p06 007

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7. The free-body diagram for the puck is shown below. 

N is the normal force of the ice on the puck, 

f is

the force of friction (in the

−x direction), and mg is the force of gravity.

(a) The horizontal component of Newton’s second law gives

−f = ma, and constant acceleration

kinematics (Table 2-1) can be used to find the acceleration.

Since the final velocity is zero, v

2

=

v

2

0

+ 2ax leads to a =

−v

2

0

/2x. This is

substituted into the Newton’s law equa-
tion to obtain

f

=

mv

2

0

2x

=

(0.110 kg)(6.0 m/s)

2

2(15 m)

=

0.13 N .

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N

m

g



f

(b) The vertical component of Newton’s second law gives N

−mg = 0, so N = mg which implies (using

Eq. 6-2) f = µ

k

mg. We solve for the coefficient:

µ

k

=

f

mg

=

0.13 N

(0.110 kg)



9.8 m/s

2

 = 0.12 .


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