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EI · lesson 1 of 12 · 80 min

Electric Charge, Current and Voltage

This is the starting point for Electronics Information. It explains where electricity comes from: protons and electrons, the coulomb, charge conservation, charging by friction, contact and induction, electric fields, and the difference between conductors, insulators and semiconductors. You then separate static electricity from current, define current as a flow rate of charge, and compare conventional current with electron drift.

Video lesson: Electric Charge, Current and Voltage

Video transcript

0:00 Welcome to this explainer. If you are prepping for the ASVAB and feeling, well, maybe just a little bit anxious about the math section, especially since you can't use a calculator on test day, you are in the absolute right place. We're going to break down these foundational electricity concepts and make them super logical, visual, and highly approachable. Here is our agenda for today. One, charge and static electricity. Two, current voltage and resistance. Three, circuits, meters, and units. Four, calculator-free math examples. Five, common ASVAB traps. And six, check yourself practice. We're starting with the smallest particles and building all the way up to solving circuit math completely by hand. Alright, let's jump right into section one. Charge and static electricity. To really get how electronics work, we've got to start with the absolute building blocks of matter. Protons carry a positive charge and are locked firmly inside the nucleus. But electrons, they carry a negative charge and can move from atom to atom. Practically every electrical effect we're going to talk about happens because those electrons are moving or shifting, while the protons just stay firmly put.

1:08 Now, individual electrons are incredibly tiny, so we grouped them into a standard unit called the Coulomb. Think of it like buying rice by the pound instead of buying it grain by grain. The Coulomb is the SI unit of electric charge, and it's equal to the charge of about 6.24 times 10 to the 18th electrons. That is over 6 quintillion electrons. For the test, just remember that the Coulomb, represented by a capital C, represents a massive amount of charge. Current voltage and resistance. So we know what charge is, but what happens when it actually moves? Well, that's the difference between static electricity and current electricity. Static electricity is charge that builds up and just stays on an insulator, like when you rub a balloon on your hair. Current electricity, on the other hand, is a continuing steady flow of charge through a conducting path. The underlying charges are exactly the same in both cases. The difference is just whether they sit still or keep moving around a circuit. This brings us to the holy trinity of basic electronics.

2:11 Current, represented by I, is the rate of charge flow, and its formula is I equals Q divided by T. Voltage, or V, is the energy transferred per unit of charge, so V equals E divided by Q. Think of voltage as the push. And resistance, R, is how strongly a component opposes that current. Linked together by Ohm's law, V equals I times R. So you've got the push, the flow that results, and the opposition. Okay, here's the detail that totally trips people up. Conventional current flows from positive to negative. This was actually a historical guess made before we even knew electrons existed. In physical reality, electron drift flows the exact opposite way, from negative to positive. But listen to me carefully on this one. Unless an ASVAB question specifically asks you for electron flow, you always always use conventional current, flowing from the positive terminal to the negative terminal. Circuits, meters, and units. To make these charges do useful work, we need a closed pathway and the right tools to measure them accurately. Memorizing this units table is absolutely your best defense on test day.

3:20 Charge is in coulombs, current is in amperes, voltage is in volts, resistance is in ohms, energy is in joules, and power is in watts. Seriously, take a mental snapshot of this. If you know what unit a meter is displaying, you instantly know exactly what it's reading. And when you're dealing with prefixes, you must convert them to base units before you calculate anything. Milli means one thousandth, so divide by 1000. Micro means 1 millionth, so divide by a million. Kilo means 1000, so you multiply by 1000. Doing this conversion first is a total game changer and will save you from getting a wildly wrong answer. When measuring these quantities in a circuit, placement is everything. An ammeter measures current, so it's placed in series, directly inside the loop, so the flow goes right through it. It has near zero resistance. A voltmeter measures the difference in energy, so it's placed in parallel across the component, and it has very high resistance, so it doesn't steal the current. Whatever you do, never put an ammeter in parallel across a battery. Its near zero resistance will create a short circuit that can literally blow the meter's fuse.

4:27 Calculator-free math examples. Let's do some math. Let's put this together and solve an exact ASVAB-style math problem completely by hand. I promise you, the math is designed to be friendly if you set it up right. Say a question asks, if a steady 30 coulombs of charge passes through a motor in six seconds, what's the current? Step 1, write the formula, i equals q divided by t. Step 2, plug in our values, 30 coulombs divided by six seconds. Step 3, do the simple division, 30 divided by six. Step 4, we get five amperes. See, no calculator needed, just trust the formula. Let's try one that's a little trickier because it involves a prefix. Question, how much charge passes if 200 milliamps flow for 30 seconds? Step 1, rearrange the formula, so q equals i times t. Step 2, convert that prefix. 200 milliamps divided by 1000 gives us 0.2 amps. Step 3, multiply 0.2 amps by 30 seconds. Mentally, just think two times three.

5:30 Step 4, that gives us a final charge of six coulombs. Always convert those prefixes first. Common ASVAB traps. Test makers love testing whether you actually understand the concepts or if you're just memorizing analogies. So let's run through some error checks. First, current is not used up by a lamp. The energy is. In a steady single loop, current is equal everywhere. Second, an open switch stops current, yes. But battery voltage still exists across that gap. Always treat open circuits as live. Finally, the water pipe analogy is great, but it has limits. If a wire breaks, it doesn't just empty out charge onto the floor like a leaky pipe. Thinking an ampere hour measures energy? It absolutely doesn't. Ampere hours only measure total charge capacity. One ampere hour is exactly 3,600 coulombs of charge. To find the actual energy, you would also need to know the voltage. Definitely don't fall for that one on test day. Check yourself practice. We have built a really solid foundation today.

6:34 So let's finish up this explainer with a quick pop quiz directly from the lesson to prove you've got this. Question 1, what is the SI unit of electric current? Is it A, coulomb, B, ampere, C, volt, or D, ohm? Think back to our units table. I'm going to pause for just a second so you can lock in your answer. And the answer is B, ampere. An ampere measures the rate of charge flow, specifically one coulomb passing a point each second. Remember, coulombs are for charge, volts are for the push, and ohms are for resistance. Alright, here is your final question. Question 4, what does a volt measure? A, electrical resistance, B, charge per second, C, total current, or D, electric potential difference. Take a moment to think about which of these perfectly describes what a volt represents. The correct answer is D, electric potential difference. Voltage is the energy given to every single unit of charge, which leaves us with a pretty great final thought for today. If voltage is the energy given to every single coulomb in a system, what kind of incredible things could you power if you truly mastered how to harness and calculate that energy?

7:46 Keep practicing those hand calculations and you are going to absolutely crush the ASVAB.

Contents · 78 sections
  1. What you will learn
  2. Electricity begins with charged particles
  3. Elementary charge and the coulomb
  4. Net positive, negative and neutral objects
  5. Like charges repel; unlike charges attract
  6. Charge conservation in charging events
  7. Charging by friction
  8. Charging by contact and grounding
  9. Charging without contact: induction
  10. Electric fields predict forces
  11. Conductors and insulators
  12. Semiconductors in context
  13. Static electricity versus current electricity
  14. Current is a flow rate of charge
  15. Current can vary during an interval
  16. Reading charge versus time
  17. Conventional current and electron drift
  18. Electrons move slowly; energy transfer can begin promptly
  19. Closed path and sustained current
  20. What a battery supplies
  21. Potential difference as energy per charge
  22. A single-point potential needs a reference
  23. Distinguishing voltage, current and resistance
  24. Ohm’s law within a limited scope
  25. Why higher voltage does not always mean more current
  26. Units at a glance
  27. Prefixes: milli, micro and kilo
  28. Ampere-hour is charge, not energy
  29. Power, charge and voltage connect
  30. Direct current versus alternating current
  31. A switch controls a path, not a charge reservoir
  32. A simple source-load-loop diagram
  33. Ammeter placement concept
  34. Voltmeter placement concept
  35. Meter units identify the physical quantity
  36. Positive and negative battery terminals
  37. Battery voltage versus available capacity
  38. Why the complete path matters
  39. A short circuit is not a normal load
  40. Electric energy in a load
  41. Avoid the water-pipe analogy trap
  42. DC polarity and potential differences
  43. Electric field versus potential difference
  44. Charge carriers are not always electrons
  45. Current continuity in a simple series path
  46. Static discharge and circuit current
  47. Interpreting electronic labels safely
  48. Calculator-free calculation strategy
  49. Estimate whether a value is plausible
  50. Reading a simple diagram without hidden assumptions
  51. Electric shock hazards: a conceptual note
  52. How EI compares with General Science
  53. Current from transferred charge
  54. Charge from current and time
  55. Time from charge and current
  56. Milliampere conversion
  57. Microampere conversion
  58. Voltage from energy and charge
  59. Energy from charge and voltage
  60. Voltage with a smaller energy transfer
  61. Charge from energy and voltage
  62. Power from voltage and current
  63. Energy from power and time
  64. Ohm’s law with a stated fixed resistor
  65. Ampere-hours as charge
  66. Series-loop current reasoning
  67. Practice: identify quantities
  68. Practice: describe conventional direction
  69. Practice: distinguish voltage from current
  70. Practice: graph slope
  71. Practice: measurement on a diagram
  72. Practice: choose units and reasonability
  73. Error check: current is not used up
  74. Error check: no current does not mean no voltage
  75. Error check: direction conventions
  76. Error check: voltage is not stored charge
  77. Memory map for test day
  78. Self-check before moving on
Visual lesson

Lesson slides

15 slides
Electric Charge, Current and Voltage – slide 1 of 15

What you will learn

This lesson builds the foundation for Electronics Information. You will describe the charges on electrons and protons, explain why total charge is conserved, compare conductors and insulators, and explain charging by friction, contact and induction. You will define current and voltage and use these relations:

You will also convert milli, micro and kilo prefixes and place meters correctly.

Electricity begins with charged particles

Ordinary matter is built from atoms. Each atom has a small nucleus containing protons, which carry positive charge, and neutrons, which carry none. Electrons, which carry negative charge, occupy the space around the nucleus.

A proton and an electron carry charges of exactly the same size but opposite sign. Protons are locked inside the nucleus in everyday situations, while some electrons, especially in metals, can move from atom to atom. Almost every electrical effect in this course comes from electrons moving or being shifted.

Elementary charge and the coulomb

The smallest free charge found in ordinary matter is the elementary charge, the size of the charge on one proton or one electron:

The coulomb (C) is the SI unit of charge. Because e is so tiny, one coulomb equals the charge of about electrons. A charged object always holds a whole-number multiple of e.

Net positive, negative and neutral objects

An object's net charge depends on its balance of protons and electrons. Equal numbers mean it is neutral. Extra electrons give it a net negative charge. Missing electrons leave more protons than electrons, so it has a net positive charge.

Neutral (4 +, 4 −), net negative (4 +, 6 −) and net positive (4 +, 2 −) objects.

Notice that objects gain positive charge by losing electrons, not by gaining protons. Neutral does not mean empty of charge; it means the positive and negative amounts cancel.

Like charges repel; unlike charges attract

Two objects with the same kind of net charge push each other apart. Two objects with opposite charges pull toward each other. Two negatively charged balloons drift apart, while a negative balloon and a positive sweater cling together.

Like charges repel; unlike charges attract.

The force grows stronger as the charges get larger and weaker quickly as the distance between them increases. Charged objects never merge their charges away just by being near each other.

Charge conservation in charging events

Electric charge is conserved. In an isolated system, the total charge before an event equals the total after it. Charging moves charge from one place to another; it never creates or destroys it.

If a plastic comb picks up a certain amount of negative charge from your hair, your hair is left with an equal amount of positive charge. Adding the two together still gives the original total, which was zero if both started neutral.

Charging by friction

When two different materials are rubbed together, electrons can transfer from one surface to the other. Materials differ in how tightly they hold electrons, and the one with the stronger hold tends to gain them.

Rub a rubber rod with wool and the rod usually becomes negative while the wool becomes positive. Dragging socks across a carpet on a dry day works the same way, and the small zap at the doorknob is the stored charge leaving you. Dry air helps because moisture lets charge leak away.

Electrons move from wool to rubber rod: rod net −, wool net +, total still 0.

Charging by contact and grounding

A charged object touching a neutral conductor shares some of its charge. Touch a negative rod to a neutral metal sphere, and some electrons flow onto the sphere, so both end up negative.

Grounding connects an object to Earth, a huge reservoir that can supply or accept electrons. A charged conductor that is grounded loses its excess charge, or receives what it lacks, until it is neutral. Grounding wires in buildings use this idea for safety.

Contact leaves rod and sphere both negative; grounding lets electrons flow to Earth until the sphere is neutral.

Charging without contact: induction

A charged object can rearrange charge in a nearby conductor without touching it. Bring a negative rod near a neutral metal sphere: the sphere's mobile electrons are pushed to the far side, leaving the near side positive. The sphere's total charge is still zero.

Negative rod near a neutral sphere: near side +, far side −, total charge 0.

If the far side is grounded while the rod stays close, electrons escape to ground. Remove the ground, then the rod, and the sphere is left with a net positive charge. The same shifting explains why a charged comb can pick up neutral bits of paper: the near side of the paper becomes slightly opposite in charge and is attracted.

Induction steps: ground far side (electrons escape), remove ground, remove rod: sphere net +.

Electric fields predict forces

An electric field is the region around a charge where another charge would feel a force. Field lines point away from positive charges and toward negative ones. A positive test charge placed in the field is pushed along the lines; a negative charge is pushed the opposite way.

Field lines point away from a positive charge and toward a negative charge.

Where the lines crowd together, the field is stronger. The field lets you predict the force on any charge at a point without listing every source charge that produces it.

Field lines from + to −: crowded where the field is stronger, sparse where weaker.

Conductors and insulators

A conductor contains charges that move easily. Metals such as copper and aluminum have loosely held outer electrons that drift through the material, which is why wiring is made of them. Salt water also conducts, using dissolved ions.

An insulator holds its electrons tightly, so charge hardly moves. Rubber, glass, dry wood and most plastics are insulators. That is why wire is coated in plastic. Insulators can still become charged by rubbing; the charge just stays where it was placed.

Semiconductors in context

Semiconductors, such as silicon and germanium, conduct better than insulators but far worse than metals. Their conductivity can be changed a great deal by temperature, light, or adding tiny amounts of other elements, a process called doping.

Doping can produce n-type material, with extra mobile electrons, or p-type material, with "holes" that act like moving positive charges. Joining these types makes diodes and transistors, the building blocks of modern electronics. Later lessons cover these devices in detail.

Static electricity versus current electricity

Static electricity is charge that builds up and stays on an object, usually an insulator, until it finds a path to escape. Balloon tricks and doorknob sparks are static effects. The charge sits still most of the time, then may discharge in a brief burst.

Current electricity is a continuing flow of charge through a conducting path, like the steady flow that lights a lamp. The underlying charges are the same; what differs is whether they stay put or keep moving around a circuit.

Current is a flow rate of charge

Electric current is how much charge passes a point each second:

I is current in amperes (A), Q is charge in coulombs, and t is time in seconds. One ampere means one coulomb passing each second. If 10 C passes in 5 s, the current is 2 A.

Current can vary during an interval

The formula

I = Q/t

gives the average current over a time interval. In many devices the current does not stay steady. A camera flash or a motor starting up draws a large surge, then settles to a smaller value.

When the current changes, the average still equals total charge divided by total time, but it hides the peaks and dips. To find the current at a particular instant, you look at a short slice of time around that moment.

Reading charge versus time

On a graph with charge on the vertical axis and time on the horizontal axis, the slope equals current. A straight line means a steady current; a steeper line means a larger current; a flat section means no current during that time.

Charge-time graph: gentle slope = smaller current, steeper = larger current, flat = none; slope equals current.

For an average over a longer stretch, take the total change in charge and divide by the total time. Do not simply average the slopes of separate pieces unless they last equally long.

Conventional current and electron drift

Conventional current is defined as the direction positive charge would flow: out of the positive terminal of a source, through the external circuit, and back into the negative terminal. This convention was set before electrons were discovered, and circuit diagrams still use it.

In metal wires, the moving carriers are actually electrons, which drift the opposite way, from negative to positive through the load. Both descriptions predict the same effects. Just be clear about which one a question asks for.

Conventional current goes + to − through the lamp; electrons drift − to +.

Electrons move slowly; energy transfer can begin promptly

Individual electrons in a wire drift slowly, often less than a millimeter per second in typical household currents. Yet a lamp lights almost instantly when you flip the switch.

The reason is that the wire is already full of mobile electrons. Closing the circuit sets up an electric field along the whole path very quickly, so electrons everywhere start drifting at nearly the same moment. Energy is delivered by that field, not by electrons racing from the switch to the lamp.

Closed path and sustained current

A steady current needs a complete, unbroken loop of conductors running from one terminal of the source, through the load, and back to the other terminal. This is a closed circuit.

If any part of the loop is broken, as by an open switch, a burned-out filament or a loose wire, the circuit is open. Charge would pile up at the gap almost at once and stop moving, so the steady current falls to zero everywhere in that loop.

Closed switch: current flows and lamp lights; open switch: gap, I = 0.

What a battery supplies

A battery does not supply electrons from an empty tank, and it does not store a fixed current. It uses chemical reactions to maintain a potential difference between its two terminals. That difference gives energy to charges that move through the external circuit.

The charges already present in the wires and the load are what flow. The battery is like a pump for energy per charge. Over time its chemicals are used up, and its ability to keep supplying energy runs down.

Potential difference as energy per charge

Voltage, or potential difference, is the energy transferred per unit of charge moved between two points:

V is in volts, E is energy in joules, and Q is charge in coulombs. One volt equals one joule per coulomb. A 1.5 V cell gives each coulomb that passes through it about 1.5 J of energy.

A single-point potential needs a reference

Voltage is always between two points. Saying a wire is at "5 volts" only means something if a reference point is agreed on, usually the circuit's ground or the negative battery terminal, which is called zero.

That is why a voltmeter has two leads. Change the reference and every potential value shifts, but the differences between points stay the same. Those differences are what drive current and transfer energy.

Distinguishing voltage, current and resistance

Voltage (V, in volts) is energy per charge between two points. Current (I, in amperes) is the rate of charge flow past a point. Resistance (R, in ohms, ) describes how strongly a component opposes current.

For many simple resistors the three are linked by Ohm's law:

A useful picture: voltage is the push, current is the flow that results, and resistance is the opposition.

Ohm’s law within a limited scope

Ohm's law, V = IR, holds well for "ohmic" components such as ordinary metal resistors kept at steady temperature. For these, doubling the voltage doubles the current, and the resistance stays constant.

Many components are not ohmic. A lamp filament's resistance climbs as it heats, and a diode lets current pass easily in one direction only. For them, V divided by I still gives a resistance value at that moment, but it changes with conditions.

Why higher voltage does not always mean more current

Current depends on both voltage and resistance. A 120 V lamp with high resistance can draw less current than a 12 V car starter motor with very low resistance.

Within one fixed ohmic resistor, more voltage does mean more current. Across different devices, you need to know the resistance too. Also, with no complete path, the current is zero no matter how large the voltage is.

Units at a glance

Charge Q is measured in coulombs (C). Current I is measured in amperes (A), where one ampere is one coulomb per second. Voltage V is measured in volts (V), where one volt is one joule per coulomb. Resistance R is measured in ohms (), where one ohm is one volt per ampere. Energy is measured in joules (J), and power in watts (W), where one watt is one joule per second.

Prefixes: milli, micro and kilo

Milli (m) means one thousandth, so 1 mA = 0.001 A. Micro () means one millionth, so 1 A = 0.000001 A. Kilo (k) means one thousand, so a 4.7 k resistor has 4,700 .

To convert milli to base units, divide by 1,000. For micro, divide by 1,000,000. For kilo, multiply by 1,000.

Ampere-hour is charge, not energy

Batteries are often labeled in ampere-hours (Ah) or milliampere-hours (mAh). An ampere-hour is a unit of charge: one ampere flowing for one hour. Since an hour has 3,600 s, 1 Ah equals 3,600 C.

It is not a measure of energy. To estimate energy you also need voltage. A 1.5 V cell and a 12 V battery with the same Ah rating move the same charge, but the 12 V battery delivers eight times as much energy.

Power, charge and voltage connect

Power is the rate of energy transfer. Combining the definitions of voltage and current gives a handy formula:

Power P is in watts, V in volts and I in amperes. A 6 V source pushing 0.5 A delivers 3 W, meaning 3 J each second.

Direct current versus alternating current

Direct current (DC) flows in one direction only. Batteries, solar cells and phone chargers' outputs supply DC. Its size can still vary, as in pulsating DC from a simple rectifier, but it never reverses.

Alternating current (AC) reverses direction periodically. Household outlets in the United States supply AC at 60 cycles per second (60 Hz), with a nominal voltage of about 120 V. AC is easy to step up or down with transformers, which makes it practical for power distribution over long lines.

Steady DC flat, pulsating DC humps above 0, AC reverses; one 60 Hz cycle = 1/60 s.

A switch controls a path, not a charge reservoir

A switch does not contain charge or energy. It simply opens or closes a gap in the conducting path. When closed, it completes the loop so current can flow. When open, it breaks the loop and the steady current stops.

Opening a switch does not drain the battery or erase its voltage. The charges in the wires remain; they just stop flowing around the loop. Across the open switch, a potential difference can still be measured.

Open switch: ammeter reads 0 A, voltmeter across the gap reads the battery voltage.

A simple source-load-loop diagram

The simplest circuit has three parts: a source, such as a battery; a load, such as a lamp or resistor, that turns electrical energy into another form; and conductors that join them into a loop. A switch is often added in the loop.

Source (battery), switch and load (lamp) joined by wires into one loop.

On a schematic, a battery is drawn as a long line (positive) and short line (negative). A resistor is a zigzag or box, and a lamp is a circle with a cross or loop inside. Straight lines are wires with negligible resistance.

Symbol key: battery, resistor (zigzag, box), lamp, wire, open and closed switch.

Ammeter placement concept

An ammeter measures current, so the current you want to measure must pass through it. That means placing it in series, inside the loop, by breaking the circuit and connecting the meter into the gap.

An ideal ammeter has nearly zero resistance, so it barely changes the circuit. Connecting an ammeter directly across a battery or a load (in parallel) creates a near short circuit and can blow the meter's fuse or damage the source.

Voltmeter placement concept

A voltmeter measures potential difference between two points, so its leads go across the component, in parallel with it. To read the voltage of a lamp, touch one lead to each side of the lamp without breaking the circuit.

An ideal voltmeter has very high resistance, so it draws almost no current and does not disturb the circuit. Placing it in series would block nearly all the current.

Ammeter in series in the loop; voltmeter across the lamp.

Meter units identify the physical quantity

The unit on a meter's display tells you what it is reading. A reading in A or mA is current from an ammeter setting. A reading in V or mV is potential difference from a voltmeter setting. A reading in or k is resistance from an ohmmeter setting, done with the circuit unpowered.

Positive and negative battery terminals

A battery's positive terminal, often marked plus and sometimes colored red, is at higher electric potential. The negative terminal, marked minus and often black, is at lower potential. The voltage rating is the difference between them.

In the external circuit, conventional current leaves the positive terminal, passes through the load, and returns to the negative terminal. Electrons drift the opposite way. Reversing a battery in a polarity-sensitive device can stop it working or damage it.

Battery voltage versus available capacity

Voltage and capacity are different ratings. Voltage tells how much energy each coulomb receives. Capacity, often in mAh or Ah, tells how much total charge the battery can deliver before it is considered empty.

AA and D cells both read about 1.5 V, but the D cell's larger capacity lets it run a flashlight much longer. Two batteries with equal capacity but different voltages store different total energy. A battery's voltage also sags somewhat as it nears depletion or delivers large currents.

Why the complete path matters

Charge flows steadily only around a closed loop. A single wire from the battery to a lamp, with no return path, lights nothing. A gap anywhere, whether at a switch, a broken solder joint or a loose connector, stops the current throughout that loop.

Troubleshooting often starts by tracing the path from the positive terminal through every component and back to the negative terminal to find the break.

A short circuit is not a normal load

A short circuit is an unintended low-resistance path that lets current bypass the load. With almost no resistance, the current can become very large, heating wires, draining the source quickly and possibly starting a fire.

The load in the shorted branch receives little or no current, so a shorted lamp goes dark even as the wires heat up. Fuses and circuit breakers exist to open the circuit when current gets dangerously high.

Shorting wire across the lamp carries a large current; lamp dark, I ≈ 0; fuse opens at high current.

Electric energy in a load

In a load, electrical energy is converted into other forms. A lamp produces light and heat, a heater produces heat, a motor produces motion and a speaker produces sound. The energy transferred equals the charge passed times the voltage across the load, and the rate is power, P = VI.

Avoid the water-pipe analogy trap

Water pipes help picture circuits: voltage is like pressure difference, current like flow rate, resistance like a narrow pipe. But the analogy has limits.

Wires do not empty out like pipes, and a broken wire does not leak charge onto the floor. Electrons are not used up in a lamp; energy is. The analogy also cannot explain induction or AC well. Rely on the definitions:

DC polarity and potential differences

In a DC circuit, polarity tells which side of a component is at higher potential. Across a resistor, the end where conventional current enters is more positive than the end where it leaves.

Meters show polarity too. If a digital voltmeter's leads are reversed, it displays a negative reading. That is not an error; it just means the red lead is at lower potential than the black lead.

Electric field versus potential difference

The electric field describes the force per unit charge at a point and has a direction. Potential difference describes the energy change per unit charge between two points and is a single number with no direction.

They are linked: a charge moving along the field direction moves toward lower potential. In a uniform field, a stronger field over the same distance gives a bigger voltage. A voltage source sets up a field in the wires, and that field pushes charges around the circuit.

Charge carriers are not always electrons

In metal wires, mobile electrons carry the current. In other materials the carriers differ. In salt water, battery electrolytes and the human body, positive and negative ions both move. In p-type semiconductors, holes act as moving positive charges.

Regardless of the carrier, current is measured as charge per second, and conventional direction is the direction positive charge would move.

Current continuity in a simple series path

In a single loop with no branches, the current is the same at every point. Charge does not pile up or vanish in a steady circuit, so the amount passing one point each second equals the amount passing any other point.

The current entering a lamp equals the current leaving it. What the lamp uses is energy, which is why the potential is lower on its exit side. Current is not used up along the way.

Static discharge and circuit current

A static discharge, such as a spark from your finger to a doorknob, can involve thousands of volts, yet it transfers only a very small charge over a tiny fraction of a second. The total energy is small, so it usually stings rather than injures.

A circuit current, by contrast, is sustained as long as the loop stays closed and the source keeps supplying energy. Static discharges can still destroy sensitive electronic chips, which is why technicians wear grounded wrist straps.

Interpreting electronic labels safely

Device labels list ratings such as voltage, current and power. A charger labeled "Output 5 V, 2 A" supplies 5 V and can deliver up to 2 A; the device decides how much it actually draws.

Match the voltage rating closely, because too high a voltage can damage a device. A supply's current rating should equal or exceed what the device needs. Never exceed a cord's or fuse's rated current. Labels are design limits, not measurements of what flows at every moment.

Calculator-free calculation strategy

The ASVAB does not allow calculators, so set problems up to stay simple. Write the formula first, then plug in values with units, converting prefixes before calculating. For example, with 200 mA and 30 s:

Rearrange before substituting:

or

Look for easy factors and cancel zeros.

Estimate whether a value is plausible

After calculating, ask whether the size makes sense. A phone charger supplying 500 A, a flashlight cell rated 1,500 V, or a lamp current of 0.000001 A would all be suspicious. Common results run from milliamps to a few amps for small electronics. A wildly off answer usually means a missed prefix or an inverted formula.

Reading a simple diagram without hidden assumptions

Answer from what the diagram actually shows. Check whether each switch is drawn open or closed, where each meter is placed, and whether any branch exists. Do not assume a switch is closed, that a meter reads current when its symbol is V, or that wires have resistance unless stated.

Treat ideal meters and wires as ideal unless the question says otherwise. If information is missing, such as the resistance needed for Ohm's law, the right answer may be that the value cannot be found from what is given.

Electric shock hazards: a conceptual note

Electric shock happens when the body becomes part of a circuit, letting current pass through it. The harm depends mainly on the current, its path through the body and how long it lasts. Even modest currents through the chest can disturb the heart's rhythm.

Higher voltages can push dangerous current through skin, and wet skin lowers resistance. Treat any circuit as live until it is properly de-energized and verified. Ground-fault protection and insulation reduce risk. Repair work on mains wiring belongs to trained people following approved procedures.

How EI compares with General Science

General Science covers electricity briefly along with biology, chemistry and Earth science. The Electronics Information subtest goes deeper into circuits, components, units, measurements and practical electronic devices.

The core ideas in this lesson, charge, current, voltage, resistance and power, appear on both tests. EI questions are more likely to ask for a calculation, a meter placement, a unit or a circuit behavior.

Current from transferred charge

A steady 30 C of charge passes through a motor in 6 s. Find the current.

The current is 5 A.

Charge from current and time

A steady 0.5 A current runs through a lamp for 40 s. How much charge passes?

The charge is 20 C.

Time from charge and current

How long does a 3 A current take to move 90 C of charge?

It takes 30 seconds.

Milliampere conversion

A meter reads 750 mA. What is that in amperes?

Milli means one thousandth, so divide by 1,000. 750 divided by 1,000 is 0.75. The current is 0.75 A. Check: an answer smaller than the milliamp number is expected, because each amp holds 1,000 mA.

Microampere conversion

A sensor draws 40 microamperes. Express this in amperes.

Micro means one millionth, so divide by 1,000,000. 40 divided by 1,000,000 is 0.00004. The current is 0.00004 A, which can also be written as 4 times 10 to the negative 5 A.

Voltage from energy and charge

A source gives 54 J of energy to 6 C of charge. What is its voltage?

The potential difference is 9 V.

Energy from charge and voltage

How much energy is transferred when 4 C of charge moves through a 12 V potential difference?

The energy is 48 J, since each coulomb carries 12 J.

Voltage with a smaller energy transfer

In a small cell, 3 J of energy is transferred to every 2 C of charge. Find the voltage.

The answer, 1.5 V, matches a typical AA cell. Voltage and charge are different quantities, so it does not matter that 1.5 is smaller than 2.

Charge from energy and voltage

A 9 V battery transfers 36 J. How much charge passed?

The charge is 4 C.

Power from voltage and current

A 12 V car accessory draws 2.5 A. What power does it use?

Use P = VI. Multiply 12 V by 2.5 A to get 30 W. The accessory takes in 30 joules of electrical energy every second.

Energy from power and time

A 60 W lamp runs for 5 minutes. How much energy does it use?

Convert time first: 5 minutes is 300 s. Energy equals power times time, so 60 W times 300 s gives 18,000 J, which is 18 kJ.

Ohm’s law with a stated fixed resistor

A fixed 300 resistor has 6 V across it. Find the current.

That equals 20 mA. Doubling the voltage to 12 V would double the current.

Ampere-hours as charge

A battery is rated 2 Ah. How many coulombs is that?

One ampere-hour is 1 A for 3,600 s, which is 3,600 C. So 2 Ah is 2 times 3,600, or 7,200 C. This is charge, not energy; energy would also need the voltage.

Series-loop current reasoning

A battery, a switch, a buzzer and a lamp form one unbranched loop. With the switch closed, an ammeter between the battery and the buzzer reads 0.3 A. What would it read between the buzzer and the lamp, and after the lamp?

There is only one path, and charge does not build up in a steady circuit, so the current is 0.3 A at every point. The buzzer and lamp convert energy, not charge. If the switch opens, current drops to 0 A everywhere in the loop.

Series loop with battery, switch, buzzer and lamp; every ammeter reads 0.3 A.

Practice: identify quantities

Prompt: A label reads 3.7 V. Which quantity? Answer: potential difference.

Prompt: A meter shows 120 mA. Which quantity? Answer: current.

Prompt: A battery is rated 2,500 mAh. Which quantity? Answer: charge capacity.

Prompt: A heater is marked 1,500 W. Which quantity? Answer: power, the rate of energy use.

Practice: describe conventional direction

Prompt: Which way does conventional current flow through a lamp connected to a battery? Answer: from the positive terminal, through the lamp, to the negative terminal.

Prompt: Which way do electrons drift in the same wire? Answer: the opposite way, from negative through the lamp to positive.

Prompt: Does choosing a direction convention change the brightness? Answer: No; both describe the same circuit.

Practice: distinguish voltage from current

Prompt: What does a 6 V rating tell you? Answer: each coulomb gets 6 J between the terminals.

Prompt: What does 2 A tell you? Answer: 2 C pass a point each second.

Prompt: A battery sits on a shelf unconnected. Is there voltage? Current? Answer: Voltage yes, current no.

Prompt: Which instrument measures each? Answer: voltmeter across, ammeter in series.

Practice: graph slope

Prompt: A charge-time line runs from (0 s, 0 C) to (5 s, 10 C). What is the current? Answer:

A

Prompt: What unit does the slope carry? Answer: coulombs per second, which is amperes.

Prompt: A flat segment means what? Answer: zero current then.

Practice: measurement on a diagram

Prompt: To measure current through a resistor, where does the ammeter go? Answer: in series with the resistor, in the same path.

Prompt: To measure voltage across the resistor? Answer: a voltmeter connected across its two ends, in parallel.

Prompt: What happens if an ammeter is placed across a battery? Answer: it acts as a near short, risking damage.

Prompt: Should resistance be measured on a live circuit? Answer: No; power it off first.

Practice: choose units and reasonability

Prompt: Energy per charge is measured in what unit? Answer: volts.

Prompt: A remote-control battery reads 3 kV. Reasonable? Answer: No; about 3 V is typical.

Prompt: A calculated LED current of 20 mA. Reasonable? Answer: Yes; small LEDs often run near that.

Prompt: Charge in what unit? Answer: coulombs.

Error check: current is not used up

Mistake: believing a lamp consumes current, so less flows out than in.

Why it is wrong: in a steady single loop, charge does not disappear or pile up, so current is equal everywhere.

Fix: say the lamp converts electrical energy into light and heat. Current in equals current out; it is the potential, not the current, that is lower after the lamp.

Error check: no current does not mean no voltage

Mistake: assuming zero current means zero voltage and therefore no danger.

Why it is wrong: an open switch stops current but the battery still has its terminal voltage, and a difference appears across the gap.

Fix: treat open circuits as possibly live. Measure voltage before touching anything.

Error check: direction conventions

Mistake: mixing conventional current with electron flow and getting the arrow backward.

Why it is wrong: the two run in opposite directions. Conventional current goes positive to negative through the load; electrons drift negative to positive.

Fix: read the question for which one it means. Unless electron flow is named, use conventional current.

Error check: voltage is not stored charge

Mistake: reading "9 V" as nine coulombs stored in the battery, or as a fixed current.

Why it is wrong: voltage is energy per coulomb between the terminals. Stored charge is the capacity, shown in Ah or mAh. Current depends on the load connected.

Fix: link volts to joules per coulomb, ampere-hours to charge, and current to what the circuit draws.

Memory map for test day

Charge Q is in coulombs; one electron carries about C. Like charges repel, unlike attract, and total charge is conserved. Conductors let charge move; insulators do not.

Conventional current runs positive to negative through the load. Ammeters go in series, voltmeters across. Milli divides by 1,000, micro by a million, kilo multiplies by 1,000. One Ah equals 3,600 C.

Self-check before moving on

Can you explain how an object becomes negatively or positively charged? Can you say why a charged rod attracts a neutral scrap of paper? Can you define the ampere and volt in coulombs and joules?

Can you convert 350 mA and 80 microamperes to amperes? Can you find current from a charge-time slope? Can you place an ammeter and a voltmeter correctly, explain why an open switch stops current but not voltage, and tell AC from DC? If any answer is shaky, revisit that section.

Quick review

How does an object become positively or negatively charged?
By gaining or losing electrons. Extra electrons give a net negative charge; missing electrons leave a net positive charge. Protons do not move. Like charges repel, unlike charges attract, and total charge is conserved.
What is the formula for electric current?
: current in amperes equals charge in coulombs divided by time in seconds. 1 A = 1 C/s. Example: 30 C in 6 s is 5 A.
How is voltage defined in terms of energy and charge?
: potential difference in volts equals energy in joules per coulomb of charge. 1 V = 1 J/C. A source giving 54 J to 6 C is 9 V.
Conventional current versus electron flow: which way does each go?
Conventional current flows from the positive terminal through the load to the negative terminal. Electrons in a metal wire drift the opposite way, negative to positive. Use conventional current unless electron flow is named.
Where do you connect an ammeter and a voltmeter?
Ammeter: in series, inside the loop, so the current passes through it (nearly zero resistance). Voltmeter: across the component, in parallel (very high resistance). An ammeter across a battery acts as a near short circuit.
How do you convert milli, micro and kilo prefixes?
Milli (m) divide by 1,000: 750 mA = 0.75 A. Micro () divide by 1,000,000: 40 A = 0.00004 A. Kilo (k) multiply by 1,000: 4.7 k = 4,700 .
Is an ampere-hour (Ah) rating a measure of energy?
No, it is charge: 1 Ah = 1 A for 3,600 s = 3,600 C, so 2 Ah = 7,200 C. Energy also requires the voltage; equal Ah at 12 V holds eight times the energy of 1.5 V.
Is current used up by a lamp in a single series loop?
No. In an unbranched loop the current is the same at every point; the lamp converts energy, not charge. Opening a switch stops current everywhere, but the battery voltage still appears across the gap.

What next?

About this lesson

Voltage is treated as energy per charge, with sections on batteries, reference points, polarity, and why higher voltage does not always mean more current. Units and prefixes, ampere-hours as charge rather than energy, switches, short circuits, and where ammeters and voltmeters belong are all covered. Worked calculations use I = Q/t, V = E/Q, simple V = IR and P = VI, followed by error checks such as current not being used up.

Expect around 80 minutes. Once you finish the self-check, take the lesson test, then continue to resistance and Ohm's law.

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