T = 2π√(m/k)
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
Period of a mass on a spring. Use it when ideal spring, small oscillations.
T = 2π√(m/k)
Fundamentals
The core facts every aspirant should own — each a titled nugget with a real-world story, the concept in plain words, and a memory trick. Works even when the internet doesn't.
300 fundamentals
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
Period of a mass on a spring. Use it when ideal spring, small oscillations.
T = 2π√(m/k)
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
Period of a simple pendulum. Use it when small angular amplitude.
T = 2π√(L/g)
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
Wave speed equals frequency times wavelength. Use it when any wave.
v = fλ
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
Number of beats heard per second. Use it when two nearly-equal frequencies.
f_beat = |f₁ − f₂|
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
In a transverse wave particles move perpendicular to the wave (light, string); in a longitudinal wave they move along it (sound).
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
Amplitude sets the loudness/energy of a wave; frequency sets its pitch/colour.
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
Mechanical waves need a medium (sound); electromagnetic waves (light) travel through vacuum.
“A swing, a guitar string and an earthquake all speak the same language: oscillations.”
It depends only on length and g — mass cancels out.
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
A frequent error is ignoring that like charges repel and unlike attract when assigning direction. In reality, the force between two point charges, F = kq₁q₂/r², along the line joining them.
Memory trick: it mirrors gravitation but can be attractive OR repulsive.
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
A frequent error is treating field (a vector) and potential (a scalar) as the same thing. In reality, the force per unit positive charge, E = F/q; field lines point away from positive charges.
Memory trick: field lines never cross and start on + and end on − charges.
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
A frequent error is thinking zero field means zero potential (or vice versa). In reality, the work done per unit charge to bring a charge from infinity to a point, V = kQ/r.
Memory trick: potential is a scalar — just add contributions with sign, no directions.
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
A frequent error is forgetting a dielectric increases capacitance. In reality, a capacitor's ability to store charge per volt, C = Q/V; for parallel plates C = ε₀A/d.
Memory trick: closer, larger plates (and a dielectric) store more charge.
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
Coulomb force between point charges. Use it when point charges in vacuum.
F = kq₁q₂/r²
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
Field of a point charge at distance r. Use it when point charge.
E = kQ/r²
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
Potential of a point charge. Use it when point charge, zero at infinity.
V = kQ/r
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
Energy stored in a charged capacitor. Use it when capacitance C at voltage V.
U = ½CV²
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
Field is a vector (force per charge, N/C); potential is a scalar (energy per charge, volts) — field points from high to low potential.
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
In series the charge is the same and 1/C adds (total C smaller); in parallel the voltage is the same and C adds (total C larger).
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
A conductor has free charges that move easily; an insulator holds its charges in place.
“Rub a balloon on your hair and it sticks to the wall — electrostatics you can feel.”
E is a vector and V a scalar; E can be zero where V isn't (inside a charged shell) and vice versa.
“Every light you switch on is Ohm's law quietly at work.”
A frequent error is assuming every component is ohmic (a diode or bulb filament is not). In reality, for many conductors V = IR at constant temperature.
Memory trick: Ohm's law is a property of some materials, not a universal rule.
“Every light you switch on is Ohm's law quietly at work.”
R = ρL/A: resistance grows with length and shrinks with cross-section; resistivity ρ is the material's own property.
Memory trick: a long thin wire resists more than a short thick one of the same material.
“Every light you switch on is Ohm's law quietly at work.”
A frequent error is confusing resistance (depends on shape) with resistivity (depends only on material and temperature). In reality, R = ρL/A: resistance grows with length and shrinks with cross-section; resistivity ρ is the material's own property.
Memory trick: a long thin wire resists more than a short thick one of the same material.
“Every light you switch on is Ohm's law quietly at work.”
In series the current is the same and resistances add; in parallel the voltage is the same and 1/R values add.
Memory trick: parallel resistance is always less than the smallest branch.