A}$

      Two significant figures like the power $1500\,\text{W}$.

      Reasonableness

      The estimate $1500\,\text{W} : 200\,\text{V} = 7.5\,\text{A}$ is slightly larger, because the divisor is smaller. The current is below $10\,\text{A}$, so the heater fits alone in a $10\,\text{A}$ circuit, but there is not much room left for anything else on the same circuit.

    2. Exercise 15-2Core

      The circuit cable of a home is protected by a $10\,\text{A}$ fuse, and the mains voltage is $230\,\text{V}$.

      How large may the total power of the devices on the circuit be at most so that the rated current of the fuse is not exceeded? Answer in watts.

      W
      Answer

      $2300\,\text{W}$

      Show the solution

      Given

      rated current of the fuse $I_\text{f} = 10\,\text{A}$, voltage $U = 230\,\text{V}$

      Find

      the greatest total power $P_\text{max}$ in watts

      Principle

      The devices of the circuit are in parallel at the same voltage, so their currents add up and the current in the circuit cable is the total power divided by the voltage. The rated current is not exceeded when this current is at most $I_\text{f}$.

      Formula

      $I$$= \dfrac{P_1 + P_2 + \dots}{U}$
      $\le I_\text{f}$

      so $P_\text{max} = UI_\text{f}$

      Conversions

      None needed: $1\,\text{V} \cdot 1\,\text{A} = 1\,\text{W}$.

      Substitution

      $P_\text{max}$$= 230\,\text{V} \cdot 10\,\text{A}$
      $= 2300\,\text{W}$

      Answer

      $2300\,\text{W}$

      That is, $2.3\,\text{kW}$, two significant figures like the rated current $10\,\text{A}$.

      Reasonableness

      One $2000\,\text{W}$ kettle fits in the circuit, but the kettle and a $900\,\text{W}$ toaster together do not. This matches the experience that the fuse of an old kitchen trips when too many heating devices are on at the same time.

    3. Exercise 15-3

      A person touches the live frame of a faulty device with wet hands. The touch voltage is $230\,\text{V}$, and the resistance of the whole current path is $2.3\,\text{k}\Omega$.

      How large a current flows through the body? Answer in milliamperes.

      mA
      Answer

      $100\,\text{mA}$

      Show the solution

      Given

      touch voltage $U = 230\,\text{V}$, resistance of the current path $R = 2.3\,\text{k}\Omega$

      Find

      the current $I$ through the body in milliamperes

      Principle

      The body is part of the circuit between the point of contact and the ground, so the current through it is obtained from Ohm's law with the resistance of the whole current path.

      Formula

      $U = RI$, so $I = \dfrac{U}{R}$

      Conversions

      $R$$= 2.3\,\text{k}\Omega$
      $= 2.3 \cdot 1000\,\Omega$
      $= 2300\,\Omega$

      the result from amperes to milliamperes: $1\,\text{A} = 1000\,\text{mA}$.

      Substitution

      $I$$= \dfrac{230\,\text{V}}{2300\,\Omega}$
      $= 0.100\,\text{A}$
      $= 100\,\text{mA}$

      Answer

      $100\,\text{mA}$

      Two significant figures like the resistance $2.3\,\text{k}\Omega$.

      Reasonableness

      The numerical value of the resistance $2300\,\Omega$ is ten times that of the voltage $230\,\text{V}$, so the numerical value of the current in amperes is one tenth, about $0.1\,\text{A}$. The current is twice the limit for the danger of ventricular fibrillation, about $50\,\text{mA}$, so touching with wet hands is life-threatening.

    4. Exercise 15-4

      When a person has dry hands and rubber-soled shoes on a dry floor, the resistance of the whole current path is $50\,\text{k}\Omega$.

      How large a current flows through the body if they touch a part whose voltage relative to the ground is $230\,\text{V}$? Answer in milliamperes.

      mA
      Answer

      $4.6\,\text{mA}$

      Show the solution

      Given

      touch voltage $U = 230\,\text{V}$, resistance of the current path $R = 50\,\text{k}\Omega$

      Find

      the current $I$ through the body in milliamperes

      Principle

      The body, the shoes and the floor are in the same current path, and their combined resistance is given. The current is obtained from Ohm's law.

      Formula

      $U = RI$, so $I = \dfrac{U}{R}$

      Conversions

      $R$$= 50\,\text{k}\Omega$
      $= 50 \cdot 1000\,\Omega$
      $= 50\,000\,\Omega$

      $1\,\text{A} = 1000\,\text{mA}$.

      Substitution

      $I$$= \dfrac{230\,\text{V}}{50\,000\,\Omega}$
      $= 0.0046\,\text{A}$
      $= 4.6\,\text{mA}$

      Answer

      $4.6\,\text{mA}$

      Two significant figures like the resistance $50\,\text{k}\Omega$.

      Reasonableness

      The current is clearly felt, because it is almost ten times the threshold of perception $0.5\,\text{mA}$, but it stays below the let-go threshold $10\,\text{mA}$. With wet hands the resistance can be a tenth or less, and then the current is ten times as large. The result holds only with undamaged, dry shoes and a dry floor, when the person does not touch anything earthed at the same time, such as a tap; otherwise the current bypasses the shoes. Shoes must not be regarded as protection.

    5. Exercise 15-5

      The total resistance of the two conductors of an extension cord is $0.20\,\Omega$, and a current of $16\,\text{A}$ flows in the cord.

      How large a thermal power is produced in the extension cord?

      W
      Answer

      $51\,\text{W}$

      Show the solution

      Given

      resistance of the conductors $R = 0.20\,\Omega$, current $I = 16\,\text{A}$

      Find

      the thermal power $P$ produced in the extension cord

      Principle

      In the resistance of a conductor, electrical energy is transformed into the internal energy of the conductor, which is transferred as heat to the surroundings. When the resistance and the current of the conductor are known, the power is obtained from Joule's law.

      Formula

      $P = RI^2$

      Conversions

      None needed:

      $1\,\Omega \cdot (1\,\text{A})^2$$= 1\,\text{V} \cdot 1\,\text{A}$
      $= 1\,\text{W}$

      Substitution

      $P$$= 0.20\,\Omega \cdot (16\,\text{A})^2$
      $= 0.20\,\Omega \cdot 256\,\text{A}^2$
      $= 51.2\,\text{W}$

      Answer

      $51\,\text{W}$

      Two significant figures like the resistance and the current.

      Reasonableness

      The power is like that of a small incandescent lamp, but it is spread over the whole length of the cord, so an intact cord heats up only a little. If the cord is wound tightly on a reel, little energy is transferred from it as heat to the surroundings, and the cord can become dangerously hot.

    Level 2 · applied practice 4 exercises

    Two steps, working with measured data, a unit conversion or rearranging a formula. Core exercises first, the rest is extra practice.

    1. Exercise 15-6Core

      A kitchen socket circuit is protected by a $16\,\text{A}$ fuse, and the mains voltage is $230\,\text{V}$. A kettle ($2000\,\text{W}$) and a microwave oven with an input power of $1200\,\text{W}$ are on in the circuit.

      How much more power can still be connected to the circuit before the rated current of the fuse is exceeded?

      W
      Answer

      $480\,\text{W}$

      Show the solution

      Given

      rated current $I_\text{f} = 16\,\text{A}$, voltage $U = 230\,\text{V}$, powers that are on $P_1 = 2000\,\text{W}$ and $P_2 = 1200\,\text{W}$

      Find

      the power $P_\text{extra}$ that can still be connected to the circuit

      Principle

      The devices of the circuit are in parallel, so the currents add up and the total current is the total power divided by the voltage. The rated current is not exceeded when the total power is at most $UI_\text{f}$; the extra power left is the difference between this and the power in use.

      Formula

      $\dfrac{P_1 + P_2 + P_\text{extra}}{U}$
      $= I_\text{f}$

      so $P_\text{extra} = UI_\text{f} - (P_1 + P_2)$

      Conversions

      None needed: $1\,\text{V} \cdot 1\,\text{A} = 1\,\text{W}$.

      Substitution

      $P_\text{extra}$$= 230\,\text{V} \cdot 16\,\text{A} - (2000\,\text{W} + 1200\,\text{W})$
      $= 3680\,\text{W} - 3200\,\text{W}$
      $= 480\,\text{W}$

      Answer

      about $480\,\text{W}$. The difference is calculated from large numbers, so it is only indicative: the rated current $16\,\text{A}$ has two significant figures.

      Reasonableness

      In terms of currents: the kettle draws $8.7\,\text{A}$ and the microwave oven $5.2\,\text{A}$, together $13.9\,\text{A}$, so about $2.1\,\text{A}$ is left, that is, $230\,\text{V} \cdot 2.1\,\text{A} \approx 480\,\text{W}$. A toaster ($900\,\text{W}$) therefore does not fit, but a refrigerator does.

    2. Exercise 15-7Core

      An electric heater ($2000\,\text{W}$, $230\,\text{V}$) is connected to a long extension cord whose conductors have a total resistance of $0.30\,\Omega$. Assume that the current of the heater is the same as when it is connected directly to the socket.

      How large a thermal power is produced in the extension cord?

      W
      Answer

      $23\,\text{W}$

      Show the solution

      Given

      power of the heater $P = 2000\,\text{W}$, voltage $U = 230\,\text{V}$, resistance of the conductors $R = 0.30\,\Omega$

      Find

      the thermal power $P_\text{c}$ produced in the extension cord

      Principle

      The extension cord is in series with the heater, so the current of the heater flows through it. The current is obtained from the power of the heater, and in the cord electrical energy is transformed into internal energy at the rate $RI^2$. Assumption: the voltage drop in the cord is so small that the current of the heater is the same as without the extension cord.

      Formula

      $P = UI$, so $I = \dfrac{P}{U}$; in the cord $P_\text{c} = RI^2$, so

      $P_\text{c}$$= R\left(\dfrac{P}{U}\right)^2$

      Conversions

      None needed: all quantities are in base units.

      Substitution

      $I$$= \dfrac{2000\,\text{W}}{230\,\text{V}}$
      $= 8.696\,\text{A}$
      $P_\text{c}$$= 0.30\,\Omega \cdot (8.696\,\text{A})^2$
      $= 22.68\,\text{W}$

      Answer

      $23\,\text{W}$

      Two significant figures like the resistance $0.30\,\Omega$.

      Reasonableness

      The voltage across the cord is

      $RI$$= 0.30\,\Omega \cdot 8.7\,\text{A}$
      $\approx 2.6\,\text{V}$

      very small compared with $230\,\text{V}$, so the assumption holds. About $1\,\%$ of the power of the heater is used in the cord, which is little but enough to heat a cord wound on a reel.

    3. Exercise 15-8

      The greatest voltage between a conductor of a power line and an earthed pole is $90\,\text{kV}$. The dielectric strength of air is $3.0\,\text{MV/m}$.

      How long an air gap between the conductor and the pole is needed at least so that the air does not break down, when the field in between is taken as uniform? Calculate the lower limit given by the calculation. Answer in centimetres.

      cm
      Answer

      $3.0\,\text{cm}$

      Show the solution

      Given

      voltage $U = 90\,\text{kV}$, dielectric strength of air $E_\text{max} = 3.0\,\text{MV/m}$, uniform field

      Find

      the smallest air gap $d$ in centimetres

      Principle

      In a uniform field, the strength of the field is the voltage divided by the length of the gap (chapter The capacitor and its energy). Air does not break down when the field is at most the dielectric strength, so the shortest allowed gap is the one where the field is exactly $E_\text{max}$.

      Formula

      $E = \dfrac{U}{d} \le E_\text{max}$, so $d = \dfrac{U}{E_\text{max}}$

      Conversions

      $U$$= 90\,\text{kV}$
      $= 90 \cdot 1000\,\text{V}$
      $= 90\,000\,\text{V}$
      $E_\text{max}$$= 3.0\,\text{MV/m}$
      $= 3.0 \cdot 1\,000\,000\,\text{V/m}$

      $1\,\text{m} = 100\,\text{cm}$.

      Substitution

      $d$$= \dfrac{90\,000\,\text{V}}{3\,000\,000\,\text{V/m}}$
      $= 0.030\,\text{m}$
      $= 3.0\,\text{cm}$

      Answer

      $3.0\,\text{cm}$

      Two significant figures like the dielectric strength $3.0\,\text{MV/m}$.

      Reasonableness

      One megavolt per metre is one kilovolt per millimetre, so air withstands about $3\,\text{kV}$ per millimetre, and $90\,\text{kV}$ requires $30\,\text{mm}$. Real safety distances are metres, because near a thin conductor the field is much stronger than a uniform one, moisture and dirt weaken the air and overvoltages can occur in the grid; the calculated gap is only a lower limit from the calculation.

    4. Exercise 15-9

      In a bathroom the resistance of the current path of a wet person can be as low as $1.5\,\text{k}\Omega$.

      How large may the touch voltage be at most so that the current through the body stays below the let-go threshold $10\,\text{mA}$?

      V
      Answer

      $15\,\text{V}$

      Show the solution

      Given

      resistance of the current path $R = 1.5\,\text{k}\Omega$, greatest allowed current $I = 10\,\text{mA}$

      Find

      the greatest touch voltage $U$ in volts

      Principle

      The current through the body follows Ohm's law: when the resistance is given, the current grows with the voltage. The greatest allowed voltage is the one that gives exactly a current of $10\,\text{mA}$.

      Formula

      $I = \dfrac{U}{R}$, so $U = RI$

      Conversions

      $R$$= 1.5\,\text{k}\Omega$
      $= 1.5 \cdot 1000\,\Omega$
      $= 1500\,\Omega$
      $I$$= 10\,\text{mA}$
      $= 10 \cdot 0.001\,\text{A}$
      $= 0.010\,\text{A}$

      Substitution

      $U$$= 1500\,\Omega \cdot 0.010\,\text{A}$
      $= 15\,\text{V}$

      Answer

      $15\,\text{V}$

      Two significant figures like the resistance $1.5\,\text{k}\Omega$.

      Reasonableness

      The result is much smaller than the mains voltage $230\,\text{V}$ and smaller than the upper limit of protective extra-low voltage, $50\,\text{V}$. This is why an RCD and an especially low voltage are used in wet spaces: when the skin is wet, a voltage of just tens of volts can be dangerous.

    Level 3 · challenging 3 exercises

    Optional: application, two ideas together or a new situation where you reason for yourself.

    1. Exercise 15-10

      A circuit cable is dimensioned for a $10\,\text{A}$ fuse, and the total resistance of its conductors is $0.50\,\Omega$. A resident replaces a blown fuse without permission with a $25\,\text{A}$ fuse and connects devices that draw a total current of $22\,\text{A}$.

      How many times as large is the thermal power produced in the conductors compared with the power produced in them at a current of $10\,\text{A}$?

      times
      Answer

      $4.8$

      Show the solution

      Given

      resistance of the conductors $R = 0.50\,\Omega$, rated current $I_1 = 10\,\text{A}$, actual current $I_2 = 22\,\text{A}$

      Find

      how many times as large the thermal power $P_2$ is compared with the power $P_1$

      Principle

      In the conductors, electrical energy is transformed into internal energy at the rate $P = RI^2$. The resistance is the same in both situations, so the ratio of the powers depends only on the ratio of the currents squared. A $25\,\text{A}$ fuse does not cut off a current of $22\,\text{A}$, so the cable is loaded beyond its rating.

      Formula

      $P_1 = RI_1^2$ and $P_2 = RI_2^2$, so

      $\dfrac{P_2}{P_1}$$= \dfrac{I_2^2}{I_1^2}$

      Conversions

      None needed: the currents are in the same unit, and the units cancel.

      Substitution

      $P_1$$= 0.50\,\Omega \cdot (10\,\text{A})^2$
      $= 50\,\text{W}$
      $P_2$$= 0.50\,\Omega \cdot (22\,\text{A})^2$
      $= 242\,\text{W}$
      $\dfrac{P_2}{P_1}$$= \dfrac{242\,\text{W}}{50\,\text{W}}$
      $= 4.84$

      Answer

      about $4.8$ times as large, two significant figures like the current $22\,\text{A}$.

      Reasonableness

      The current is a little over twice as large, so the power is a little over four times as large, since $2^2 = 4$. The cable therefore heats up much more than it was designed to withstand, and the insulation can melt and catch fire. This is why a fuse must not be replaced with a larger one.

    2. Exercise 15-11

      A person touches the frame of a faulty device whose voltage relative to the ground is $230\,\text{V}$. The resistance of the body from hand to feet is $1.5\,\text{k}\Omega$, but they wear undamaged, dry rubber-soled shoes, and the resistance of the shoes and the dry floor together is $100\,\text{k}\Omega$. They do not touch anything else earthed at the same time.

      How large a current flows through the body? Answer in milliamperes.

      mA
      Answer

      $2.3\,\text{mA}$

      Show the solution

      Given

      voltage $U = 230\,\text{V}$, resistance of the body $R_\text{body} = 1.5\,\text{k}\Omega$, resistance of the shoes and the floor $R_\text{sh} = 100\,\text{k}\Omega$

      Find

      the current $I$ through the body in milliamperes

      Principle

      The current flows through the body, the shoes and the floor one after another, so the resistances are in series and their total resistance is the sum (chapter Resistors in series and in parallel). The same current flows through each, and it is obtained from Ohm's law with the total resistance.

      Formula

      $R = R_\text{body} + R_\text{sh}$ and $I = \dfrac{U}{R}$, so

      $I$$= \dfrac{U}{R_\text{body} + R_\text{sh}}$

      Conversions

      $R_\text{body}$$= 1.5 \cdot 1000\,\Omega$
      $= 1500\,\Omega$
      $R_\text{sh}$$= 100 \cdot 1000\,\Omega$
      $= 100\,000\,\Omega$

      $1\,\text{A} = 1000\,\text{mA}$.

      Substitution

      $I$$= \dfrac{230\,\text{V}}{1500\,\Omega + 100\,000\,\Omega}$
      $= \dfrac{230\,\text{V}}{101\,500\,\Omega}$
      $= 0.002266\,\text{A}$
      $= 2.3\,\text{mA}$

      Answer

      $2.3\,\text{mA}$

      Two significant figures like the resistance of the body $1.5\,\text{k}\Omega$.

      Reasonableness

      Without shoes the current would be $230\,\text{V} : 1500\,\Omega \approx 150\,\text{mA}$, over the limit for the danger of ventricular fibrillation. Shoes and a dry floor reduce the current below the let-go threshold $10\,\text{mA}$, but the current is felt, because it is over the threshold of perception $0.5\,\text{mA}$. A wet floor, a damaged shoe or touching a tap or an earthed device at the same time would bypass the shoes completely, so shoes are not protection.

    3. Exercise 15-12

      The graph shows the potential of the ground around a conductor that has fallen to the ground, in a calculated model. A person stands with their feet $1.0\,\text{m}$ apart directly away from the point of contact: the nearer foot is at a distance of $2.0\,\text{m}$ and the farther at $3.0\,\text{m}$. The resistance of the current path from one foot to the other, shoes included, is $4.0\,\text{k}\Omega$.

      Read the needed values from the graph. How large a current flows from one foot to the other? Answer in milliamperes.

      $1$
      $2$
      $3$
      $4$
      $5$
      $6$
      $7$
      $8$
      $200$
      $400$
      $600$
      $800$
      $1000$
      $1200$
      $0$
      $r\ (\text{m})$
      $V\ (\text{V})$
      mA
      Answer

      $50\,\text{mA}$

      Show the solution

      Given

      the potential of the ground from the graph $(r, V)$; the feet at distances $r_1 = 2.0\,\text{m}$ and $r_2 = 3.0\,\text{m}$; resistance of the current path $R = 4.0\,\text{k}\Omega$

      Find

      the current $I$ flowing from one foot to the other in milliamperes

      Principle

      The voltage between the feet, that is, the step voltage, is the difference of the potentials of the ground at the feet. The current flows from one foot through the body to the other foot, and it is obtained from Ohm's law.

      Reading the graph

      At $r = 2.0\,\text{m}$ the curve passes through an intersection of the grid at the value $V_1 = 600\,\text{V}$ and at $r = 3.0\,\text{m}$ at the value $V_2 = 400\,\text{V}$. The step voltage is their difference.

      Formula

      $U = V_1 - V_2$ and $I = \dfrac{U}{R}$, so $I = \dfrac{V_1 - V_2}{R}$

      Conversions

      $R$$= 4.0\,\text{k}\Omega$
      $= 4.0 \cdot 1000\,\Omega$
      $= 4000\,\Omega$

      $1\,\text{A} = 1000\,\text{mA}$.

      Substitution

      $I$$= \dfrac{600\,\text{V} - 400\,\text{V}}{4000\,\Omega}$
      $= \dfrac{200\,\text{V}}{4000\,\Omega}$
      $= 0.050\,\text{A}$
      $= 50\,\text{mA}$

      Answer

      $50\,\text{mA}$

      Two significant figures like the resistance $4.0\,\text{k}\Omega$.

      Reasonableness

      The current is at the limit for the danger of ventricular fibrillation, even though the person does not touch the conductor at all. If the feet were together, the potential difference and the current would be almost zero. A current from one foot to the other does not necessarily pass through the heart, but a fall can bring the heart into the path of the current. Farther away the curve levels off: the voltage between $4.0\,\text{m}$ and $6.0\,\text{m}$ is only $100\,\text{V}$, even though the gap is two metres, so it is worth moving away with short steps.

    Photographs

    • Moeller Xpole PXF-40-4-003-A-2288. Raimond Spekking. source, CC BY-SA 4.0
    • High voltage warning sign (pictogram) on fuse box in German shop. Pittigrilli. source, CC BY 4.0