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A demonstration gyroscope wheel is constructed by removing the tire from a bicycle wheel 0.650 m in diameter, wrapping lead wire around the rim, and taping it in place. The shaft projects 0.200 m at each side of the wheel, and a woman holds the ends of the shaft in her hands. The mass of the system is 8.00 kg; its entire mass may be assumed to be located at its rim. The shaft is horizontal, and the wheel is spinning about the shaft at 5.00 rev/s. Find the magnitude and direction of the force each hand exerts on the shaft (a) when the shaft is at rest; (b) when the shaft is rotating in a horizontal plane about its center at 0.050 rev/s; (c) when the shaft is rotating in a horizontal plane about its center at 0.300 rev/s. (d) At what rate must the shaft rotate in order that it may be supported at one end only?

Short Answer

Expert verified

(a) The shaft is rest at FR=39.2NandFL=39.2N .

(b) The work done by the tension force is W=mv12r1221r22-1r12.

(c) The change in kinetic energy is equal to work done that is K=W.

Step by step solution

01

Given Data

It is given that the diameter of wheel as D = 0.650m , shaft length as d = 0.200m , mass of the system as m = 8.00 kg and the angular speed of the wheel as =5.00rev/sor =31.4rad/s.

02

(a) The shaft at rest

The weight of the wheel is depends on the force exerted by the hands. So the weight of the wheel can be written as W=FL+FR and the net torque is given by =dFR-FL.

The torque is related to the angular speed by =/then,

dFRFL=/FRFL=/d

Substitute FL=mg-FRin the above equation

FRmgFR=/d2FRmg=/d2FR=/d+mgFR=12/d+mg

Similarly, find FL as follows:

FL=mg12/d+mg=12/d+mg=12mg/d

Since, the moment of inertia about the axis through the center isI=mR2 then,
FR=12mR2d+mgandFL=12mgmR2d

Here, the shaft does not rotate implies =0 then,

FR=12mR2d+mg=120+(8.00kg)9.80m/s2=39.2N

Similarly find FLas follows:

FL=12mgmR2d=12(8.00kg)9.80m/s20=39.2N

Therefore, the shaft is rest at FR=39.2Nand FL=39.2N.

03

(b) Shaft rotating about center at  0.050 rev/s

It is given that =0.050rev/sthat implies =0.314rad/s.

Substitute the known values in FRand simplify.

FR=12mR2d+mg=12(8.00kg)(0.314rad/s)(0.325m)2(31.4rad/s)0.200m+(8.00kg)9.80m/s2=(8.00kg)2(0.314rad/s)(0.325m)2(31.4rad/s)0.200m+9.80m/s2=60.0N

Similarly, Substitute the known values in FLand simplify.

FL=12mR2d+mg=12(8.00kg)(0.314rad/s)(0.325m)2(31.4rad/s)0.200m+(8.00kg)9.80m/s2=(8.00kg)2(0.314rad/s)(0.325m)2(31.4rad/s)0.200m+9.80m/s2=18.4N

Therefore, the required values are FR=60.0NandFL=18.4N.

04

(c) Shaft rotating about center at  

It is given that =0.300rev/sthat implies=1.89rad/s.

Substitute the known values in FRand simplify.

FR=12mR2d+mg=12(8.00kg)(1.89rad/s)(0.325m)2(31.4rad/s)0.200m+(8.00kg)9.80m/s2=(8.00kg)2(1.89rad/s)(0.325m)2(31.4rad/s)0.200m+9.80m/s2=165N

Similarly, Substitute the known values in FLand simplify.

FL=12mR2d+mg=12(8.00kg)(1.89rad/s)(0.325m)2(31.4rad/s)0.200m+(8.00kg)9.80m/s2=(8.00kg)2(1.89rad/s)(0.325m)2(31.4rad/s)0.200m+9.80m/s2=86.2N

Therefore, the required values are FR=165NandFL=-86.2Nand .

05

(b) Rotation of shaft

Let one force FRbe zero then FL=mg.

Consider the equation =wdIwhich can be written as =mgdmR2.

Substitute all the known values and simplify.

=mgdmR2=gdR2=9.80m/s2(0.200m)(0.325m)2(31.4rad/s)=0.591rad/s

Therefore, the shaft rotate in a rate at =0.591rad/s.

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