Final Report - Claymore - Grand Valley State University
Final Report - Claymore - Grand Valley State University
Final Report - Claymore - Grand Valley State University
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where, ω = angular velocity of the launcher motor, τ = torque motor give, J =<br />
mass moment. The state equations above allow us to find the angular velocity the<br />
motor gives. Once angular velocity is found, time is found by<br />
dθ<br />
ω = . (2.3)<br />
dt<br />
Integrate (2.3), and solve for t = time<br />
t = θ / ω<br />
(2.4)<br />
2.1.2<br />
Scilab Calculation for Panning Motor Selection<br />
Figure 2.2: The torque and inertia in a basic motor model<br />
The first-order differential equation can developed from motor properties using<br />
some basic measurements.<br />
Tm = KI<br />
(2.6)<br />
Tm<br />
I = ( 2 .7)<br />
K<br />
where, T = motor torque, K= constant, and I = current. Then consider the<br />
m<br />
power in motor,<br />
P m +<br />
= V I = Tω<br />
KIω<br />
(2.8)<br />
V m = Kω<br />
(2.9)<br />
V m<br />
where, = voltage supply to motor, and P = power. The dynamics of the<br />
rotating masses can be found by summing moments,<br />
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