A block of mass m lying on a rough horizontal plane is acted upon by a horizontal force P and another force Q inclined at an angle. to the vertical. The block will remain in equilibrium, if the coefficient of friction between it and the surface
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see figure,
here we have to break force Q into two components .
e.g.,
and
of course we can write in vector format,
e.g.,
we know, friction is a contact force and it is directly proportional to normal reaction between between two contacting bodies.
here, force P and horizontal component of Q act forward then, friction acts backward direction.
hence, friction = P + Qsinθ
fr = μN = P + Qsinθ
here normal reaction , N = Mg + Qcosθ
so, μ = (P + Qsinθ)/N
= (P + Qsinθ)/(Mg + Qcosθ)
here we have to break force Q into two components .
e.g.,
and
of course we can write in vector format,
e.g.,
we know, friction is a contact force and it is directly proportional to normal reaction between between two contacting bodies.
here, force P and horizontal component of Q act forward then, friction acts backward direction.
hence, friction = P + Qsinθ
fr = μN = P + Qsinθ
here normal reaction , N = Mg + Qcosθ
so, μ = (P + Qsinθ)/N
= (P + Qsinθ)/(Mg + Qcosθ)
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=》Here we have to break force Q into two components .
e.g., Q horizontal = Q sin θ
and Q vertical = Q cos θ
we know, friction is a contact force and it is directly proportional to normal reaction between between two contacting bodies.
here, force P and horizontal component of Q act forward then, friction acts backward direction.
hence, friction = P + Qsinθ
fs = μN = P + Qsinθ
here normal reaction , N = Mg + Qcosθ
so, μ = (P + Qsinθ)/N
= (P + Qsinθ)/(Mg + Qcosθ)
》》Answer《《
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