P11215 Analysis Documents Anthony Poli Wheel Speed / Kinematic Drive Analysis Motor Transmission Wheel Gear Ratios: Motor to Transmission: Transmission to Wheel: Wheel Diameter: 10:72 24:40 12 in. .1388 .6 ωm = Motor Speed ωT = Transmission Speed ωw = Wheel Speed V = Vehicle Velocity ππ = 10 π 72 π ππ€ = 24 π 40 π π= 1[ππ‘] 12[ππ] ππ‘ ∗ 12 [ππ]πππ€ [ π ] Combine to get: π= 1[ππ‘] 24 10 ππ‘ ∗ 12 [ππ]π ∗ ππ [ ] 12[ππ] 40 72 π So at the lowest motor revolutions obtained by the previous group, 22.5 [°/s] or 3.75rpm, V = 11.78 [ft./min] The old goal was 10 [ft./min] so this is acceptable. For lowest speed, Which is the autonomous Operation speed ωm = 22.5 [°/s] or 3.75rpm ωT = 0.52 rpm ωw = 0.3125 rpm P11215 Analysis Documents Anthony Poli P11215 Analysis Documents Anthony Poli Force on Pin: Motor Torque Hole Motor Transmission Max torque output of the motor: Radius of 10T Drive Cog: Radius of 72T Cog: Radius to pin hole: Diameter of pin hole: Radius to hole center τm d1 d2 d3 21 [N*m] 0.6896 in. 4.405 in. 1 in. 0.5 in. or 185.87 [in.*lb.] π =πΉ∗π τ = Torque F = Force d = Distance from pivot πΉπβπππ = ππ π1 ππ‘ππππ . = πΉπβπππ ∗ π2 πΉβπππ = ππ‘ππππ . π3 Combine to get: πΉβπππ ππ ∗ π2 ππ π2 π1 = = π3 π1 π3 Sub to get: πΉβπππ = 21[ππ.∗ ππ. ] ∗ 4.405[ππ. ] = 1187 πππ. 1[ππ. ] ∗ 0.6896[ππ. ] P11215 Analysis Documents Pin Stress: Force on Pin Direction of Motion ½“ gap The Pin will receive most of its stress in the form of shear. Max shear force Ey of 10060 Steel Poisson’s Ratio Fp E ν Shear Modulus πΈ = 2πΊ(1 + π) For Steel πΊ = 24000[ππ π] 2(1+.3) 1200 [lbf] 24[kpsi] (lowest grade I could find in Shigley p.1020) 0.3 (for most Structural Metals) πΊ= πΈ 2(1+π) = 9230.77 For a pin: ππππ₯ = πΉ π΄ τ = Shear Stress F = Force Applied A = Cross-sectional Area π΄= π 2 π π = 0.5[ππ. ]2 = 0.19635[ππ.2 ] 4 4 Sub: ππππ₯ = G = 9231[psi] τmax = 6112[psi] G > τmax therefore the pin won’t break. 1200[πππ] = 6111.55 [ππ π] 0.19635[ππ.2 ] Anthony Poli P11215 Analysis Documents Anthony Poli Gear Stress: The Stress on the hole in the 24tooth gear was performed in ANSYS by Chris. A view of the mesh A close up of the stress concentration at the hole. The max stress experienced by the gear hole is 23000ksi A conservative yield strength for steel is 34000ksi This yields a factor of safety of 1.7 which is within tolerable limits of the part. Also this is stress concentration was simulated with the max stall force the motor can output. This force is much greater than the force required to drive the robot. The last team found it took 9[in.*lbs.] of motor output to move the robot and this simulation was run with a motor output of over 185[in.*lbs.] P11215 Analysis Documents Anthony Poli Transmission Axle Stress Cantilevered Beam Weld joint for axle To determine if the axle is strong enough the max force applied at the end of the axle will be found. If no forces exceed that force the beam will hold. Max. Force at furthest distance Axle L P Ey G Length Load Yield Strength Shear Modulus 4[in.] Find. 218000 [psi] 11900000 [psi] The properties are for O1 Hardened Tool Steel (from Matweb.com) which is the steel to be ordered for this axel. This specification was based on workability and price for the length and diameter needed. For Bending: ππ₯ = Where: σx = Bending Stress M = Bending Force y = distance from axis I = Area Moment of Inertia ππ¦ πΌ [psi] [in. * lb] [in.] [in4] I for a cylinder: πΌ= π 4 π π = 0.254 = 0.000192[ππ.4 ] 64 64 Max Bending Force: ππ₯ πΌ πΈπΌ 218000[ππ π] ∗ 0.000192[ππ.4 ] π= = π π’π: = = 334.408 [ππ.∗ ππ] π¦ π¦ . 125[ππ. ] Max Force: π 334 π= = = 83[ππ] πΏ 4 P11215 Analysis Documents For Shear: ππππ₯ = πΊ = πΉ π΄ τ = Shear Stress F = Force Applied A = Cross-sectional Area π΄= π 2 π π = 0.75[ππ. ]2 = 0.049087[ππ.2 ] 4 4 Max Shear Force: πΉ = πΊπ΄ = 11900000 [psi] ∗ 0.049087[ππ.2 ] = 584140 [ππ] No worries here. Anthony Poli P11215 Analysis Documents Anthony Poli Axle Stress Cantilevered Beam To determine if the axle is strong enough the max force applied at the end of the axle will be found. If no forces exceed that force the beam will hold. Max. Force at furthest distance Axle mount Axle L P Ey G Length Load Yield Strength Shear Modulus 6[in.] Find. 34100 [psi] 11600000 [psi] The properties are for Ultra-Machinable 12L14 Carbon Steel (from Matweb.com) which is the steel to be ordered for this axel. This specification was based on workability and price for the length and diameter needed. For Bending: ππ₯ = Where: σx = Bending Stress M = Bending Force y = distance from axis I = Area Moment of Inertia ππ¦ πΌ [psi] [in. * lb] [in.] [in4] I for a cylinder: πΌ= π 4 π π = 0.754 = 0.015532[ππ.4 ] 64 64 Max Bending Force: ππ₯ πΌ πΈπΌ 34100[ππ π] ∗ 0.015532[ππ.4 ] π= = π π’π: = = 1412.34[ππ.∗ ππ] π¦ π¦ . 375[ππ. ] Max Force: π 1412 π= = = 235[ππ] πΏ 6 P11215 Analysis Documents Anthony Poli Since the Robot is supported by 4 wheels and may weigh a total of 200 pounds this should be acceptable. If not a Steel with a higher yield modulus can be used. For Shear: ππππ₯ = πΊ = πΉ π΄ τ = Shear Stress F = Force Applied A = Cross-sectional Area π΄= π 2 π π = 0.75[ππ. ]2 = 0.441786[ππ.2 ] 4 4 Max Shear Force: πΉ = πΊπ΄ = 11600000 [psi] ∗ 0.441786[ππ.2 ] = 5124723.02 [ππ] No worries here.