p06 071

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71.

(a) The force which provides the horizontal acceleration v

2

/R necessary for the circular motion of

radius R = 0.25 m is T sin θ, where T in the tension in the L = 1.2 m string and θ is the angle of
the stringmeasured from vertical. The other component of tension must equal the bob’s weight so
that there is no vertical acceleration: T cos θ = mg. Combiningthese observations leads to

v

2

R

= g tan θ

where

sin θ =

R

L

so that θ = sin

1

(0.25/1.2) = 12

and v =

gR tan θ = 0.72 m/s. It should be mentioned that

Sample Problem 6-11 discusses the conical pendulum.

(b) Thus, a = v

2

/R = 2.1 m/s

2

.

(c) The tension is

T =

mg

cos θ

=

(0.050)(9.8)

cos 12

= 0.50 N .


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