Salam Academy
Paper 1 · Module

Electricity

6 subtopics≈ 205 min in total
  1. Electric current

    Current is the rate of flow of charge, I=ΔQΔtI=\dfrac{\Delta Q}{\Delta t}. Charge comes in whole multiples of the elementary charge e=1.60×10−19e=1.60\times10^{-19} C. In a conductor, current depends on the number density of charge carriers, their charge and their drift velocity: I=AnvqI=Anvq. Electrons drift slowly, but the signal travels almost instantly.

    ≈ 30 min
  2. E.m.f. and internal resistance

    A real source has an e.m.f. EE and an internal resistance rr. When it drives a current II through an external resistance RR, some energy is dissipated inside the source: E=I(R+r)E=I(R+r), so the terminal p.d. is V=E−IrV=E-Ir. The "lost volts" IrIr grow with current. A graph of VV against II is a straight line with intercept EE and gradient −r-r.

    ≈ 35 min
  3. Potential difference and power

    The potential difference across a component is the energy transferred from electrical to other forms per unit charge: V=WQV=\dfrac WQ, so 11 V =1=1 J C⁻¹. Electrical power is P=VIP=VI; combining with V=IRV=IR gives P=I2R=V2RP=I^2R=\dfrac{V^2}R. Choose whichever form uses the quantities you know.

    ≈ 30 min
  4. Kirchhoff's laws

    Kirchhoff's first law: the sum of currents into a junction equals the sum out (conservation of charge). Kirchhoff's second law: round any closed loop, the sum of e.m.f.s equals the sum of p.d.s (conservation of energy). From these: series R=R1+R2+…R=R_1+R_2+\dots; parallel 1R=1R1+1R2+…\dfrac1R=\dfrac1{R_1}+\dfrac1{R_2}+\dots.

    ≈ 40 min
  5. Resistance and resistivity

    Resistance is R=VIR=\dfrac VI. A metal at constant temperature obeys Ohm's law: current is proportional to p.d. A wire's resistance depends on its material, length and area: R=ρLAR=\dfrac{\rho L}A, where the resistivity ρ\rho is a material property. Filament lamps, diodes, thermistors and LDRs have non-ohmic, changing resistances.

    ≈ 35 min
  6. Potential dividers

    Two resistors in series share the supply p.d. in proportion to their resistances: Vout=R2R1+R2VinV_{\text{out}}=\dfrac{R_2}{R_1+R_2}V_{\text{in}}. Replacing one resistor with a thermistor or LDR makes the output depend on temperature or light. A potentiometer is a uniform resistance wire whose p.d. per unit length lets you compare e.m.f.s by finding the balance length, where a galvanometer reads zero.

    ≈ 35 min