Mechatronic Design of a Soccer Robot for the Small-Size League of ...
Mechatronic Design of a Soccer Robot for the Small-Size League of ...
Mechatronic Design of a Soccer Robot for the Small-Size League of ...
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Chapter 3: Kicking device<br />
At <strong>the</strong> moment <strong>of</strong> impact, <strong>the</strong> conservation <strong>of</strong> impulse law can be used to<br />
determine <strong>the</strong> velocity after <strong>the</strong> impact.<br />
m plunger v plunger ,t1 + m bal v bal ,t1 = (m plunger + m ball ). v t2 (4.23)<br />
Assuming that <strong>the</strong> velocity <strong>of</strong> <strong>the</strong> ball is zero be<strong>for</strong>e impact:<br />
v t2 = m plunger v plunger ,t1<br />
m plunger + m ball<br />
( 4.24)<br />
v t2 =<br />
m plunger<br />
2. α. F 0 − k. α²<br />
m plunger<br />
m plunger + m ball<br />
(4.25)<br />
C. Accelerating plunger and ball<br />
This calculation is similar to those made in section A. The mass becomes <strong>the</strong><br />
combined mass <strong>of</strong> plunger and ball. Only <strong>the</strong> start conditions <strong>of</strong> <strong>the</strong> differential<br />
equation change. Variable ‘x’ is equal to α at <strong>the</strong> start. The velocity is equal to v t2 at<br />
<strong>the</strong> start and <strong>the</strong> acceleration at <strong>the</strong> start becomes:<br />
F 0 − k. α<br />
m total<br />
x t = α − F 0<br />
k<br />
. cos ωt + v t2<br />
ω . sin ωt + F 0<br />
k<br />
(4.26)<br />
v t = ω. F 0<br />
k − α . sin ωt + v t2. cos(ωt) (4.27)<br />
a t = ω 2 . F 0<br />
k − α . cos ωt − v t2. ω. sin(ωt) (4.28)<br />
31