Group B Tedros Ghebretnsae Xinyan Li Zhen Yu Tang Ankit Panwar
Mar 26, 2015
Group BTedros Ghebretnsae
Xinyan LiZhen Yu TangAnkit Panwar
Design a fourbar to move from point A to B Point B is at a height, H=6R,4R,2R Single motor drives the input crank Preferable a Grashoff crank rocker or double
crank The Chassis is fixed What is required from the motor• Compactness• Dynamically well behaved
Links: Aluminum T6061Area of each link: 1 cm2
Weight of wheel: 1 kg
Two most important constraints were:• the ground link had to lie inside the chassis• the lower arm should travel from without
colliding with the step. First choice was whether to synthesize the
mechanism for two or three points. The main advantage for the two point
mechanism was that there were more free choices.
Whereas with the three point, there was a better control
This was the first method employed by us. Total variables: 18, total equations: 12 The free choices were α2 , α3 , β2 , β3 , γ2
and γ3
The problems with this method:• no constraints on the ground link• the arms were colliding with the step• None of the solutions satisfied our design
requirements
Next we employed the same technique but with fixed ground.
The values of the betas (α2 and α3 for the upper blue link, β2 and β3 for the lower black link) were found first
The known variables were the ground link and the coupler angles γ2 and γ.
We were able to get the solution for all the three points which satisfied the design requirements.
0 5 10 15 200
2
4
6
8
10
12
14
16
18
20
0 5 10 15 200
2
4
6
8
10
12
14
16
18
20
0 5 10 15 200
2
4
6
8
10
12
14
16
18
20
The problem with this method was that the arm moves from point one to point two, but fails to trace the last point.
The reason why this method fails is that it does not always guarantee that the fourbar will pass through all the three points
The plot shows the same fourbar mechanism but in the crossed configuration
Whereas the previous plots were for the uncrossed configuration
Total variables: 14, total equations: 8 The free choices were C, S (this is the part extended
beyond the joint of U and C), β2, γ2 and γ3
-1 -0.5 0 0.5 1 1.5 2-1
-0.5
0
0.5
1
1.5
2
Steps taken:• Determination of Position, Velocity and
acceleration of all the center of masses and also that of the wheel
• Formulation of Torque versus input Theta 2• Plotting Torque versus Theta 2 using Matlab for
different height H(6R, 4R and 2R)• Analyze the plotted Torque and • Determine and select the feasible one for the
given mechanism size and orientation
0 50 100 150 200 250 300 350-100
-80
-60
-40
-20
0
20
40
60
80
100
theta2
Tor
que
actin
g at
link
2
0 50 100 150 200 250 300 350-100
-80
-60
-40
-20
0
20
40
60
80
100
theta2
Tor
que
actin
g at
link
2
For heights 4R and 2R The Torque seems to stabilize for theta
greater than 100 For those values of theta, it was managed
to lower the Torque to little more than zero value which in turn means less work is needed to do the task, and hence a small Motor would work
For height equal to 6R Unstable torque. There is a lot of fluctuation in magnitude
and direction There is a big range between max and min
valuesTheta2 values Values between 50 and 100 resulted in
great fluctuation of the torque with extreme high values and lack of stability