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Gynkana atmosférica_Paracaídas - Contenido educativo

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Subido el 20 de marzo de 2023 por Maria Jesús T.

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Diseño de paracaídas para un CanSat

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Welcome to CANSAT EVA 00:00:00
Let's talk about parachute design. 00:00:11
Parachutes are vital parts of any CANSAT mission. 00:00:17
They are often regarded as simple pieces of public compared to the complex electronics that lies within the CANSAT. 00:00:24
But that's a big mistake. 00:00:34
Without a well-designed parachute, your concept might not have time to complete its scientific 00:00:36
objective, or rather yet, it could crash land. 00:00:44
As in any other engineering project, our concept must meet some specific requirements, such 00:00:50
such as the size, mass and even more important, the concept's design speed must not be lower 00:00:59
than 5 ms or higher than 12 ms for safety reasons. 00:01:09
For recovery reasons, a maximum flight time of 120 seconds is recommended. 00:01:18
Without a well-designed parachute, these requirements cannot be met. 00:01:25
Let's try to understand our design equation. 00:01:35
First, we are going to draw the free-body diagram to analyse all the forces acting on 00:01:39
our contact. 00:01:47
The two main forces acting on it are the weight due to gravity and the drag force due to the 00:01:49
resistance. Combining these equations and considering Newton's laws, we can get to 00:01:58
the design equation. In the fall, the cansat is dropped, then the initial 00:02:05
velocity is zero and the only force acting on it is gravity. As it falls, the 00:02:13
velocity increases and the drag force increases as well. Finally, both forces 00:02:19
are balanced and the terminal velocity is reached. From this point on the cancels 00:02:28
will form at a steady rate. Combining these forces we reach to the design 00:02:35
equation where A is the canopy surface area equals 2 times the mass times the 00:02:45
acceleration of gravity divided by the product of the air density, zv, the drag 00:02:55
coefficient and the square terminal velocity. Canopy surface area can be 00:03:03
changed by making the parachute smaller or larger and the drag coefficient can be 00:03:09
changed using a different style of parachute. Drag coefficients are 00:03:16
are determined experimentally. We are going to design a flat octagon parachute. 00:03:23
Applying several geometric equations, we can reach to the length and the height needed 00:03:34
to draw a template of the triangles. With the 8 triangles joined together, the complete 00:03:43
template of the flat octagon is ready to be used but there is an easier way to 00:03:52
get our parachute ready. We will show you how to do it using a little bag. The first 00:04:01
step is to fold it in half so that you will make a square. Cut the remaining 00:04:13
part to get a complete triangle so with a square fold it in twice in half fold it again and again 00:04:22
and then cut it so you have a triangle cut the tip to make the spill and there it is your canopy 00:04:41
is ready. Cut a piece of thread. Join the thread to the corners of the canopy using 00:04:55
fellow tape. Do the same with the other three pieces of thread. Congratulations! 00:05:06
your parachute is now ready 00:05:18
Idioma/s:
en
Autor/es:
María Tamés Esteban
Subido por:
Maria Jesús T.
Licencia:
Reconocimiento - No comercial - Compartir igual
Visualizaciones:
35
Fecha:
20 de marzo de 2023 - 9:08
Visibilidad:
Público
Enlace Relacionado:
https://esamultimedia.esa.int/docs/edu/T10_Parachute_Design.pdf
Centro:
IES PRINCIPE FELIPE
Duración:
05′ 40″
Relación de aspecto:
1.78:1
Resolución:
1920x1080 píxeles
Tamaño:
126.90 MBytes

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