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bazaltina [42]
3 years ago
5

A uniform ladder stands on a rough floor and rests against a frictionless wall. Since the floor is rough, it exerts both a norma

l force N1 and a frictional force f1 on the ladder. However, since the wall is frictionless, it exerts only a normal force N2 on the ladder. The ladder has a length of L = 4.6m, a weight of WL= 69.0N , and rests against the wall a distance d = 3.75 m above the floor. If a person with a mass of m = 90 kg is standing on the ladder, determine the forces exerted on the ladder when the person is halfway up the ladder.
Required:
Solve of N1, N2 and f1
Physics
1 answer:
vampirchik [111]3 years ago
8 0

Answer:

The  normal force N1 exerted by the floor is  N_1 = 951 \ N

The  normal force N2 exerted by the wall is  N_2= 616.43 \ N

The frictional force exerted by the wall is  f  = N_2 = 616.43 \ N  

Explanation:

From the question we are told that

    The length of the ladder is  L =  4.6 \ m

    The weight of the ladder  is

    The distance of the ladder position on the wall from the floor is  D = 3.75 \ m

     The mass of the person is  m =  90 kg

Applying Pythagoras theorem

The length of the position the ladder on the ground from the base of the wall is

    A  =  \sqrt{L^ 2 -  D^2}

substituting values

    A =  \sqrt{(4.6^2)-(3.75^2)}

    A = 2.66 \  m

  In order the for the ladder not to shift from the ground the sum of the moment about the position of the ladder on the ground must be equal to zero this is mathematically represented as

        \sum M = 0  = N_2 * D - [\frac{1}{2} * W_L ] * [(mg) *A  ]

         \sum M = 0  = N_2 * 3.75 - [\frac{1}{2} * 69.0 ] * [(90*9.8) * \frac{4.6}{2.66} ]

        N_2 * 3.75 =2311.62

        N_2 * 3.75 =2311.62

        N_2= 616.43 \ N

Now the force exerted by the floor on the ladder is mathematically represented as

           N_1 =  W_L  + (m * g )

substituting values

          N_1 = 951 \ N

Now the horizontal forces acting on the ladder are N_2 \ and  \ f and they are in opposite direction so

     f  = N_2 = 616.43 \ N  

         

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   From the question we are told that

          The mass of the beam  is   m_b =M

          The length of the beam is  l = L

           The hanging mass is  m_h = 3M

            The length of the hannging mass is l_h = \frac{3}{4} l

            The angle the cable makes with the wall is \theta = 60^o

The free body diagram of this setup is shown on the first uploaded image

The force F_x \ \ and \ \ F_y are the forces experienced by the beam due to the hinges

      Looking at the diagram we ca see that the moment of the force about the fixed end of the beam along both the x-axis and the y- axis is zero

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           \sum F =0

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            F_x =T cos (60)

                 F_x= \frac{T}{2} ---(1)

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           F_y  + Tsin \theta  = M *g + 3M *g ----(2)

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          M* g * \frac{L}{2}  + 3M * g \frac{3L}{2} - T sin(60) * L = 0

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