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22.322 Mechanical Design II. Spring 2013. Summary. Lectures 1-4. A cam converts one motion into another form A follower follows the cam profile. Think of a cam-follower system as a linkage with variable-length “effective” links Become familiar with basic cam terminology: - PowerPoint PPT Presentation
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Learning with Purpose February 1, 2013Learning with Purpose February 1, 2013
22.322 Mechanical Design II
Spring 2013
Learning with Purpose February 1, 2013
A cam converts one motion into another formA follower follows the cam profile
Summary
Lectures 1-4
Think of a cam-follower system as a linkage with variable-length “effective” linksBecome familiar with basic cam terminology:• Translating vs. rotating
followers• Follower types:
• Flat-faced• Roller• Knife-edge• Curved
Learning with Purpose February 1, 2013
Follower displacement curves: • Rise, dwell, return/fall
Graphical Design• Based on a displacement curve, generate the cam contour (HW #1)• Understand what these are:
• Base Circle• Pressure Angle• Pitch Point• Throw/stroke/travel
• Start with your base circle,divide it into q intervalsaccording to displacementcurve, plot thecorresponding points, maketangent lines and drawcam contour tangent tothose lines
Summary
Lectures 1-4
Learning with Purpose February 1, 2013
Summary
HW #1 Solution
Learning with Purpose February 1, 2013
SVAJ Diagrams (HW #2)• When designing a cam-follower system, consider the higher derivatives of displacement• Satisfy the Fundamental Law of Cam Design
• s, v, a must be continuous • j must be finite
SCCA Family of Functions• Acceleration curves that will change
the peak magnitude of velocity, acceleration, jerk
• Curves are defined by the same set ofequations but by varying parametersand coefficients• Don’t worry about the derivation of those
equations/parameters programs likeDYNACAM do that for you!
• Different values lead to different curvesdepending on the design specifications
e.g. modified sine acceleration functionleads to a low peak velocityIf the follower mass is large, you want tominimize its velocity
Summary
Lectures 1-4
Learning with Purpose February 1, 2013
Kloomok and Muffley method of combining displacement curves
Summary
Lectures 1-4
Learning with Purpose February 1, 2013
Summary
C-1
H-2P-2
Learning with Purpose February 1, 2013
Lecture 5
Polynomial Functions
The general form of a polynomial function is:
s = Co + C1x + C2x2 + C3x3 + C4x4 + … + Cnxn
where s is the follower displacement, x is the independent variable (q/b or time t)
C coefficients are unknown and depend on design specificationThe number of terms in the polynomial will be equal to the number of boundary conditions on the s v a j diagrams.
Learning with Purpose February 1, 2013
Lecture 5
For the double-dwell problem, we can define six BCs:
Since we have 6 BCs, we need a polynomial with 6 coefficients:
Differentiate with respect to q to get V and a:
Now we can apply the BC’s to solve for C0, C1, C2, C3, C4, C5
Learning with Purpose February 1, 2013
Lecture 5
We now have 3 equations and 3 unknowns and can solve for the unknown coefficients!
Learning with Purpose February 1, 2013
Lecture 5
𝑠=h[10 (𝜃𝛽 )3
−15( 𝜃𝛽 )4
+6 (𝜃𝛽 )5]
This is called a 3-4-5 polynomial because of the exponents
Velocity and acceleration are continuous but jerk is not it was left unconstrained.
In order to constrain the jerk, we need to add two additional coefficients, C6 and C7, and use two more BCs:
Learning with Purpose February 1, 2013
Lecture 5
If we repeat the same analysis but add the two extra BCs and coefficients, we will result in the following 4-5-6-7 polynomial for the displacement function:
This 4-5-6-7 polynomial will have a smoother jerk but a higher acceleration than the 3-4-5 polynomial.
Learning with Purpose February 1, 2013
Many applications require a single dwell cam profile (rise-fall-dwell)Example: the cam that opens valves in an engine The valve opens on the rise, closes on the return, and remains shut while combustion and compression take place.The cam profiles for the double dwell case may work but will not be optimal (e.g. cycloidal displacement)
Lecture 5
Single-Dwell Cams
Acceleration is negative in rise and fall regions…why go to 0?
Subsequently leads to discontinuous jerk
Learning with Purpose February 1, 2013
Although the jerk is finite, it is discontinuous. A better approach is to use the double harmonic function.
Lecture 5
Single-Dwell Cams
Double harmonic should never be used for double-dwell case non-zero acceleration at one end of interval.
Learning with Purpose February 1, 2013
If we used a polynomial function to design the single dwell cam, we could use only one function to describe the rise and the return. The BC’s are:
With 7 BC’s, we need 7 coefficients. If we solve as we have previously, the function turns out to be a 3-4-5-6 polynomial:
Lecture 5
Single-Dwell Cams
𝑠=h[64 ( 𝜃𝛽 )3
−192 (𝜃𝛽 )4
+192( 𝜃𝛽 )5
−64( 𝜃𝛽 )6]
Learning with Purpose February 1, 2013
Note that the acceleration is reduced compared to the double harmonic, but the jerk is discontinuous at the ends.We could have also set but that would increase the order of the polynomial by two.
Lecture 5
Single-Dwell Cams
A high-degree function may have undesirable oscillations between its BCs!