Answer:
Approximately
in each of the two ropes.
Explanation:
Let
and
denote the tension in each of the two ropes.
Refer to the diagram attached. The tension force in each rope may be decomposed in two directions that are normal to one another.
The first direction is parallel to resultant force on the barge.
- The component of
in that direction would be
. - Similarly, the component of
in that direction would be
.
These two components would be in the same direction. The resultant force in that direction would be the sum of these two components:
. That force should be equal to
.
The second direction is perpendicular to the resultant force on the barge.
- The component of
in that direction would be
. - Similarly, the component of
in that direction would be
.
These two components would be in opposite directions. The resultant force in that direction would be the difference of these two components:
. However, the net force on the barge is normal to this direction. Therefore, the resultant force should be equal to zero.
That gives a system of two equations and two unknowns:
, and
.
The second equation suggests that
. Hence, replace the
in the first equation with
and solve for
:
.
Because
(as seen in the second equation,)
.
In other words, the tension in each of the two ropes is approximately
.