Physics | Insight Maker

Physics Insight

Jessica Crane

bungee jump

Leonardo Albuquerque Heidemann

3

Masa=Energía

Philipp von Bülow Duden

This shows the motion of a damped harmonic oscillator, described in terms of the undamped natural frequency, and a frequency gamma that reflects the degree of damping, parameterized as a damping ratio gamma/natural frequency. An accurate solution requires a small time step and RK4 as the integration algorithm.

Simple harmonic oscillator with damping 2

Alfredo Louro

5

Z203 from System Zoo 1 p88-90

Bossel: Z203 Brusselator

Alfred Aenishaenslin

Dieses Modell simuliert das Anfahren eines Gelenktriebwagens der Firma Stadler Rail. Mehr dazu im Video "Physik im Jahr 2053"

https://youtu.be/RMOv8A0MvyY

Zugfahrt

Werner Maurer

This shows the motion of a driven damped harmonic oscillator, described in terms of the undamped natural frequency, and a frequency gamma that reflects the degree of damping, parameterized as a damping ratio gamma/natural frequency.

The oscillator is driven with a force that is a sine function of time, with a frequency that can be varied, expressed as a forcing ratio driving frequency/natural frequency.

An accurate solution requires a small time step and RK4 as the integration algorithm.

Clone of Driven damped oscillator

luis gomez

Spring-Mass-Damper model (based on IACS physics)

Spring-Mass-Damper Model

Egbert Ypma

Clone of Conducción térmica 5x5

Philipp von Bülow Duden

Z212 from System Zoo 1 p142-148

Clone of House Heating Dynamics

Igor Krejčí

Oscillator with limit cycle from Z202 System Zoo 1 p84-87

Bossel: Z202 Van der Pol Oscillator

Alfred Aenishaenslin

Clone of Wind Resistance Model

Tristan Robitaille

Nur Zerfall

Bariumzerfall

Prof. Dr. Horst Schecker

Problem of the sliding chain

Clone of Sliding Chain

Laurence Fournier

Grundmodell der Newtonschen Mechanik angewendet auf den Fall mit Luftreibung (z.B. Fallschirmspringen)

Clone of Fall_mit_Luftreibung

Bobby

Um corpo é lançado obliquamente no vácuo com velocidade inicial de 100 m/s, numa direção que forma com a horizontal um ângulo x, tal que sen(x) = 0,8 e cos(x) = 0,6. Adotando g = 10m/s², determine:

a) Os módulos das componentes horizontal e vertical da velocidade no instante de lançamento;

b) O instante em que o corpo atinge o ponto mais alto da trajetória;

c) A altura máxima atingida pelo corpo;

d) O alcance do lançamento.

Fonte: (RAMALHO, NICOLAU E TOLEDO;Fundamentos da Física, Volume 1, 8ª edição, pp. 12 – 169, 2003).

Clique aqui para ver uma descrição do que é Lançamento Oblíquo no vácuo.

Lançamento Oblíquo no vácuo (ñ)