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Question

Two sides of a step ladder BA and CA are 1.6 m long and hinges at A, A rope DE, 0.5 m long is tied half way up. A weight 40 kg is suspended from point F, 1.2 m from B along the ladder BA. assuming the floor to be frictionless and neglecting the weight of ladder find the tension in the rope and forces exerted by floor on ladder.
1241231_fa894335a4d746cd83ecf6dcb0066230.png

A
T=350 N R1=250N
R2=150B
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B
T=97 N R1=150N
R2=100N
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C
T=97 N R1=250N
R2=150N
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D
T=250 N R1=100N
R2=50N
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Solution

The correct option is B T=97 N R1=150N
R2=100N

NB= Force exerted on the ladder by the floor point B
NC= Force exerted on the ladder by the floor point C
T= tension in the rope
BA=CA=1.6m
DE=0.5m
BF=1.2m
Man of the weight, m=40kg drawing the perpendicular form A on the floor BC,
This intersects DE at mid-point H.
ΔABJ and ΔAIC are similar BI=IC
Hence, I is the mid-point of BC
DEBC
BC=2×DE=1m
AF=BABF
=0.4m(i)
D is the mid-point of AB.
Hence, we can write
AD=(12)×BA
=0.8m(ii)
Using equations (i) and (ii) we get,
FE=0.4m
Hence, F is the mid point AD. FGDH and F is the mid-point of AD. Hence, G will also be the mid point of AH.
ΔAFG and ΔADH are similar
FG/DH=AF/AD
FG/DH=0.4/0.8=1/2
FG=(1/2)×DH
=12×0.25=0.125m
In ΔADH,
AH=(AD2DH2)1/2
=(0.820.252)1/2
=0.76m
For translational equilibrium at the ladder, the upward force should be equal to the downward force,
NC+NB=mg=392(iii)
For rotational equilibrium of the ladder, the net moment about A is,
NB×B1+mg×FG+NC+C1+T×AGT×AG=0
NB×0.5+40×9.8+0.125+NC×0.5=0
(NCNB)×0.5=49
NCNB=98(iv)
Adding equations (iii) and (iv), we get
NC=245N
NB=147N
For rotational equilibrium of the side AB consider the moment about A.
NB×B1+mg×FG+T×AG=0
245×0.5+40×9.8+0.125+T×6.76=0
T=96.7N

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