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SOLUTION:

We
write SF = ma from the
force diagram for the stationary hanging mass, with down positive:
mg
– FT=
ma
= 0;which gives
FT=
mg.
For the rotating puck, the tension provides the centripetal acceleration,
SFR
= MaR:
FT=
Mv2/R.
When
we combine the two equations, we have
Mv2/R
= mg, which gives v = (mgR/M)1/2.

This
friction force provides the centripetal acceleration.We
take a coordinate system with the x-axis in the direction of the
centripetal acceleration.
We
write SF = ma from the
force diagram for the auto:
x-component:Ffr
= ma = mv2/R;
y-component:FN–
mg
= 0.
The
speed is maximum when Ffr
= Ffr,max
= msFN.
When
we combine the equations, the mass cancels, and we get
msg
= vmax2/R;
(0.80)(9.80
m/s2) = vmax2/(70
m), which gives vmax
= 23 m/s.
The
mass canceled, so the result isindependent
of the mass.
(b) g = GME/r2 = GME/(RE
+ h)2 = (6.67 x 10-11)(5.98 x 1024 kg)/(3.2
x 106 m + 6.38 x 106 m)2 = 4.30m/s2
v
= 2pR/T.
The
required centripetal acceleration is provided by the gravitational attraction:
GMMm/R2
= mv2/R = m(2pR/T)2/R
= m4p2R/T2,
so we have
GMM
= 4p2(RM
+ h)3/T2;
(6.67
´ 10–11
N · m2/kg2)(7.4
´ 1022
kg) = 4p2(1.74
´ 106
m + 1.00 ´ 105
m)3/T2,
which
gives T = 7.06
´ 103
s = 2.0
h.
worbit=
Dq/Dt
=
(2p rad)/(1 yr)(3.16 ´ 107
s/yr) = 1.99 ´ 10–7
rad/s.
(b)The
Earth rotates one revolution in one day, so we have
wrotation=
Dq/Dt
=
(2p rad)/(1 day)(24 h/day)(3600 s/h) = 7.27 ´ 10–5
rad/s.
=½ [(210
rev/min + 350 rev/min)][(2p rad/rev)/(60 s/min)](6.5
s) = 191 rad = 30.3 rev.
For
each revolution the point on the edge will travel one circumference, so
the total distance traveled is
d = qD = (30.3 rev)(0.40 m) =38 m.