Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Net Torque Calculations01:19

Net Torque Calculations

9.0K
When a mechanic tries to remove a hex nut with a wrench, it is easier if the force is applied at the farthest end of the wrench handle. The lever arm is the distance from the pivot point (the hex nut in this case) to the person’s hand. If this distance is large, the torque is higher. Only the component of the force perpendicular to the lever arm contributes to the torque. Therefore, pushing the wrench perpendicular to the lever arm is more advantageous. If multiple people apply force to...
9.0K
Kinematic Equations: Problem Solving01:15

Kinematic Equations: Problem Solving

11.8K
When analyzing one-dimensional motion with constant acceleration, the problem-solving strategy involves identifying the known quantities and choosing the appropriate kinematic equations to solve for the unknowns. Either one or two kinematic equations are needed to solve for the unknowns, depending on the known and unknown quantities. Generally, the number of equations required is the same as the number of unknown quantities in the given example. Two-body pursuit problems always require two...
11.8K
Kinematic Equations - II01:17

Kinematic Equations - II

9.3K
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...
9.3K
Kinematic Equations - III01:18

Kinematic Equations - III

7.4K
The first two kinematic equations have time as a variable, but the third kinematic equation is independent of time. This equation expresses final velocity as a function of the acceleration and distance over which it acts. The fourth kinematic equation does not have an acceleration term and provides the final position of the object at time t in terms of the initial and final velocities. This equation is useful when the value of the constant acceleration is unknown.
Using the kinematic equations,...
7.4K
Kinematic Equations - I01:26

Kinematic Equations - I

10.3K
When an object moves with constant acceleration, the velocity of the object changes at a constant rate throughout the motion. The kinematic equations of motions are derived for such cases where the acceleration of the object is constant. The first kinematic equation gives an insight into the relationship between velocity, acceleration, and time. We can see, for example:
10.3K
Three-Dimensional Force System01:30

Three-Dimensional Force System

2.0K
In mechanical engineering, a three-dimensional force system is a system of forces acting in three dimensions, with forces applied along the x, y, and z coordinate axes. The three-dimensional force system is an important concept in mechanical engineering, as it allows engineers to understand and analyze the behavior of objects and structures in three dimensions. By understanding the forces acting on a system, engineers can design more efficient and effective mechanical systems that can withstand...
2.0K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Canned seafood as a potential source of microplastics exposure with taxon-specific partitioning and packaging-derived contamination.

Environmental pollution (Barking, Essex : 1987)·2026
Same author

Air-to-ground channel dataset via UAV-aided measurements in multiple scenarios.

Data in brief·2025
Same author

Optical pulse subtractor for fiber neural networks.

Applied optics·2025
Same author

Broadband stepped-frequency radar waveform generation by Fourier domain mode-locking period-one laser dynamics.

Optics letters·2024
Same author

Integrated bioinformatics and multiomics reveal Liupao tea extract alleviating NAFLD via regulating hepatic lipid metabolism and gut microbiota.

Phytomedicine : international journal of phytotherapy and phytopharmacology·2024
Same author

Oleanolic Acid Promotes the Formation of Probiotic <i>Escherichia coli</i> Nissle 1917 (EcN) Biofilm by Inhibiting Bacterial Motility.

Microorganisms·2024

Related Experiment Video

Updated: May 30, 2025

Computational Modeling of Retinal Neurons for Visual Prosthesis Research - Fundamental Approaches
10:50

Computational Modeling of Retinal Neurons for Visual Prosthesis Research - Fundamental Approaches

Published on: June 21, 2022

1.7K

Fiber transmission model with parameterized inputs based on generative pre-trained physics-informed neural networks.

Yubin Zang, Boyu Hua, Zhipeng Lin

    Optics Express
    |January 29, 2025
    PubMed
    Summary
    This summary is machine-generated.

    A new principle-driven fiber transmission model offers efficient, universal solutions for short-distance optical communication. It achieves high accuracy without retraining for different bit rates or pre-collected data.

    More Related Videos

    Author Spotlight: Development of an Automated Camera-Based System for Real-Time Blast Overpressure Monitoring and TBI Risk Assessment in Military Training
    06:20

    Author Spotlight: Development of an Automated Camera-Based System for Real-Time Blast Overpressure Monitoring and TBI Risk Assessment in Military Training

    Published on: December 6, 2024

    2.4K
    Targeting Neuronal Fiber Tracts for Deep Brain Stimulation Therapy Using Interactive, Patient-Specific Models
    14:14

    Targeting Neuronal Fiber Tracts for Deep Brain Stimulation Therapy Using Interactive, Patient-Specific Models

    Published on: August 12, 2018

    8.8K

    Related Experiment Videos

    Last Updated: May 30, 2025

    Computational Modeling of Retinal Neurons for Visual Prosthesis Research - Fundamental Approaches
    10:50

    Computational Modeling of Retinal Neurons for Visual Prosthesis Research - Fundamental Approaches

    Published on: June 21, 2022

    1.7K
    Author Spotlight: Development of an Automated Camera-Based System for Real-Time Blast Overpressure Monitoring and TBI Risk Assessment in Military Training
    06:20

    Author Spotlight: Development of an Automated Camera-Based System for Real-Time Blast Overpressure Monitoring and TBI Risk Assessment in Military Training

    Published on: December 6, 2024

    2.4K
    Targeting Neuronal Fiber Tracts for Deep Brain Stimulation Therapy Using Interactive, Patient-Specific Models
    14:14

    Targeting Neuronal Fiber Tracts for Deep Brain Stimulation Therapy Using Interactive, Patient-Specific Models

    Published on: August 12, 2018

    8.8K

    Area of Science:

    • Optical Communications
    • Computational Physics
    • Signal Processing

    Background:

    • Accurate modeling of fiber optic transmission is crucial for high-speed data communication.
    • Existing models often require extensive retraining for varying transmission parameters.
    • Developing computationally efficient and physically grounded models remains a challenge.

    Purpose of the Study:

    • To introduce a principle-driven fiber transmission model for short-distance communication.
    • To enable universal solutions for diverse bit rates without model re-training.
    • To enhance computational efficiency and physical interpretability in optical modeling.

    Main Methods:

    • Utilized a previously proposed principle-driven fiber model as the core solver.
    • Applied the reduced basis expansion method for efficient computation.
    • Transformed parameterized inputs into coefficients for the Nonlinear Schrödinger Equations.

    Main Results:

    • Achieved universal solutions for various bit rates by parameterizing model coefficients.
    • Demonstrated prominent advantages in computational efficiency and physical background.
    • Successfully trained the model without requiring pre-collected transmitted signals.
    • Validated model fidelity using on-off keying and pulse amplitude modulated signals over 100 km.

    Conclusions:

    • The developed model provides an efficient and versatile approach for short-distance fiber transmission.
    • It offers significant computational savings and retains strong physical grounding.
    • The model's ability to train without prior signal data enhances its practical applicability.