Theme B — The Particulate Nature of Matter
B.5 Current and Circuits — IB Physics HL Revision Notes & Topical Questions
5 min read 13 parts Lesson 41 of 53 1 quiz
Lesson summary
B.5 Current and Circuits — IB PHYSICS HL notes: Define current, potential difference, resistance, resistivity, power and e.m.f.
- Energy source
- Complete circuit
- Components
- Definition
- Conventional current
- Electron flow
Part 1 of 11Circuit diagrams and meters
Circuit diagrams and meters
Energy source
- Energy source a cell, battery or power supply provides the potential difference
- A cell converts chemical energy to electrical energy and a battery is several cells
Complete circuit
- Complete circuit current flows only in a closed loop
- A switch opens or closes the loop
Ammeter
- Ammeter measures current and is connected in series
- An ideal ammeter has zero resistance
Voltmeter
- Voltmeter measures potential difference and is connected in parallel across the component
- An ideal voltmeter has infinite resistance
Components
- Components fixed resistor, variable resistor, LDR, thermistor, potentiometer, lamp, LED, heating element, motor and earth
Part 2 of 11Current and potential difference
1
Definition
- Definition current is the rate of flow of charge, I = Δq/Δt
- 1 A = 1 C s−1
2
Conventional current
- Conventional current the flow of positive charge from the positive to the negative terminal
3
Electron flow
- Electron flow electrons move the opposite way, from the negative to the positive terminal
4
Direct current
- Direct current flows in one direction only and is produced by cells and batteries
5
Definition
- Definition potential difference is the work done per unit charge moving a positive charge between two points, V = W/q
- 1 V = 1 J C−1
6
Electronvolt
- Electronvolt the energy needed to move an electron through a potential difference of 1 V
- 1 eV = 1.6 × 10−19 J from W = eV
7
Cells
- Cells charge gains electrical potential energy passing through the cell and transfers it to metal ions in the wire
8
Conductor
- Conductor allows charge to flow easily, for example silver, copper, aluminium and steel
- Metals have a lattice of positive ions in a sea of delocalised electrons
9
Insulator
- Insulator has very few free charges, for example rubber, plastic, glass and wood
- An insulator can still hold static charge on its surface
Part 3 of 11Conductors, resistance and Ohm's law
Conductors, resistance and Ohm's law
Cause of resistance
- Cause of resistance electrons collide with lattice ions and transfer energy that heats the wire
Definition
- R = V/I in ohms
- 1 Ω = 1 kg m2 s−3 A−2
Ohm's law
- Ohm's law for a component at constant temperature the current is proportional to the p.d.
- The I–V graph is a straight line through the origin
Ohmic components
- Ohmic components fixed resistors and metal wires at constant temperature
Non-ohmic components
- Non-ohmic components filament lamps, diodes, LEDs, thermistors and LDRs
Gradient
- Gradient with I on the y-axis, R = 1/gradient
Part 4 of 11Resistivity
Dependence
- Dependence resistance is proportional to length L and inversely proportional to cross-sectional area A
Definition
- ρ = RA/L in ohm-metres
- It is a property of the material and depends on temperature
Wire area
- A = πr2 so doubling the diameter quadruples the area and cuts the resistance to a quarter
Metals
- Metals low resistivity so they make good wires
Insulators
- Insulators very high resistivity so they safely cover wires
Part 5 of 11I–V characteristics
I–V characteristics
Fixed resistor
- Fixed resistor a straight line through the origin
Diode and LED
- Diode and LED forward-biased they show a sharp rise in current
- Reverse-biased the current is zero
Filament lamp
- Filament lamp nearly ohmic at low voltage
- The filament heats up as V rises, its resistance increases and the graph curves with a decreasing gradient
Part 6 of 11Series and parallel circuits
| Feature | Series | Parallel |
|---|---|---|
| Current | Same everywhere | Splits, I = I1 + I2 + … |
| Potential difference | Splits, V = V1 + V2 + … | Same across each branch |
| Total resistance | R = R1 + R2 + … (larger than any one) | 1/R = 1/R1 + 1/R2 + … (smaller than any one) |
| One component open | All components stop | Other branches continue |
- Equal resistors
- two in series double the resistance and two in parallel halve it
Part 7 of 11Electrical power
Heating effect
- Heating effect electrical energy is dissipated as thermal energy by current in a resistance
Equations
- P = E/t = IV = I2R = V2/RWhat the symbols mean: P = power (W = J s−1) · W or E = work done / energy transferred (J) · t = time (s) · F = force (N) · v = velocity (m s−1)
- E = VItWhat the symbols mean: E or W = energy transferred (J) · Q = charge (C) · V = potential difference (V) · I = current (A) · t = time (s)
Doubling
- Doubling doubling the current or voltage through a fixed resistor gives four times the power
Part 8 of 11Sources of electrical energy
Chemical cells
- Chemical cells single-use cells such as alkaline are non-rechargeable
- Lithium-ion and lead-acid cells are rechargeable
Solar cells
- Solar cells photons release electrons from the surface of photovoltaic cells
- Output is variable, daytime only and needs large areas
Wind generators
- Wind generators no fuel cost but the output is inconsistent and needs windy sites
Mains from fossil fuels
- Mains from fossil fuels reliable with high energy density but unsustainable and polluting
Part 9 of 11E.m.f. and internal resistance
E.m.f.
- E.m.f. the energy converted from chemical to electrical per coulomb passing through the supply
- It equals the terminal p.d. when no current flows
Internal resistance r
- Internal resistance r resistance inside the source that wastes energy and warms the cell
Equation
- ε = I(R + r)What the symbols mean: E or ε = e.m.f. (V) · I = current (A) · R = external resistance (Ω) · r = internal resistance (Ω) · V = terminal p.d. (V)
- Lost volts Vr = Ir and terminal p.d. V = ε − Ir
V–I graph
- V–I graph the intercept is ε and the gradient is −r
Part 10 of 11Variable resistance and sensors
Thermistor
- Thermistor an NTC thermistor has resistance that falls as temperature rises
- It is used in ovens, fire alarms and digital thermometers
LDR
- LDR resistance falls as light intensity rises
- It is millions of ohms in the dark and tens of ohms in bright light and is used in automatic street lights
Potentiometer
- Potentiometer a resistor with a sliding contact used as an adjustable potential divider
- The output varies from zero to the supply p.d.
Potential divider
- V1 = V × R1/(R1 + R2)
Part 11 of 11More from the specification
1
Circuit diagrams
- Circuit diagrams standard symbols show cells, resistors, ammeters and voltmeters and how they are connected.
2
Current flowing
- Current flowing current is the rate of charge flow, I = Q divided by t, the same at all points in series.
3
Charge passes
- Charge passes the charge passing a point in a time equals current times time, measured in coulombs.
4
Combined resistance
- Combined resistance in series it is the sum of resistances, in parallel the reciprocals add.
5
Kirchhoff's laws
- Kirchhoff's laws currents at a junction sum to zero, and voltages around a loop sum to zero.
6
Combined resistance
- Single resistance that could replace several resistors.
7
Circuit diagram
- Drawing of a circuit using standard symbols.
Key terms
| Term | Meaning |
|---|---|
| Electric current | The rate of flow of charge. |
| Potential difference | The work done per unit charge in moving charge between two points. |
| Electromotive force | The energy per unit charge transferred to electrical energy by a source. |
| Resistance | The ratio of the potential difference across a component to the current in it. |
| Resistivity | A material property equal to RA/L. |
| Internal resistance | The resistance of the materials inside a source of e.m.f. |
| Ohmic conductor | A conductor for which current is proportional to p.d. at constant temperature. |
| Potential divider | A series arrangement of resistors that provides a fraction of the supply p.d. |
Avoid these mistakes
1
Connecting an ammeter in parallel or a voltmeter in series — the ammeter goes in series and the voltmeter in parallel.
2
Saying all conductors obey Ohm's law — only components with constant resistance at constant temperature do.
3
Treating resistivity as the same as resistance — resistivity is a material property while resistance depends on shape.
4
Using the load resistance alone in ε = I(R + r) — the internal resistance must be added.
5
Forgetting to convert mA and kV to A and V before finding resistance.
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