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​Lab 2 for Physics PHY201
Simulating a spherical projectile released with an initial velocity of 0 m/s that experiences both forces of gravity and air drag.
PHY201 - Lab #2 - Projectile with Air Drag (V1)
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Uma roda-gigante de raio 14 m gira em torno de um eixo horizontal. Um passageiro sentado em uma cadeira, move-se com velocidade linear v=7 m/s. Determine:

a) a velocidade angular do movimento.

b) gráfico XY do movimento da cadeira.

c) em quanto tempo o passageiro executa uma volta completa.

Clique aqui para ver uma descrição do que é Movimento Circular.

Movimento Circular Uniforme (ñ)
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Based on equations of motion in this paper however this implementation is incorrect; when it is run then:

a) when the pendulum passes past the vertical upright position is does not accelerate downwards but instead starts to decelerate before reversing and going backwards
b) when it is left for some time to run it increases in speed (energy) over time.

Clone from original single pendulum.
Double Pendulum
3 7 months ago
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Simulation of MTBF with controls

F(t) = 1 - e ^ -λt 
Where  
• F(t) is the probability of failure  
• λ is the failure rate in 1/time unit (1/h, for example) 
• t is the observed service life (h, for example)

The inverse curve is the trust time
On the right the increase in failures brings its inverse which is loss of trust and move into suspicion and lack of confidence.
This can be seen in strategic social applications with those who put economy before providing the priorities of the basic living infrastructures for all.

This applies to policies and strategic decisions as well as physical equipment.
A) Equipment wears out through friction and preventive maintenance can increase the useful lifetime, 
B) Policies/working practices/guidelines have to be updated to reflect changes in the external environment and eventually be replaced when for instance a population rises too large (constitutional changes are required to keep pace with evolution, e.g. the concepts of the ancient Greeks, 3000 years ago, who based their thoughts on a small population cannot be applied in 2013 except where populations can be contained into productive working communities with balanced profit and loss centers to ensure sustainability)

Early Life
If we follow the slope from the leftmost start to where it begins to flatten out this can be considered the first period. The first period is characterized by a decreasing failure rate. It is what occurs during the “early life” of a population of units. The weaker units fail leaving a population that is more rigorous.

Useful Life
The next period is the flat bottom portion of the graph. It is called the “useful life” period. Failures occur more in a random sequence during this time. It is difficult to predict which failure mode will occur, but the rate of failures is predictable. Notice the constant slope.  

Wearout
The third period begins at the point where the slope begins to increase and extends to the rightmost end of the graph. This is what happens when units become old and begin to fail at an increasing rate. It is called the “wearout” period. 
BATHTUB MEAN TIME BETWEEN FAILURE (MTBF) RISK
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​Lab 4 for Physics PHY201
Simulating a spherical projectile approaching the speed of light.
PHY201 - Lab #4 - Modeling E = m c^2 (V1)
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Z209 from Hartmut Bossel's System Zoo 1 p112-118. Compare with PCT Example IM-9010

Balancing an Inverted Pendulum
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Satellitenbahn
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How Newton's inverse square law of gravity produces the elliptical orbits of the planets
Planetary orbits
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How gravity and air drag interact to create terminal velocity.
Terminal velocity
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​Lab 2 for Physics PHY201
Simulating a spherical projectile released with an initial velocity of 0 m/s that experiences both forces of gravity and air drag.
PHY201 - Lab 2 - Projectile with Air Drag (V2)
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Attempt to create a very simple decay model for a single radioactive substance.
Radioactive decay
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Barium Produktion und Zerfall
Barium_Produktion_Zerfall
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Maiel Richards Rocket Model 2015
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Pêndulo Amortecido e Forçado
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Josh Doherty's Rocket Model
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Ein- und Ausschaltvorgang bei einer Spule im Gleichstromkreis
Spule_Ein_Aus
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Após uma enchente, um grupo de pessoas ficou ilhado numa região. Um avião de salvamento, voando horizontalmente a uma altura de 720 m e mantendo uma velocidade de v = 50m/s, aproxima-se do local para que um pacote com medicamentos e alimentos seja lançado para as pessoas isoladas. A que distância, na direção horizontal, o pacote deve ser abandonado para que caia junto às pessoas? Despreze a resistência do ar e adote um g = 10m/s².

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 Horizontal no vácuo.

Lançamento Horizontal no vácuo
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Model describing a simple pendulum with exact equation (but without dampening).
Simple pendulum
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Maiel Richards Rocket Model
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Após uma enchente, um grupo de pessoas ficou ilhado numa região. Um avião de salvamento, voando horizontalmente a uma altura de 720 m e mantendo uma velocidade de v = 50m/s, aproxima-se do local para que um pacote com medicamentos e alimentos seja lançado para as pessoas isoladas. A que distância, na direção horizontal, o pacote deve ser abandonado para que caia junto às pessoas? Despreze a resistência do ar e adote um g = 10m/s².

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 Horizontal no vácuo.

Lançamento Horizontal no vácuo (ñ)
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A Fourier series is a way to expand a periodic function in terms of sines and cosines. The Fourier series is named after Joseph Fourier, who introduced the series as he solved for a mathematical way to describe how heat transfers in a metal plate.

The GIFs above show the 8-term Fourier series approximations of the square wave and the sawtooth wave.

Fourier series
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In mathematics, a Lissajous curve /ˈlɪsəʒuː/, also known as Lissajous figure or Bowditch curve /ˈbaʊdɪtʃ/, is the graph of a system of parametric equations{\displaystyle x=A\sin(at+\delta ),\quad y=B\sin(bt),}

which describe complex harmonic motion. This family of curves was investigated by Nathaniel Bowditch in 1815, and later in more detail by Jules Antoine Lissajous in 1857.

Lissajous curve
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Um corpo é atirado verticalmente para cima, a partir do solo, com uma velocidade de 20 m/s. Considerando a aceleração gravitacional 9,8 m/s² e desprezando a resistência do ar, a altura máxima, em metros, alcançada pelo corpo é? 

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 Movimento Vertical no Vácuo.

Clone of Lançamento Vertical no Vácuo
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Magnetómetro 14 10 2021