Where is the object?
Choose a coordinate system.
A physical description begins by defining the frame and variables that locate the system.
Side 17
A study of how physical systems change, interact and conserve structure. Physics builds simplified models, derives consequences mathematically, then forces those predictions into contact with measurement.
Classical mechanics asks how position, velocity and acceleration evolve, and how forces alter that evolution.
Choose a coordinate system.
A physical description begins by defining the frame and variables that locate the system.
v = dx/dt
Velocity carries both magnitude and direction.
a = dv/dt
An object can accelerate by changing speed, direction or both.
F = ma in the classical regime.
Net force determines acceleration for a body of constant mass.
Surface, joint, string, orbit?
Constraints remove degrees of freedom and introduce reaction forces.
When symmetries or isolation conditions apply, quantities such as energy and momentum can remain constant even while the system changes internally.
For a classical particle, kinetic energy scales with mass and the square of speed.
Gravitational, elastic and electric interactions can be represented through potential-energy functions.
Net work changes kinetic energy; conservative forces can trade kinetic and potential energy.
Total momentum is conserved in an isolated system, making collisions easier to analyze.
It is conserved when no external torque acts on the system.
Two machines can perform the same work while differing in how quickly they do it.
A field assigns a physical quantity to each point in space and time, allowing distant interactions to be treated locally.
In Newtonian gravity, mass generates an attractive field; general relativity later reframes gravity geometrically.
A test mass responds to the local gravitational field.
Potential provides a scalar description related to the field through spatial change.
Electric fields act on charge and can store energy.
Moving charge and changing electric fields are associated with magnetic fields.
Maxwell’s equations unify electricity, magnetism and electromagnetic waves.
It is a mathematical object with values defined across space-time, used to predict how matter or other fields respond.
Wave descriptions connect local oscillation with transport through space and time.
| Quantity | Meaning | Relationship | Question |
|---|---|---|---|
| Amplitude | Maximum size of oscillation. | Often tied to energy or intensity. | How strong is the disturbance? |
| Frequency | Cycles per unit time. | f = 1/T | How rapidly does it oscillate? |
| Wavelength | Spatial period. | v = fλ | How far apart are matching phases? |
| Phase | Position within a cycle. | Controls interference. | Are oscillations aligned? |
| Group behavior | Envelope or packet motion. | Can differ from phase velocity. | How does information or energy propagate? |
Superposition can produce reinforcement or cancellation depending on phase.
Small repeated forcing can create large responses near a system’s resonant frequency.
The effect becomes prominent when dimensions are comparable to wavelength.
Thermodynamics tracks energy, heat, work and entropy without needing the exact trajectory of every microscopic particle.
Pressure, volume, temperature and composition summarize macroscopic state.
Energy is conserved: changes in internal energy arise through heat and work transfers.
Entropy tracks the number of accessible microscopic arrangements and constrains spontaneous macroscopic change.
For an isolated system, entropy does not spontaneously decrease.
Macroscopic thermodynamic behavior is connected to probability distributions over microscopic states.
Relativity and quantum mechanics revise assumptions that work extremely well at everyday scales but fail at very high speeds, strong gravity or microscopic scales.
The speed of light is invariant for inertial observers; simultaneity, time intervals and lengths are frame-dependent.
Mass and energy are related within relativistic dynamics rather than being completely separate conserved substances.
Matter-energy influences spacetime geometry, while geometry shapes free-fall motion.
Atomic and subatomic systems require quantum states rather than classical trajectories alone.
A quantum system can be represented as a combination of possible basis states before measurement.
Quantum uncertainty is structural to the theory, not merely poor instrumentation.
Newtonian mechanics is not “wrong” because relativity exists; it remains an excellent approximation within the regime where relativistic corrections are negligible.