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Engineering examples for Line Vectors


Example 1

Consider a roof truss problem. The following is a drawing of a simple roof truss, consisting of five light weight bars AC, AD, BC, BD and CD, the whole structure resting on walls at A and B, which are on the same horizontal level. The structure is symmetrical about the line CD. A and B are 40 meters apart, and C, D are 15 meters, 5 meters respectively above the level of A and B. Loads of 1000kg, 400kg and 400kg rest on C, A and B respectively, causing reactive vertical forces at A and B, as shown.

                       1000kg wt                                C     400kg wt                      D                      400kg wt   A                                                    B     reactive force                                         reactive force

Calculate the magnitudes of the reactive forces at A and B, and calculate the magnitude of the pushing or pulling force of each of the five bars on its end points, distinguishing which are pulls and which pushes.

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Solution

Let i, j be the unit vectors in the directions AB, DC respectively.

By symmetry the reactive forces at A and B are equal, of magnitude R kg wt say.

The vector sum of all the external forces on the structure as a whole must be zero:

- 1000j-  400j-  400j + Rj + Rj = 0.

Hence each reactive force has magnitude

1000-+-400-+--400         2         = 900 kg wt.

Now suppose the bars AC, AD and CD exert pushing forces of magnitude |x|, |y| and |z| kg wt respectively at their ends. Some of x, y, z may be negative, which will mean the corresponding bar pulls instead of pushes.

By symmetry BC and BD push with forces of magnitude |x| and |y| kg wt respectively.

                         1000                             x  C  x                            z                              z 400                                                   400                         y  D  y    x                                               x A   y                                             y  B     900                                                   900

Let a, b be the angles CAB, DAB respectively.

Clearly a = tan -115 20 = tan -13 4, and b = tan -15- 20 = tan -11 4.

  5       3  a   4   V~ ---   17     1  4b

The forces at A sum to zero:

- 400j + 900j-  (xcos a)i- (x sin a)j - (ycos b)i- (y sin b)j = 0.

Equating i and j components gives two equations:

xcos a + ycos b    =  0 xsina +  ysinb   = 500

These have the unique solution

x = 1250,     y = - 1031 (rounded  to an integer).

By symmetry, considering the forces at B gives equations (1) and (2) again.

Considering forces at C:

- 1000j + zj + (x cosa)i + (xsin a)j- (x cosa)i + (x sin a)j = 0

which gives one non-trivial equation:

z + 2xsina  = 1000

which, using the value of x found above, gives

z = - 500.

The forces at D give

- zj + (y cosb)i + (y sin b)j- (y cosb)i + (ysin b)j = 0

which also yields one non-trivial equation:

z - 2y sin b = 0.

This is satisfied by the values of y and z found above (and, indeed, equation (4) can be deduced from (2) and (3) by taking (3) - 2 × (2).)

So bars AC and BC push with a force of magnitude 1250 kg wt;

bars AD and BD pull with a force of magnitude approximately 1031 kg wt;

and bar CD pulls with a force of magnitude 500 kg wt.

Note: It is important to engineers which are pulls and which pushes -- chains can pull but not push, whereas concrete pylons can push, but would come apart if pulled.

Example 2

A bent lever has perpendicular arms CA (vertical, of length 30cm) and CB (horizontal, of length 12cm), and is pivoted at C. A force P of 35kg wt is applied at A at 15° to the horizontal, and another force Q is applied at B at 20° to the vertical, as shown in the diagram.

Assuming the situation is static, find the magnitude of Q, and the magnitude and direction of the reaction at C.

 A  P         reactive force                       Q        C             B

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Solution

Let i, j be the unit vectors in the directions CB, CA respectively, so k = i × j is the unit vector vector perpendicular to and up from the plane of ABC.

The magnitude of Q, can be determined from the fact that, because the situation is static, the sum of the moments of P and Q about C is zero:

P  × CA  + Q  × CB  = 0

i.e.,

           o           o                      o             o (- 35cos 15 i- 35 sin 15 j) × 30j + (- |Q |sin 30 i- |Q |cos20 j) × 12i = 0

or

(- 1050 cos15o + 12|Q |cos20o)k =  0

which gives

                o |Q |=  700-cos15--= 89.94 ··· = 90        12 cos20o

to 2 significant figures.

From the fact that the situation is static the reaction force at C must be the negative of the sum of the forces P and Q, that is,

- P - Q
= (35 cos 15°i + 35 sin 15°j) + (|Q| sin 20°i + |Q| cos 20°j)
= 64.57i + 93.58j
= 113.6(cos 55.4°i + sin 55.4°j).
So The reactive force at C is (approximately) 113.6kg wt, in the direction 55.4° from the horizontal.