**Problem : **

A 5*kg* picture frame is held up by two ropes, each inclined 45^{o}
below vertical, as shown below. What is the tension in each of the ropes?

Because the picture frame is at rest, the tension in the two ropes must exactly counteract the gravitational force on the picture frame. Drawing a free body diagram we can calculate the vertical components of the tension in the ropes:

Clearly the horizontal components of the tension in the two ropes cancel exactly. In addition, the vertical components are equal in magnitude. Since*F*= 0, then the vertical components of the tension in the two ropes must cancel exactly with the gravitational force: 2

*T*

_{y}=

*mg*âá’2

*T*sin 45

^{o}= (5)(9.8) = 49

*N*. Thus:

*T*= = 34.6

*N*. The total tension on each rope is thus 34.6

*N*.

**Problem : **

Consider a 10*kg* block resting on a frictionless plane inclined
30^{o} connected by a rope through a pulley to a 10*kg* block
hanging free, as seen in the figure below. What is the direction and
magnitude of the resulting acceleration of the 2-block system?

Though this problem seems quite complex, it can be solved by simply drawing a free body diagram for each block. Since the resulting acceleration of each block must be of the same magnitude, we will get a set of two equations with two unknowns, T and a. First we draw the free body diagram:

On block 1, there are 3 forces acting: normal force, gravitational force and tension. The gravitational force, in terms of parallel and perpendicular components, and the normal force can be easily calculated:

F_{G} | = (10kg)(9.8) | = 98N | |

F_{Gâä¥} | = F_{G}cos 30^{o} | = 84.9N | |

F_{G || } | = F_{G}sin 30^{o} | = 49N |

The normal force is simply a reaction to the perpendicular component of the gravitational force. Thus

*F*

_{N}=

*F*

_{Gâä¥}= 84.9

*N*.

*F*

_{N}and

*F*

_{Gâä¥}thus cancel, and the block is left with a force of 49

*N*down the ramp, and the tension, T, up the ramp.

On block 2, there only two forces, the gravitational force and the
tension. We know that *F*_{G} = 98*N*, and we denote the tension by T. Using
Newton's Second Law to combine the forces on block 1 and block 2, we have
2 equations and 2 unknowns, a and T:

F | = ma | ||

10a_{1} | = T - 49 | ||

10a_{2} | = 98 - T |

However, we know that

*a*

_{1}and

*a*

_{2}are the same, because the two blocks are bound together by the rope. Thus we can simply equate the right side of the two equations:

*T*- 49 = 98 -

*T*Thus 2

*T*= 147 and

*T*= 73.5

*N*

*a*= 73.5 - 49 = 24.5

*a*= 2.45

*m*/

*s*

^{2}. Interpreting our answer physically, we see that block 1 accelerates up the incline, while block 2 falls, both with the same acceleration of 2.45

*m*/

*s*

^{2}.

**Problem : **

Two 10*kg* blocks are connected by a rope and pulley system, as in the
last problem. However, there is now friction between the block and the
incline, given by *μ*_{s} = .5 and *μ*_{k} = .25. Describe the resulting
acceleration.

We know from the last problem that block 1 experiences a net force up the
incline of 24.5 N. Since friction is present, however, there will be a
static frictional force counteracting this motion. *F*_{s}^{max} = *μ*_{s}*F*_{n} = (.5)(84.9) = 42.5*N*. Because this maximum value for the frictional
force exceeds the net force of 24.5 N, the frictional force will
counteract the motion of the blocks, and the 2 block system will not move.
Thus *a* = 0 and neither block will move.