22.03.2019 Views

fisica1-youn-e-freedman-exercicios-resolvidos

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

5.59: Consider a point a distance x from the top of the rope. The forces acting in this<br />

point are T up and ( M<br />

m ( L−<br />

x<br />

+ )<br />

)g downwards. Newton’s Second Law becomes<br />

T<br />

m(<br />

L−<br />

x)<br />

m(<br />

L−<br />

x)<br />

( M + ) g = ( M + ) a.<br />

L<br />

L<br />

F −(<br />

M m)<br />

g<br />

m(<br />

L x)<br />

F<br />

− Since , ( +<br />

−<br />

T = M + )( ).<br />

L<br />

= . At<br />

a<br />

M + m<br />

L M + m<br />

MF<br />

M m<br />

= M ( a +<br />

x = 0 , T = F , and at x = L, T =<br />

+<br />

g)<br />

as expected.<br />

5.60: a) The tension in the cord must be m2g in order that the hanging block move at<br />

constant speed. This tension must overcome friction and the component of the<br />

gravitational force along the incline, so m2g<br />

= ( m1<br />

g sin α + µ<br />

k<br />

m1<br />

g cosα)<br />

and<br />

m (sin<br />

2<br />

= m1 α + µ<br />

k<br />

cosα)<br />

.<br />

b) In this case, the friction force acts in the same direction as the tension on the block<br />

of mass m<br />

1<br />

, so m2 g = ( m1<br />

g sin α − µ<br />

km1g<br />

cosα)<br />

, or m (sin 2<br />

= m1 α − µ<br />

k<br />

cosα)<br />

.<br />

c) Similar to the analysis of parts (a) and (b), the largest m<br />

2<br />

could be is<br />

m1 (sinα + µ<br />

s<br />

cos α)<br />

and the smallest m<br />

2<br />

could be is m1 (sinα − µ<br />

s<br />

cos α)<br />

.<br />

5.61: For an angle of 45 .0°<br />

, the tensions in the horizontal and vertical wires will be the<br />

same. a) The tension in the vertical wire will be equal to the weight w = 12.0 N ; this must<br />

be the tension in the horizontal wire, and hence the friction force on block A is also 12.0<br />

N . b) The maximum frictional force is µ<br />

s<br />

w A<br />

= (0.25)(60.0 N) = 15 N ; this will be the<br />

tension in both the horizontal and vertical parts of the wire, so the maximum weight is 15<br />

N.<br />

5.62: a) The most direct way to do part (a) is to consider the blocks as a unit, with total<br />

weight 4.80 N. Then the normal force between block B and the lower surface is 4.80 N,<br />

and the friction force that must be overcome by the force F is<br />

µ<br />

k<br />

n = (0.30)(4.80 N) = 1.440 N, or 1.44 N, to three figures. b) The normal force<br />

between block B and the lower surface is still 4.80 N, but since block A is moving<br />

relative to block B, there is a friction force between the blocks, of magnitude<br />

( 0.30)(1.20 N) = 0.360 N, so the total friction force that the force F must overcome is<br />

1 .440 N + 0.360 N = 1.80 N . (An extra figure was kept in these calculations for clarity.)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!