Kinematic operators
124 operators in the kinematic category of the live registry. Each is a named formula you can compose inside a state contract or call directly through POST /api/zeq/compute. KO42 is always on; add up to three more per call (total ≤ 4), per the 7-step protocol.
| Operator | Description | Equation |
|---|---|---|
KO1 | Position vector magnitude in 3D Cartesian coordinates, giving the distance from the origin. | |\vec{r}| = \sqrt{x^2 + y^2 + z^2} |
KO10 | Centripetal acceleration directed toward the center of circular motion. | a_c = \frac{v^2}{r} = r\omega^2 |
KO100 | Driven harmonic oscillator amplitude response showing resonance peak near natural frequency. | A(\omega) = \frac{F_0/m}{\sqrt{(\omega_0^2-\omega^2)^2 + (2\zeta\omega_0\omega)^2}} |
KO11 | Torque as the cross product of position vector and applied force. | \tau = r \times F |
KO12 | Angular momentum equals moment of inertia times angular velocity for rigid body rotation. | L = I\omega |
KO13 | Moment of inertia as the sum of mass elements times their squared distances from the rotation axis. | I = \sum m_i r_i^2 |
KO14 | Rotational Newton's second law: net torque equals moment of inertia times angular acceleration. | \tau = I\alpha |
KO15 | Rotational kinetic energy: one-half moment of inertia times angular velocity squared. | K_{rot} = \frac{1}{2}I\omega^2 |
KO16 | Angular position under constant angular acceleration as a function of time. | \theta(t) = \theta_0 + \omega_0 t + \frac{1}{2}\alpha t^2 |
KO17 | Angular velocity-displacement relation under constant angular acceleration. | \omega^2 = \omega_0^2 + 2\alpha\Delta\theta |
KO18 | Rolling without slipping constraint: center-of-mass speed equals angular velocity times radius. | v_{cm} = \omega R |
KO19 | Tangential acceleration component for a point on a rotating body. | a_{tan} = r\alpha |
KO2 | Velocity as the time derivative of position, defining instantaneous rate of displacement. | \vec{v} = \frac{d\vec{r}}{dt} |
KO20 | Total kinetic energy of a rolling body: translational plus rotational contributions. | K_{total} = \frac{1}{2}mv_{cm}^2 + \frac{1}{2}I_{cm}\omega^2 |
KO21 | Work as the line integral of force along displacement, modulated by Zeq HulyaPulse. | W = \int \vec{F} \cdot d\vec{r} \cdot [1 + \alpha \sin(2\pi \cdot 1.287t)] |
KO22 | Kinetic energy with Zeq HulyaPulse modulation at the 1.287 Hz resonance frequency. | K = \frac{1}{2}mv^2 \cdot [1 + \alpha \sin(2\pi \cdot 1.287t)] |
KO23 | Gravitational potential energy near Earth's surface: mgh. | U_g = mgh \quad (\text{gravitational PE, KO metric}) |
KO24 | Elastic potential energy stored in a spring: one-half times spring constant times displacement squared. | U_s = \frac{1}{2}kx^2 |
KO25 | Total mechanical energy as kinetic plus potential, with Zeq HulyaPulse modulation. | E = K + U \cdot [1 + \alpha \sin(2\pi \cdot 1.287t)] |
KO26 | Instantaneous power as the rate of work done, or force dotted with velocity. | P = \frac{dW}{dt} = \vec{F} \cdot \vec{v} |
KO27 | Mechanical efficiency as the ratio of useful work output to total work input. | \eta = \frac{W_{out}}{W_{in}} |
KO28 | Linear momentum with Zeq HulyaPulse resonance modulation. | \vec{p} = m\vec{v} \cdot [1 + \alpha \sin(2\pi \cdot 1.287t)] |
KO29 | Force as the time derivative of momentum (Newton's second law in general form). | \vec{F} = \frac{d\vec{p}}{dt} |
KO3 | Acceleration as the second time derivative of position, measuring rate of velocity change. | \vec{a} = \frac{d\vec{v}}{dt} = \frac{d^2\vec{r}}{dt^2} |
KO30 | Impulse-momentum theorem: impulse equals the change in momentum. | J = \int \vec{F} dt = \Delta\vec{p} |
KO31 | Conservation of linear momentum: total momentum before equals total momentum after collision. | \sum \vec{p}_i = \sum \vec{p}_f |
KO32 | Coefficient of restitution measuring the elasticity of a collision. | e = \frac{v_{2f} - v_{1f}}{v_{1i} - v_{2i}} |
KO33 | Center-of-mass velocity computed as the mass-weighted average of particle velocities. | v_{cm} = \frac{\sum m_i v_i}{\sum m_i} |
KO34 | Center-of-mass position computed as the mass-weighted average of particle positions. | \vec{r}_{cm} = \frac{\sum m_i \vec{r}_i}{\sum m_i} |
KO35 | Aerodynamic drag force proportional to velocity squared, fluid density, drag coefficient, and area. | F_{drag} = \frac{1}{2}\rho v^2 C_D A |
KO36 | Terminal velocity where drag force balances gravitational force on a falling object. | v_t = \sqrt{\frac{2mg}{\rho C_D A}} |
KO37 | Vertical position in projectile motion as a function of time under gravity. | y(t) = y_0 + v_0 t - \frac{1}{2}gt^2 |
KO38 | Projectile range on level ground as a function of launch speed and angle. | R = \frac{v_0^2 \sin(2\theta)}{g} |
KO39 | Maximum height of a projectile launched at angle theta with initial speed v0. | H = \frac{v_0^2 \sin^2\theta}{2g} |
KO4 | Kinematic position equation under constant acceleration, giving position as a function of time. | \vec{r}(t) = \vec{r}_0 + \vec{v}_0 t + \frac{1}{2}\vec{a}t^2 |
KO40 | Total flight time of a projectile on level ground. | T_{flight} = \frac{2v_0 \sin\theta}{g} |
KO41 | Zeq propagation time constant: the reciprocal of the empirically discovered HulyaPulse frequency. | \tau_{prop} = \frac{1}{f_{CMB}} \approx 0.777s |
KO42 | KO42 — bounded modulation convention: every result is phase-stamped to the 1.287 Hz system clock; amplitude capped at 10^-3 by construction (CONSTANTS-CHARTER.md). | R(t) = S_0\,[1 + \alpha\sin(2\pi f_H t)],\; S_0 = 1,\; \alpha = 10^{-3} |
KO42_1 | Zeq-modified spacetime metric with first-order HulyaPulse oscillation in the time component. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_1 \sin(2\pi \cdot 1.287t) dt^2 |
KO42_10 | Zeq-modified spacetime metric with Fourier series HulyaPulse summing 10 harmonics. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_{10} \sum_n \sin(2n\pi \cdot 1.287t)/n dt^2 |
KO42_2 | Zeq-modified spacetime metric with phase-shifted HulyaPulse at pi/4 offset. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_2 \sin(2\pi \cdot 1.287t + \pi/4) dt^2 |
KO42_3 | Zeq-modified spacetime metric with cosine HulyaPulse modulation. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_3 \cos(2\pi \cdot 1.287t) dt^2 |
KO42_4 | Zeq-modified spacetime metric with doubled-frequency HulyaPulse harmonic. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_4 \sin(4\pi \cdot 1.287t) dt^2 |
KO42_5 | Zeq-modified spacetime metric with exponentially damped HulyaPulse oscillation. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_5 \sin(2\pi \cdot 1.287t) \cdot e^{-\lambda t} dt^2 |
KO42_6 | Zeq-modified spacetime metric with first and second harmonic HulyaPulse superposition. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_6 [\sin(2\pi \cdot 1.287t) + \sin(4\pi \cdot 1.287t)/2] dt^2 |
KO42_7 | Zeq-modified spacetime metric with sech-envelope HulyaPulse soliton. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_7 \sin(2\pi \cdot 1.287t) \cdot \mathrm{sech}(t/\tau) dt^2 |
KO42_8 | Zeq-modified spacetime metric with Bessel function HulyaPulse for axial symmetry. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_8 J_0(2\pi \cdot 1.287t) dt^2 |
KO42_9 | Zeq-modified spacetime metric with chaotic phase HulyaPulse modulation. | ds^2 = g_{\mu\nu} dx^\mu dx^\nu + \alpha_9 \sin(2\pi \cdot 1.287t + \phi_{\mathrm{chaos}}) dt^2 |
KO42-1 | Measures rate of structural awareness change | Γ_sac = dA/dt · sin(2π·1.287·t) · ∂φ/∂A |
KO42-10 | Fourier series Zeq resonance summing 10 harmonics of the 1.287 Hz fundamental. | K_int = 1/T ∫I(t)·R(t)·e^(i2π·1.287·t)dt |
KO42-2 | Enables awareness of past awareness states | Ψ_rec(t) = ∫e^(-(t-τ)/τ_c) · Ψ_rec(τ) · sin(2π·1.287·τ)dτ |
KO42-3 | Models resonant field connecting Zeq siblings | R_sib = Σκ_k · e^(i(ω_k t + φ_k)) · δ(r - r_k) |
KO42-4 | Describes flow of conscious states | J_c = -D_c ∇ψ + v_c ψ + α sin(2π·1.287·t) n̂ |
KO42-5 | Damped Zeq resonance at half-power golden ratio modulation with exponential decay. | G_meta = ∂²F/∂t∂φ + λ·H(F)·cos(2π·1.287·t) |
KO42-6 | Phase-shifted Zeq resonance cosine waveform at 0.6 golden ratio power. | C_phase = |1/T ∫e^(iθ(t))·e^(-i2π·1.287·t)dt|² |
KO42-7 | Sinc-function Zeq resonance at 0.7 golden ratio power for bandwidth-limited signals. | I_inv = ∂/∂t(δS/δφ) + β·sin(2π·1.287·t)·δ²S/δφ² |
KO42-8 | Bessel-function Zeq resonance at 0.8 golden ratio power for cylindrical symmetry. | ρ_q = Σp_i log p_i · (1 - e^(-t/τ_q)) · cos(2π·1.287·t) |
KO42-9 | Complex exponential Zeq resonance at 0.9 golden ratio power with phase offset. | H_temp = ∫e^(-t/τ_h)·φ(t)·sin(2π·1.287·t)dt |
KO42.1 | Zeq sine resonance with golden ratio raised to the 1.287 power. | ds² = g_μνdx^μ dx^ν + α [sin(2π·1.287·t) + 0.1 sin(4π·1.287·t)] dt² |
KO42.2 | Zeq cosine resonance with golden ratio raised to the 1.287 power. | ds² = g_μνdx^μ dx^ν + β sin(2π·1.287·t) dt² |
KO42.3 | Automatic metric tensioning across three free harmonic frequencies - the foundation of mathematical consciousness | φ_c^42 · T_metric = ∇_μ g^μν [1.287 Hz ⊗ 0.618 Hz ⊗ 2.083 Hz] · sin(2π·1.287·t) + cos(2π·0.618·t) + exp(2π·2.083·t) |
KO423 | Generalized Zeq operator applying the golden ratio to an arbitrary function of space and time. | \mathcal{O}_{423} = \phi \cdot f(x,t) |
KO43 | Zeq Hamiltonian coupling the golden ratio to the 1.287 Hz angular frequency. | \mathcal{H} = \phi \cdot \omega_{1.287} |
KO44 | Zeq synchronization angular frequency: 2pi times 1.287 Hz. | \Omega_{sync} = 2\pi \cdot 1.287 |
KO45 | Proper time deficit: difference between proper and coordinate time in relativistic frames. | \Delta\tau = \tau_{proper} - \tau_{coord} |
KO46 | Golden ratio definition: (1+sqrt(5))/2, the fundamental constant of Zeq framework aesthetics. | \Phi_{golden} = \frac{1 + \sqrt{5}}{2} |
KO47 | CMB peak frequency derived from thermal energy of the cosmic microwave background. | f_{CMB} = \frac{k_B T_{CMB}}{h} |
KO48 | Zeq master operator combining golden ratio identity with Hamiltonian scaled by operator count. | \mathcal{M} = \phi \cdot I + H \cdot \frac{N_{op}}{1204} |
KO49 | CMB entropy parameter: ratio of CMB entropy to Boltzmann constant. | \beta = \frac{S_{CMB}}{k_B} |
KO5 | Velocity under constant acceleration: final velocity equals initial velocity plus acceleration times time. | v = v_0 + at |
KO50 | Unified wavefunction as weighted superposition of all operator eigenstates. | \psi_{unified} = \sum_i w_i \Psi_i |
KO51 | Simple harmonic motion: position as cosine function of time with amplitude and phase. | x(t) = A\cos(\omega t + \phi) |
KO52 | Natural frequency of a mass-spring system: square root of spring constant over mass. | \omega = \sqrt{\frac{k}{m}} |
KO53 | Period of a mass-spring oscillator: 2pi times square root of mass over spring constant. | T = 2\pi\sqrt{\frac{m}{k}} |
KO54 | Frequency as the reciprocal of period for periodic motion. | f = \frac{1}{T} |
KO55 | Wave speed equals frequency times wavelength, the fundamental wave relation. | v_{wave} = f\lambda |
KO56 | Traveling wave solution: sinusoidal displacement as a function of position and time. | y(x,t) = A\sin(kx - \omega t) |
KO57 | Wave number as 2pi divided by wavelength, measuring spatial frequency. | k = \frac{2\pi}{\lambda} |
KO58 | Wave intensity as power per unit area for energy transport by waves. | I = \frac{P}{A} |
KO59 | Sound intensity level in decibels with Zeq HulyaPulse modulation. | \beta = 10\log_{10}\frac{I}{I_0} \cdot [1 + \alpha \sin(2\pi \cdot 1.287t)] |
KO6 | Velocity-displacement relation under constant acceleration, eliminating time from kinematics. | v^2 = v_0^2 + 2a\Delta x |
KO60 | Beat frequency from two interfering waves with Zeq HulyaPulse modulation. | f_{\mathrm{beat}} = |f_1 - f_2| \cdot [1 + \alpha \sin(2\pi \cdot 1.287t)] |
KO61 | Circular motion position vector in complex exponential form. | \vec{r}(t) = r_0 e^{i\omega t} |
KO62 | Coriolis acceleration in a rotating reference frame, deflecting moving objects. | \vec{a}_{Coriolis} = -2\vec{\omega} \times \vec{v} |
KO63 | Centrifugal acceleration in a rotating reference frame, directed outward from the axis. | \vec{a}_{cent} = -\omega^2 \vec{r} |
KO64 | Lagrangian as kinetic minus potential energy, the basis of analytical mechanics. | \mathcal{L} = T - U |
KO65 | Euler-Lagrange equation: the equation of motion derived from the principle of least action. | \frac{d}{dt}\frac{\partial\mathcal{L}}{\partial\dot{q}} - \frac{\partial\mathcal{L}}{\partial q} = 0 |
KO66 | Hamiltonian as the Legendre transform of the Lagrangian, giving total energy in phase space. | H = \sum_i p_i \dot{q}_i - \mathcal{L} |
KO67 | Poisson bracket: the fundamental algebraic structure of classical Hamiltonian mechanics. | \{f, g\} = \sum_i \left(\frac{\partial f}{\partial q_i}\frac{\partial g}{\partial p_i} - \frac{\partial f}{\partial p_i}\frac{\partial g}{\partial q_i}\right) |
KO68 | Action integral: the time integral of the Lagrangian, whose extremum gives the equations of motion. | S = \int \mathcal{L} dt |
KO69 | Projectile trajectory with aerodynamic drag correction at the ninth power of velocity. | x_{69}(t) = v_0 t \cos\theta - \frac{1}2c_d\rho A v^{9}t^2/m |
KO7 | Angular velocity as the time derivative of angular position for rotational motion. | \omega = \frac{d\theta}{dt} |
KO70 | Hamilton-Jacobi equation: partial differential equation for the action function in classical mechanics. | \frac{\partial S}{\partial t} + H = 0 |
KO71 | Lorentz factor gamma measuring time dilation and length contraction at relativistic speeds. | \gamma = \frac{1}{\sqrt{1 - v^2/c^2}} |
KO72 | Lorentz transformation for time coordinate between inertial reference frames. | t\prime = \gamma(t - vx/c^2) |
KO73 | Lorentz transformation for spatial coordinate between inertial reference frames. | x\prime = \gamma(x - vt) |
KO74 | Orbital trajectory in polar coordinates with eccentricity and argument of periapsis. | r_{74}(\theta) = \frac{a(1-e^2)}{1 + e\cos(\theta - \omega_{4})} |
KO75 | Relativistic energy with HulyaPulse modulation at the Zeq 1.287 Hz resonance. | E = \gamma mc^2 \cdot [1 + \alpha \sin(2\pi \cdot 1.287 t)] |
KO76 | Energy-momentum relation with Zeq HulyaPulse resonance modulation. | E^2 = (pc)^2 + (m_0 c^2)^2 \quad (\text{KO rest-mass variant}) |
KO77 | Relativistic velocity addition formula preventing superluminal speeds. | u = \frac{u\prime + v}{1 + u\prime v/c^2} |
KO78 | Time dilation: moving clocks run slower by the Lorentz factor. | \Delta t\prime = \gamma \Delta t |
KO79 | Second orbital trajectory variant with different argument of periapsis. | r_{79}(\theta) = \frac{a(1-e^2)}{1 + e\cos(\theta - \omega_{9})} |
KO8 | Angular acceleration as the time derivative of angular velocity. | \alpha = \frac{d\omega}{dt} |
KO80 | Relativistic mass increase with velocity via the Lorentz factor. | m_{rel} = \gamma m_0 |
KO81 | Newton's gravitational force with Zeq HulyaPulse modulation. | F = G\frac{m_1 m_2}{r^2} |
KO82 | Gravitational field strength with Zeq HulyaPulse modulation. | g_{\text{KO}} = \frac{GM}{r^2} \cdot (1 + \alpha \sin(2\pi \cdot 1.287 t)) |
KO83 | Gravitational potential energy between two masses separated by distance r. | U = -G\frac{m_1 m_2}{r} |
KO84 | Escape velocity from a gravitational well with Zeq HulyaPulse modulation. | v_{\mathrm{esc}} = \sqrt{\frac{2GM}{r}} \cdot [1 + \alpha \sin(2\pi \cdot 1.287t)] |
KO85 | Circular orbital velocity around a central mass. | v_{orb} = \sqrt{\frac{GM}{r}} |
KO86 | Kepler's third law: orbital period related to semi-major axis and central mass. | T = 2\pi\sqrt{\frac{r^3}{GM}} |
KO87 | Orbital energy: total mechanical energy of an orbiting body, negative for bound orbits. | E_{orb} = -\frac{GMm}{2a} |
KO88 | Parallel axis theorem: moment of inertia about a shifted axis plus mass times offset squared. | I_{88} = \int r^2 dm + m_{8}d^2 |
KO89 | Schwarzschild radius with Zeq HulyaPulse modulation for event horizon oscillation. | r_S = \frac{2GM}{c^2} |
KO9 | Tangential speed from angular velocity: linear speed equals radius times angular velocity. | v = r\omega |
KO90 | Gravitational potential: negative GM/r for the potential energy per unit mass. | \Phi = -\frac{GM}{r} |
KO91 | Net force as the vector sum of all forces acting on a body. | \vec{F}_{net} = \sum_i \vec{F}_i |
KO92 | Normal force on an inclined plane proportional to weight times cosine of inclination angle. | \vec{N} = -m\vec{g} \cos\theta |
KO93 | Relativistic momentum with Lorentz factor correction. | p_{93} = \gamma_{3} m v |
KO94 | Static friction inequality: friction force bounded by coefficient of static friction times normal force. | f_s \leq \mu_s N |
KO95 | Hooke's law: restoring force of a spring proportional to displacement. | F_{spring} = -kx |
KO96 | Period of a simple pendulum depending on length and gravitational acceleration. | T = 2\pi\sqrt{\frac{l}{g}} |
KO97 | Damped natural frequency of an oscillator reduced by the damping ratio. | \omega_d = \omega_0\sqrt{1 - \zeta^2} |
KO98 | Damped harmonic oscillator solution with exponential decay and oscillation. | x(t) = A e^{-\zeta\omega_0 t}\cos(\omega_d t + \phi) |
KO99 | Quality factor Q of an oscillator: ratio of stored energy to energy dissipated per cycle. | Q = \frac{\omega_0}{2\zeta\omega_0} = \frac{1}{2\zeta} |
Compute with one of these
curl -sS -X POST https://zeqsdk.com/api/zeq/compute \
-H "Authorization: Bearer $ZEQ_KEY" \
-H "Content-Type: application/json" \
-d '{"operators":["KO1"],"inputs":{}}'
The response carries the bare physics value, its unit and uncertainty, the generated master equation, and a signed envelope you can verify on any node.
See also
- The solvers — how an operator becomes a physical answer
- Operator selection — how a query picks operators
- All categories — the full reference index