5 Engineering Example 3

5.1 Vintage car brake pedal mechanism

Introduction

Figure 16 shows the structure and some dimensions of a vintage car brake pedal arrangement as far as the brake cable. The moment of a force about a point is the product of the force and the perpendicular distance from the point to the line of action of the force. The pedal is pivoted about the point A . The moments about A must be equal as the pedal is stationary.

Problem in words

If the driver supplies a force of 900 N , to act at point B , calculate the force ( F ) in the cable.

Mathematical statement of problem

The perpendicular distance from the line of action of the force provided by the driver to the pivot point A is denoted by x 1 and the perpendicular distance from the line of action of force in the cable to the pivot point A is denoted by x 2 . Use trigonometry to relate x 1 and x 2 to the given dimensions. Calculate clockwise and anticlockwise moments about the pivot and set them equal.

Figure 16 :

{ Structure and dimensions of vintage car brake pedal arrangement}

Mathematical Analysis

The distance x 1 is found by considering the right-angled triangle shown in Figure 17 and using the definition of cosine.

Figure 17

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The distance x 2 is found by considering the right-angled triangle shown in Figure 18.

Figure 18

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Equating moments about A :

900 x 1 = F x 2 so F = 2013 N.

Interpretation

This means that the force exerted by the cable is 2013 N in the direction of the cable. This force is more than twice that applied by the driver. In fact, whatever the force applied at the pedal the force in the cable will be more than twice that force. The pedal structure is an example of a lever system that offers a mechanical gain.

Task!

Obtain all the angles and the remaining side for the triangle shown:

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This is Case 3. To obtain the angle at B we use tan B = 4 5 so B = tan 1 ( 0.8 ) = 38.6 6 .

Then the angle at A is 18 0 ( 9 0 38.6 6 ) = 51.3 4 .

By Pythagoras’ theorem c = 4 2 + 5 2 = 41 6.40 .

Task!

Obtain the remaining sides and angles for the triangle shown.

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This is Case 1. Since 3 1 4 0 = 31.6 7 then cos 31.6 7 = a 15 so a = 15 cos 31.6 7 = 12 . 77 .

The angle at A is 18 0 ( 90 + 31.6 7 ) = 58.3 3 .

Finally sin 31.6 7 = b 15 b = 15 sin 31.6 7 = 7.85 .

(Alternatively, of course, Pythagoras’ theorem could be used to calculate the length b .)

Task!

Obtain the remaining sides and angles of the following triangle.

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This is Case 2.

Here tan 34.3 3 = 8 a so a = 8 tan 34.3 3 = 11.7

Also c = 8 2 + 11 . 7 2 = 14.18 and the angle at A is 18 0 ( 9 0 + 34.3 3 ) = 55.6 7 .

Exercises
  1. Obtain cosec θ , sec θ , cot θ , θ in the following right-angled triangle.

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  2. Write down sin θ , cos θ , tan θ , cosec θ for each of the following triangles:

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  3. If θ is an acute angle such that sin θ = 2 7 obtain, without use of a calculator, cos θ and tan θ .
  4. Use your calculator to obtain the acute angles θ satisfying
    1. sin θ = 0.5260 ,
    2. tan θ = 2.4 ,
    3. cos θ = 0.2
  5. Solve the right-angled triangle shown:

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  6. A surveyor measures the angle of elevation between the top of a mountain and ground level at two different points. The results are shown in the following figure. Use trigonometry to obtain the distance z (which cannot be measured) and then obtain the height h of the mountain.

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  7.   As shown below two tracking stations S 1 and S 2 sight a weather balloon ( W B ) between them

     at elevation angles α and β respectively.

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     Show that the height h of the balloon is given by h = c cot α + cot β

  8.   A vehicle entered in a ‘soap box derby’ rolls down a hill as shown in the figure. Find the total

     distance ( d 1 + d 2 ) that the soap box travels.

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  1. h = 1 5 2 + 8 2 = 17 , cosec θ = 1 sin θ = 17 8 sec θ = 1 cos θ = 17 15 cot θ = 1 tan θ = 15 8

    θ = sin 1 8 17 ( for example ) θ = 28.0 7

    1. sin θ = 2 5 cos θ = 21 5 tan θ = 2 21 21 cosec θ = 5 2
    2. sin θ = y x 2 + y 2 cos θ = x x 2 + y 2 tan θ = y x cosec θ = x 2 + y 2 y
  2. Referring to the following diagram

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    Hence cos θ = 3 5 7 tan θ = 2 3 5 = 2 5 15

    1. θ = sin 1 0.5260 = 31.7 3
    2. θ = tan 1 2.4 = 67.3 8
    3. θ = cos 1 0.2 = 78.4 6
  3. β = 90 α = 32 . 5 , b = 10 tan 57 . 5 6.37 c = 10 sin 57 . 5 11.86
  4. tan 3 7 = h z + 0.5 tan 4 1 = h z from which

    h = ( z + 0.5 ) tan 3 7 = z tan 4 1 , so z tan 3 7 z tan 4 1 = 0.5 tan 3 7

    z = 0.5 tan 3 7 tan 3 7 tan 4 1 3.2556 km , so h = z tan 4 1 = 3.2556 tan 4 1 2.83 km

  5. Since the required answer is in terms of cot α and cot β we proceed as follows:

    Using x to denote the distance S 1 P cot α = 1 tan α = x h cot β = 1 tan β = c x h

    Adding: cot α + cot β = x h + c x h = c h h = c cot α + cot β as required.

  6. From the smaller right-angled triangle d 1 = 200 sin 2 8 = 426.0 m . The base of this triangle then has length = 426 cos 2 8 = 376.1 m

    From the larger right-angled triangle the straight-line distance from START to FINISH is 200 sin 1 5 = 772.7 m. Then, using Pythagoras’ theorem ( d 2 + ) = 772 . 7 2 20 0 2 = 746.4 m from which d 2 = 370.3 m d 1 + d 2 = 796.3 m