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10. Satelliet om aarde
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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
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Clone of Homework 9/16
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Z205 from System Zoo 1 p95-98

Clone of Chaotic Bistable Oscillator
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Problem of the sliding chain
Clone of Sliding Chain
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Buenos Dias, Goeden dag, Guten Tag, Muraho, Jasas, Sabadi Kap, Bonjour, Buongiourno, Good day
Clone of Clone of eenparige worp in twee dimensies
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Buenos Dias, Goeden dag, Guten Tag, Muraho, Jasas, Sabadi Kap, Bonjour, Buongiourno, Good day
Clone of Clone of eenparige worp in twee dimensies
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Clone of Wind Resistance Model
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Z207 from Hartmut Bossel System Zoo 1 p103-107


After running the default settings Bossel describes A=0.2, B=0.2, Initial Values X=0 Y=2 and Z=0 and varying C=2,3,4,5 shows period doubling and transition to chaotic behavior
Rossler Chaotic Attractor
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Clone of Bomba de golpe de Ariete 06 08 2022
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Dynamics Model Skydiver
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Oscillator with limit cycle from Z202 System Zoo 1 p84-87
Clone of Van der Pol Oscillator
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Bipolar II treatment modeling using Van der Pol-like oscillators.

In this simulation an afflicted individual with Bipolar II disorder is put to treatment after 20 months the calibration of the medicine or treatment he recieves is such that it simulates the natural cycles of a "normal being". You can note by manipulating the parameters that sometimes too much treatment disrupts equilibria. Also note that in the state diagrams there are 2 limit cycles, the lower one being the healthiest as there are less changes.
Bipolar II dynamics
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L'idée est de simuler le fonctionnement d'un siphon (vidange brusque d'un réservoir lorsqu'un certain seuil est atteint). Le flux de remplissage est basé sur une sinusoïde dont on peut régler l'amplitude et la fréquence (seule la partie positive de l'oscillation est utilisée).

Dans un second temps, nous utiliserons ensuite l'idée du siphon pour construire un circuit logique hydraulique non trivial (en l'occurrence un additionneur).
Simulation d'un siphon
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Nuclear Decay Chain
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5. Lanceren van een raket in 1 dimensie
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Clone of Wind Resistance Model
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Simulating soil temperature profile.

'Tm' is the annual surface mean temperature. 'delta T' is the annual variation in surface temperature. 'Te' is the long term equilibrium temperature at depth.

Seasonal Heat Flow into Surface of Earth
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Problem of the sliding chain
Clone of Sliding Chain
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Problem of the sliding chain
Clone of Sliding Chain
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Work in progress. Simulating soil temperature profile.

Heat Flow into Surface of Earth (no atmosphere)
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Nik Vieira's Rocket Model
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NOT YET FUNCTIONAL

This is a simple energy balance model of radiation through the atmosphere. It's a simple single layer model.

Version 2 of Greenhouse Effect in the Atmsophere
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Practicum Paris Gun