PHYS 5204
- 3—I think that choice 2 could also be right, but it is described a little confusing for me. As you can see in the pic, the velocity vector V is tangent to a point on the circumference which is also parallel to the plane of rotation. If choice 2 had the word “tangent” in the description I would feel more confident, otherwise I’m not sure it describes a point on the circumference which actually draws out a curved path, not a straight path that the velocity vector does
- 3—action and reaction forces act on both bodies
- 2—steeper is faster
- 1—speed is based on height: Potential Energy is converted to Kinetic Energy, it’s just that the steeper plane converts it faster
- 2—Higher torque results in higher angular acceleration and velocity if turning the same load
- 2—Right Hand Rule indicates the Angular velocity vector is to the left and rotation is counter clockwise
- 1—Right Hand Rule indicates the Angular acceleration vector is slowing the disk down
- 5—Only force acting on the system is the gravitational force pulling on m2 and that force is m2g
- 3—That same force is being applied to the entire mass of the system (m1+m2)
- 7—simple division of m2g/(m1+m2)
- 4—Tension is force acting on m1 or m1a or m1m2g/(m1+m2)
- 1—Tension on block A is not working against any force (like friction or gravity) so therefore no work is being done
- 5—KE1=m1v2/2 and v2=2ad so KE1=m1ad= m1m2gd/(m1+m2)
- 4—All of the Potential Energy in Block B is converted to Kinetic Energy in Blocks A and B
- 1—Rotational inertia of a solid cylinder (since the mass is evenly distributed) is I=mr2/2, with m=250kg and r=d/2=.30/2=.15mI=250(.15)2/2=2.81kg-m2
- 3—Torque=Rotational Inertia x Angular accelerationτ=Iα so,
α=τ/I=120 N-m/2.81 Kg-m2=42.7 rad/s2 - 2—Angular acceleration is the change in Angular velocity over the change in timeα=Δω/Δt and Δω=ωfinal-ωinitial Since ωinitial=0 rad/s, we can easily solve for Δt=Δω/α=
3000rpm(1min/60s)(2π rad/1 rev)/42.7 rad/s2=7.35 sec - 3—Power(in kW) from a motor=Torque(N-m)(2π)(# rpm)/60,000=(120)(2π)(3000)/60,000=
37.68 kW=37680 W and 1 hp=746 W so the motor generates 37680/746=50.5 hp - 4—All of the rotational Kinetic Energy of the motor will be converted to Heat. KErot=Iω2/2
=(2.81 kg-m2)((3000 rpm)(1min/60s)(2π rad/1 rev))2/2=138,527 Joules - 2—The Force of friction is related to the weight of the armature on the bearings. Recall W=mg=(250kg)(9.8m/s2)=2450N. This corresponds to a friction force of Ffric=Wη (where η is the coefficient of friction=0.008) so Ffric=(2450N)(0.008)=19.6N. Recall that τ=Fr where the Force (F) is applied at a distance (r) from the center of the shaft to create Torque (τ). Since we already know the Friction force = 19.6N, what is the equivalent torque due to friction on the bearings? The torque is τ=Fr=(19.6N)(.016m)=.314N-m
- 4—The torque of friction creates a small angular deceleration α where τ=Iα from Prob 16 above. Solving for α α=τ/I=.314N-m/2.81 kg-m2=-0.112rad/s2. We can use this to calculate the time for the angular velocity to decrease from 3000 rpm to a complete stop with the relationship from Prob 17: α=Δω/Δt and Δω=ωfinal-ωinitial Since ωinitial=3000 rpm and ωfinal=0 rpm, we can easily solve for Δt Δt=Δω/α=(0-(3000rpm)(1min/60s)(2π rad/1 rev))/(-0.112rad/s2)=2810 sec
- 4—output torque=(input torque)(gear reduction ratio)(120N-m)(3/1)=360N-m