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Whenever we have two-dimensional vector problems in which no two vectors are parallel, the easiest method of solution is to pick a convenient coordinate system and project the vectors onto its axes. In this case, the best coordinate system has one horizontal axis ( x ) and one vertical axis ( y ).

Solution

First, we need to resolve the tension vectors into their horizontal and vertical components. It helps to look at a new free-body diagram showing all horizontal and vertical components of each force acting on the system ( [link] ).

There are three figures. The first one shows TL, at an angle of 5 degrees with the horizontal, pointing left. Two dotted arrows, TLx, pointing straight left and TLy pointing straight up, form a right triangle with TL. The second figure shows TR, at an angle of 5 degrees with the horizontal, pointing right. Two dotted arrows, TRx, pointing straight right and TRy pointing straight up, form a right triangle with TR. The third figure shows a free body diagram. TRx points right. TRy and TLy point up. TLx points left. W points down. Net Fx is equal to 0 and net Fy is qual to 0.
When the vectors are projected onto vertical and horizontal axes, their components along these axes must add to zero, since the tightrope walker is stationary. The small angle results in T being much greater than w .

Consider the horizontal components of the forces (denoted with a subscript x ):

F net x = T R x T L x .

The net external horizontal force F net x = 0 , since the person is stationary. Thus,

F net x = 0 = T R x T L x T L x = T R x .

Now observe [link] . You can use trigonometry to determine the magnitude of T L and T R :

cos 5.0 ° = T L x T L , T L x = T L cos 5.0 ° cos 5.0 ° = T R x T R , T R x = T R cos 5.0 ° .

Equating T L x and T R x :

T L cos 5.0 ° = T R cos 5.0 ° .

Thus,

T L = T R = T ,

as predicted. Now, considering the vertical components (denoted by a subscript y ), we can solve for T . Again, since the person is stationary, Newton’s second law implies that F net y = 0 . Thus, as illustrated in the free-body diagram,

F net y = T L y + T R y w = 0 .

We can use trigonometry to determine the relationships among T Ly , T Ry , and T . As we determined from the analysis in the horizontal direction, T L = T R = T :

sin 5.0 ° = T L y T L , T L y = T L sin 5.0 ° = T sin 5.0 ° sin 5.0 ° = T R y T R , T R y = T R sin 5.0 ° = T sin 5.0 ° .

Now we can substitute the vales for T Ly and T Ry , into the net force equation in the vertical direction:

F net y = T L y + T R y w = 0 F net y = T sin 5.0 ° + T sin 5.0 ° w = 0 2 T sin 5.0 ° w = 0 2 T sin 5.0 ° = w

and

T = w 2 sin 5.0 ° = m g 2 sin 5.0 ° ,

so

T = ( 70.0 kg ) ( 9.80 m/s 2 ) 2 ( 0.0872 ) ,

and the tension is

T = 3930 N .

Significance

The vertical tension in the wire acts as a force that supports the weight of the tightrope walker. The tension is almost six times the 686-N weight of the tightrope walker. Since the wire is nearly horizontal, the vertical component of its tension is only a fraction of the tension in the wire. The large horizontal components are in opposite directions and cancel, so most of the tension in the wire is not used to support the weight of the tightrope walker.

If we wish to create a large tension, all we have to do is exert a force perpendicular to a taut flexible connector, as illustrated in [link] . As we saw in [link] , the weight of the tightrope walker acts as a force perpendicular to the rope. We saw that the tension in the rope is related to the weight of the tightrope walker in the following way:

T = w 2 sin θ .

We can extend this expression to describe the tension T created when a perpendicular force ( F ) is exerted at the middle of a flexible connector:

T = F 2 sin θ .

The angle between the horizontal and the bent connector is represented by θ . In this case, T becomes large as θ approaches zero. Even the relatively small weight of any flexible connector will cause it to sag, since an infinite tension would result if it were horizontal (i.e., θ = 0 and sin θ = 0 ). For example, [link] shows a situation where we wish to pull a car out of the mud when no tow truck is available. Each time the car moves forward, the chain is tightened to keep it as straight as possible. The tension in the chain is given by T = F 2 sin θ , and since θ is small, T is large. This situation is analogous to the tightrope walker, except that the tensions shown here are those transmitted to the car and the tree rather than those acting at the point where F is applied.

Questions & Answers

V=E½-P-½ where v; velocity, P; density and E; constant. Find dimension and it's units of E (constant)
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w=vr where w, angular velocity. v; velocity and r; radius of a circle
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sorry I meant Maximum positive angular velocity of
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please can u tell me the formular for tension in angular velocity I kind of forget it please don't ignore this msg I need it nw
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what is imaginary mass how we express it
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Khlil Reply
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i wanted to know the steps
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Practice Key Terms 3

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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