Related Experiment Video
Updated: Nov 2, 2025

11:51
Visually Based Characterization of the Incipient Particle Motion in Regular Substrates: From Laminar to Turbulent Conditions
Published on: February 22, 2018
8.9K
Kinetic uncertainty relation on first-passage time for accumulated current
1Department of Physics, Kyoto University, Kyoto 606-8502, Japan.
Physical Review. E
|June 17, 2021
Summary
We derived a kinetic uncertainty relation for first passage time, showing precision is limited by the number of system jumps. This provides a tighter bound than existing relations, especially far from equilibrium.
Area of Science:
- Statistical Mechanics
- Information Theory
- Stochastic Processes
Background:
- The kinetic uncertainty relation (KUR) quantifies trade-offs between measurement precision and dynamical activity in Markov chains.
- Existing KURs apply to fixed time intervals and homogeneous systems.
Purpose of the Study:
- Derive a KUR for first passage time (FPT) of integrated current.
- Establish a bound on FPT precision based on system activity.
Main Methods:
- Utilized information inequalities at stopping times.
- Applied the derived KUR to simple systems.
Main Results:
- Established a KUR for FPT, bounding precision by the mean number of jumps.
- Demonstrated tighter bounds compared to the thermodynamic uncertainty relation in non-equilibrium regimes.
Conclusions:
- The derived KUR offers a more refined constraint on FPT precision.
- This finding has implications for understanding non-equilibrium systems and information processing.
Related Concept Videos
The Uncertainty Principle
29.3K
Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He...
29.3K
Kinematic Equations - II
11.9K
The second kinematic equation expresses the final position of an object in terms of its initial position, the distance traveled with the initial constant velocity, and the distance traveled due to a change in velocity. Similar to the first kinematic equation, this equation is also only valid when the acceleration is constant throughout the motion of an object.
Suppose a car merges into freeway traffic on a 200 m long ramp. If its initial velocity is 10 m/s and it accelerates at 2 m/s2, then the...
Suppose a car merges into freeway traffic on a 200 m long ramp. If its initial velocity is 10 m/s and it accelerates at 2 m/s2, then the...
11.9K
Ampere-Maxwell's Law: Problem-Solving
856
A parallel-plate capacitor with capacitance C, whose plates have area A and separation distance d, is connected to a resistor R and a battery of voltage V. The current starts to flow at t = 0. What is the displacement current between the capacitor plates at time t? From the properties of the capacitor, what is the corresponding real current?
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
856
Continuity Equation
1.1K
The total amount of current flowing per unit cross-sectional area is called the current density. Hence, the current passing through a cross-sectional area can be written as the surface integral of the current density.
1.1K
Continuity Equation
2.9K
The continuity equation asserts that the mass flow rate must remain constant for a steady flow of an incompressible fluid within a confined system. This principle applies to systems where fluid passes through varying cross-sectional areas, such as nozzles, syringes, and pipes.
The mass flow rate is expressed as:
The mass flow rate is expressed as:
2.9K
Displacement Current
3.3K
Ampère's law, in its usual form, does not work in places where the current changes with time and is not steady. Thus, Maxwell suggested including an additional contribution, called the displacement current, Id, to the real conduction current I.
3.3K

