Motion Taking Resistance into Account
Author: shiroeExecutions: 6
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The input range for θ is from 0 to π/2 (in radians).
If t > 0 and y < 0, the calculation is terminated.
The input range for “Resistance” is 0 or greater.
(Resistance coefficient / Mass)
Example value for g: g=9.8
Example time step: 0.1
Example resistance input: 0.7
Example v input: 222
Example θ input: pi/4
(pi/4=90 degrees)
Reference: 1 [m/s] = 360 [m/h]
Reference: 1 [km/h] = 2.777… [m/s]
Reference: 80 [km/h] = 222.222… [m/s]
Reference: 150 [km/h] = 416.666… [m/s]
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Digit display set to 6 digits. Digit count can be changed. Real number calculation mode.
If t > 0 and y < 0, the calculation is terminated.
The input range for “Resistance” is 0 or greater.
(Resistance coefficient / Mass)
Example value for g: g=9.8
Example time step: 0.1
Example resistance input: 0.7
Example v input: 222
Example θ input: pi/4
(pi/4=90 degrees)
Reference: 1 [m/s] = 360 [m/h]
Reference: 1 [km/h] = 2.777… [m/s]
Reference: 80 [km/h] = 222.222… [m/s]
Reference: 150 [km/h] = 416.666… [m/s]
----------------------------------------------------------------------
Digit display set to 6 digits. Digit count can be changed. Real number calculation mode.
No customer feedback for this calculation yet.
Consider the x-y plane. The x-axis is horizontal, the y-axis is vertical,
the magnitude of gravitational acceleration is g, and the y=-∞ side is defined as “down.”
An object starts at the origin (0,0) with an initial velocity, which we denote as v.
Let θ be the angle at which the object is “thrown.”
We consider cases where “drag” (drag coefficient divided by mass) acts in the opposite direction of velocity and its magnitude is proportional to velocity.