E = -G M m / 2r
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
Total mechanical energy of a circular orbit. Use it when bound circular orbit.
E = -G M m / 2r
Advanced Concepts
The JEE-Advanced / NEET-hard concepts that separate top rankers — each a titled nugget with a real-world story, the idea in plain words, and a memory trick. Works even when the internet doesn't.
1,600 advanced concepts
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
Total mechanical energy of a circular orbit. Use it when bound circular orbit.
E = -G M m / 2r
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
Kepler's third law. Use it when orbit around a much larger mass M.
T^2 = (4 pi^2 / G M) a^3
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
Gravity at altitude h. Use it when above the surface.
g_h = g (R/(R+h))^2
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
Orbital velocity keeps a satellite circling; escape velocity (sqrt(2) times larger) lets it leave the gravity well entirely.
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
Above the surface g falls as 1/(R+h)^2; below the surface g falls roughly linearly to zero at the centre.
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
A bound orbit has negative total energy (ellipse/circle); an unbound path has zero or positive energy (parabola/hyperbola).
“GPS satellites must correct for both special and general relativity, or your maps would drift by kilometres a day.”
A higher orbit has greater (less negative) total energy; you must add energy to raise a satellite.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Simple harmonic motion is the projection of uniform circular motion onto a diameter, which is why it is sinusoidal.
Memory trick: SHM needs a linear restoring force F = -kx.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
A frequent error is thinking any periodic motion is SHM. In reality, simple harmonic motion is the projection of uniform circular motion onto a diameter, which is why it is sinusoidal.
Memory trick: SHM needs a linear restoring force F = -kx.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Total energy stays constant, continuously trading between kinetic and potential, and is proportional to amplitude squared.
Memory trick: E = 1/2 m omega^2 A^2, independent of time.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
A frequent error is thinking energy depends on where in the cycle you look. In reality, total energy stays constant, continuously trading between kinetic and potential, and is proportional to amplitude squared.
Memory trick: E = 1/2 m omega^2 A^2, independent of time.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Parallel springs add stiffness (k adds); series springs are softer (1/k adds).
Memory trick: springs are opposite to resistors: parallel adds k.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
A frequent error is swapping the series and parallel rules for springs. In reality, parallel springs add stiffness (k adds); series springs are softer (1/k adds).
Memory trick: springs are opposite to resistors: parallel adds k.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Damping removes energy so the amplitude decays exponentially; heavy damping stops oscillation altogether.
Memory trick: light damping lowers the frequency slightly and shrinks amplitude.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
A frequent error is thinking the frequency of light damping equals the undamped one exactly. In reality, damping removes energy so the amplitude decays exponentially; heavy damping stops oscillation altogether.
Memory trick: light damping lowers the frequency slightly and shrinks amplitude.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Driving a system near its natural frequency produces large-amplitude resonance, limited only by damping.
Memory trick: damping caps the resonant amplitude.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
A frequent error is thinking resonance amplitude is infinite even with damping. In reality, driving a system near its natural frequency produces large-amplitude resonance, limited only by damping.
Memory trick: damping caps the resonant amplitude.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Any rigid body swinging about a pivot has a period set by its moment of inertia and the distance to its centre of mass.
Memory trick: T = 2 pi sqrt(I / (m g d)).
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
A frequent error is using the simple-pendulum formula for an extended body. In reality, any rigid body swinging about a pivot has a period set by its moment of inertia and the distance to its centre of mass.
Memory trick: T = 2 pi sqrt(I / (m g d)).
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Two perpendicular SHMs combine into Lissajous figures; two parallel SHMs of close frequency give beats.
Memory trick: perpendicular SHMs trace Lissajous curves.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
A frequent error is assuming two SHMs always add to another simple SHM. In reality, two perpendicular SHMs combine into Lissajous figures; two parallel SHMs of close frequency give beats.
Memory trick: perpendicular SHMs trace Lissajous curves.
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Period of a mass on a spring. Use it when ideal spring, small oscillations.
T = 2 pi sqrt(m/k)
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Total energy of SHM. Use it when amplitude A, angular frequency omega.
E = 1/2 m omega^2 A^2
“Engineers add dampers to skyscrapers and bridges so wind and quakes don't drive them into deadly resonance.”
Period of a simple pendulum. Use it when small angular amplitude.
T = 2 pi sqrt(L/g)