Physics, asked by purva1694, 4 months ago

figure it out please

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Answered by sandipsagare8588
0

Answer:

Solution

verified

The ladder AB is 3m long, its foot A is at distance AC=1m from the wall. From Pythagons theorem, BC=2  

2

m. The forces on the ladder are its weight W acting at its centre of gravity D, reaction forces F  

1

 and F  

2

 of the wall and the floor respectively. Force F  

1

 is perpendicular to the wall, since the wall is frictionless. Force F  

2

 is resolved into two components, the normal reaction N and the force of friction F. Note that F prevents the ladder from sliding away from the wall and is therefore directed toward the wall.

For translational equilibrium, taking the forces in the vertical direction,

N−W=0                                       (i)

Taking the forces in the horizontal direction,

F−F  

1

=0                                    (ii)

For rotational equilibrium, taking the moments of the forces about A,  

2  

2

F  

1

−(1/2)W=0                                          (iii)

Now W=20g=20×9.8N=196.0N

From (i)N=196.0

From (iii)F  

1

=W/4  

2

=196.0/4  

2

=34.6N

From (ii)F=F  

1

=34.6N

F  

2

=  

F  

2

+N  

2

 

=199.0N

The force F  

2

 makes an angle α with the horizontal,

tanα=N/F=4  

2

,α=tan  

−1

(4  

2

)=80  

o

Explanation:

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