VEHICULAR SHAFT FOR POWER TRANSMISSION DESIGN

advertisement
VEHICULAR SHAFT
FOR POWER
TRANSMISSION
DESIGN PROJECT
MEC 410: Design of Machine Elements
Kanchan Bhattacharyya
Jackie Chen
Matthew Stevens
Han John Tse
Known Information:
1. Purpose: Power Transmission w/ Diff. Speed Ratios
2. Shaft Material: Stainless Steels (Many Types)
3. Known Dimensions:
Figure 1. Initial Design Sketch With Proposed Dimensions
4. Rotational load is considered sinusoidal with cyclic dynamic loading
5. Peak load 10,000 N @ frequency = 100 Hz, Design Safety Factor = 3.0
Design Objectives:
1. Determining Endurance Limit
2. Stress Concentration Reduction (With FEA Visualizations)
3. Machine Keyway Width & Height Selection
4. Final CAD Drawing
1
I.
Determining Endurance Limit:
Endurance Limit Considerations
a. Considering AISI 304 Stainless Steel with 𝑆𝑒𝑑 = 73.2 π‘˜π‘π‘ π‘–
(choice pre-determined from fillet radii calculations in section III.)
The Rotary-Beam Endurance Limit: 𝑆𝑒′ = 0.5𝑆𝑒𝑑 = 36.6 π‘˜π‘π‘ π‘–
Considering Modification Factors;
Surface Factor: π‘˜π‘Ž = π‘Žπ‘†π‘’π‘‘ 𝑏 considering a machined surface; π‘Ž = 2.70, 𝑏 = −0.265
Then π‘˜π‘Ž = (2.70)(73.2 π‘˜π‘π‘ π‘–)−0.265 = 0.8655
Size Factor: Consider diameter d = 0.2m = 7.87 in; π‘˜π‘ = 0.91𝑑−0.157 = 0.658
*Note that the main diameter is d (the one with the key-way)
Loading Factor: For combined bending and torsion experienced by the shaft, we let π‘˜π‘ = 1
Temperature Factor: Neglecting extreme temperature conditions, let π‘˜π‘‘ = 1
Reliability Factor: Assume a relatively high degree of reliability, and a reliability goal of 99%,
π‘˜π‘’ = 0.814
Miscellaneous Factors: Assume π‘˜π‘’ = 1
Then, the endurance limit at the critical locations becomes
𝑆𝑒 = π‘˜π‘Ž π‘˜π‘ π‘˜π‘ π‘˜π‘‘ π‘˜π‘’ π‘˜π‘“ 𝑆𝑒 ′
= (0.8655)(0.658)(1)(1)(0.814)(1)(36.6)
= πŸπŸ”. πŸ—πŸ” π’Œπ’‘π’”π’Š
2
II.
Stress Concentration Reduction
A. Where are the highest stresses present? (Analytical)
Figure 2. Main Shaft Diameter w/ Keyway FBD:
Given: π‘ƒπ‘’π‘Žπ‘˜ π‘‡π‘Ÿπ‘Žπ‘›π‘ π‘šπ‘–π‘‘π‘‘π‘’π‘‘ πΏπ‘œπ‘Žπ‘‘ 𝐹𝑇 = 10,000 𝑁
Solving for Reaction Forces:
𝐹𝑇
𝐹𝑅 =
= 10,641.78 𝑁
cos(20°)
𝐹𝑁 = sin(𝐹𝑅 ) = 3,639.7 𝑁
𝐹𝑁
π‘…π‘’π‘Žπ‘π‘‘π‘–π‘œπ‘› πΉπ‘œπ‘Ÿπ‘π‘’π‘  𝑖𝑛 π‘₯𝑦 π‘π‘™π‘Žπ‘›π‘’ =
= 1819.85 𝑁
2
𝐹
π‘…π‘’π‘Žπ‘π‘‘π‘–π‘œπ‘› πΉπ‘œπ‘Ÿπ‘π‘’π‘  𝑖𝑛 π‘₯𝑧 π‘π‘™π‘Žπ‘›π‘’ = 𝑇 = 5,000 𝑁
2
*Note: Middle of Bearing O taken as “zero” for XY Plot; Range of Plots are from Bearing to Bearing.
Figure 3. XY Plane FBD:
Figure 4. XY Plane Shear Diagram:
Figure 5. XY Plane Bending Moment Diagram:
XY Shear:
0 ≤ π‘₯ ≤ 0. 45 π‘š → 𝑉 = 1819.85 𝑁
0.45 π‘š < π‘₯ ≤ 0.90 π‘š → 𝑉 = −1819.85 𝑁
XY Bending: (“Key” M values @ middle of shaft segments)
π΅π‘’π‘Žπ‘Ÿπ‘–π‘›π‘” 𝑂: π‘₯ = 0. 05 π‘š → 𝑀 = 90.9975 𝑁 π‘š
𝐿𝑒𝑓𝑑/π‘…π‘–π‘”β„Žπ‘‘ π‘†β„Žπ‘Žπ‘“π‘‘: π‘₯ = 0.215; 0.685 π‘š
→ 𝑀 = 454.9625 𝑁 π‘š
π‘ͺ𝒆𝒏𝒕𝒆𝒓 𝑺𝒉𝒂𝒇𝒕: 𝒙 = 𝟎. πŸ’πŸ“ π’Ž → 𝑴 = πŸ–πŸπŸ–. πŸ–πŸ— 𝑡 π’Ž
π‘…π‘–π‘”β„Žπ‘‘ π‘†β„Žπ‘Žπ‘“π‘‘: π‘₯ = 0.685 π‘š → 𝑀 = 454.9625 𝑁 π‘š
3
Figure 6. XZ Plane FBD:
Figure 7. XZ Plane Shear Diagram:
Figure 8. XZ Plane Bending Moment Diagram:
XY Shear:
0 ≤ π‘₯ ≤ 0. 45 π‘š → 𝑉 = 5,000 𝑁
XY Bending:
0.45 π‘š < π‘₯ ≤ 0.90 π‘š → 𝑉 = −5,000 𝑁
π΅π‘’π‘Žπ‘Ÿπ‘–π‘›π‘” 𝑂: π‘₯ = 0. 05 π‘š → 𝑀 = 250 𝑁 π‘š
𝐿𝑒𝑓𝑑/π‘…π‘–π‘”β„Žπ‘‘π‘†β„Žπ‘Žπ‘“π‘‘: π‘₯ = 0.250; 0.650 π‘š
→ 𝑀 = 1250 𝑁 π‘š
π‘ͺ𝒆𝒏𝒕𝒆𝒓 𝑺𝒉𝒂𝒇𝒕: 𝒙 = 𝟎. πŸ’πŸ“ π’Ž → 𝑴 = πŸπŸπŸ“πŸŽ 𝑡 π’Ž
Stress Calculations:
Stresses can be calculated using moments from critical points found in the shear-moment diagrams
and these relations:
𝑀𝑐
πœ‹π‘‘ 4
πœŽπ‘Ž =
;𝐼=
;𝜎 = 0
𝐼
64 π‘š
π‘‡π‘Ÿ
πœ‹π‘‘4
πœπ‘š =
;𝐽=
; πœπ‘Ž = 0
𝐽
32
XY PLANE NORMAL STRESSES: (AT EACH SHOULDER FROM LEFT TO RIGHT)
𝜎1 = 7,414,735.9 π‘ƒπ‘Ž
𝜎2 = 4,634,201.0 π‘ƒπ‘Ž
𝜎3 = 1,042,694.1 π‘ƒπ‘Ž
XZ PLANE NORMAL STRESSES: (AT EACH SHOULDER FROM LEFT TO RIGHT)
𝜎1 = 20,371,832.7 π‘ƒπ‘Ž
𝜎2 = 12,737,395.5 π‘ƒπ‘Ž
𝜎3 = 2,864,789.0 π‘ƒπ‘Ž
The resultant stress at shoulder 1 is clearly going to be largest:
πœŽπ‘  = 𝜎1 2 + 𝜎2 2
πˆπ’”πŸ = 𝟐𝟏, πŸ”πŸ•πŸ—, πŸπŸ“πŸŽ 𝑷𝒂
SHEAR STRESSES:
Shoulder 1:
π‰π’”πŸ = 𝟐𝟎, πŸ‘πŸ•πŸ, πŸ–πŸ‘πŸ‘ 𝑷𝒂
Shoulder 2:
πœπ‘ 2 = 2,546,479 π‘ƒπ‘Ž
REVISITING Q: Where are the highest stresses present?
ANSWER: Local stress maximums at shoulders 1, 2, and 3, with the highest absolute stresses at shoulder
1 with πˆπ’”πŸ = 𝟐𝟏, πŸ”πŸ•πŸ—, πŸπŸ“πŸŽ 𝑷𝒂 and πœπ‘ 1 = 𝟐𝟎, πŸ‘πŸ•πŸ, πŸ–πŸ‘πŸ‘ 𝑷𝒂.
4
B. Where are the highest stresses? (FEA Visualization)
Figure 9. Snapshots of FEA simulations shown prior to shoulder modification via fillets to reduce stress
concentrations; Top Left shows displacement in mm; Top Right shows strain in mm/mm; Bottom Center
shows Von Mises Stresses in MPa. General color coding scheme is blue οƒ  sky blue οƒ  green οƒ  yellow οƒ  red
from lowest to highest values for given quantities.
-
-
-
-
Note that transition from bearing to left shaft at Shoulder 1 and from left shaft to center shaft at
Shoulder 2 both exhibit a transition from the sky blue to a localized green in both strain and vonmises stresses. For the displacement, it happens to be a blue to green transition for Shoulder 1
and a yellow to orange transition for Shoulder 2. The actual colors are magnitude dependent but
the important thing to notice is that it can be visually confirmed that the shoulders bear the
most localized stress while stresses within shaft segments are relatively uniform. These
shoulders therefore become the main area to reduce stress concentrations.
C. Choosing Fillet Radii for Shoulder 1 (between bearing and left shaft) and Shoulder 2 (between left
and center shaft) to reduce stress concentrations:
Fillet radii can either be determined by choosing a material and using its yield strength to
calculate fillet radii or picking the fillet radii and checking against material strengths (in this case
among stainless steels) to pick the steel.
o This latter option was chosen.
Equations for Comparison:
(1) Von-Mises Maximum Stress: (Under steady conditions)
𝜎 ′ π‘šπ‘Žπ‘₯ = [(πœŽπ‘š + πœŽπ‘Ž )2 + 3(πœπ‘š + πœπ‘Ž )2 ]1/2 = [(πœŽπ‘Ž )2 + 3(πœπ‘š )2 ]1/2
(2) Material Yield Strength: (Given 𝑛𝑑 = 3.0)
𝑆𝑦 = 𝜎 ′ π‘šπ‘Žπ‘₯ × π‘›π‘‘ = [(𝐾𝑓 πœŽπ‘  )2 + 3(𝐾𝑓𝑠 πœπ‘š )2 ]1/2 × 3.0
RESULTS FOR FILLET RADII TO REDUCE STRESS CONCENTRATIONS AT SHOULDERS:
o By choosing AISI 304 Stainless Steel with 𝑆𝑒𝑑 = 73.2 π‘˜π‘π‘ π‘– and searching for fillet radii
yielding exactly 𝑛𝑑 = 3.0:
 Shoulder 1 Fillet Radius = 0.03 m
 Shoulder 2 Fillet Radius = 0.05 m
5
D. FEA Visualization of 𝑛𝑑 of Shaft Segments & Stresses After Fillets Added:
Figure 10. Snapshots of FEA simulations shown after shoulder 1 fillet of 0.03 m and shoulder 2 fillet of 0.05 m
applied to reduce stress concentrations; Top Left shows displacement in mm; Top Right shows strain in
mm/mm; Bottom Left shows Von Mises Stresses in MPa; Bottom Right shows checks factor of safety for each
region, blue indicating all segments have 𝑛𝑑 ≥ 3.0. General color coding scheme is blue οƒ  sky blue οƒ  green
οƒ  yellow οƒ  red from lowest to highest values for given quantities.
-
Note that in comparison to the FEA simulations prior to adding shoulder fillets, the von-mises
stresses and strains in the shoulder region have dropped significantly, both dropping down from
the “green” into the “sky blue” region of the scale and uniform stress and strains in the shaft
segment regions have also dropped as well. Also note that the bottom right figure shows that all
regions of the graph now have a factor of safety of 3 or above, as the “dark blue” covers the
entire shaft.
III.
Keyway Width & Height Selection:
- Using “Table 1: Key Size vs. Shaft Diameter” from Machinery’s Handbook 27th Edition, for a given
diameter 𝑑 = 0.2 π‘š for the center shaft, converting to inches and finding equivalent width and
height allowed from the table, converting back to meters for our purposes, the key-way
dimensions were determined to be:
o Keyway Length = 0.3 (Given)
o Keyway Width = 0.07 m
6
Download