1.

Arrive at an expression for power and velocity. Given some examples for the same.

Answer»

Solution :(i) The work done by a force `vec(F)` for a displacement `d vec(r )` is
`W = int vec(F).d vec(r )""`…(1)
Left hand side of the EQUATION (1) can be written as
`W=int dW = int(dW)/(dt)dt`
(multiplied and DIVIDED by dt)` ""` .....(2)
(ii) Since, velocity is `vec(v)=(d vec(r ))/(dt),d vec(r )= vec(v )dt`. Right hand side of the equation (1) can be written as
`int vec(F).d vec(r )= int(vec(F).vec(v))dt[vec(v)=(d vec(r ))/(dt)]""` ....(3)
Substituting equations (2) and (3) in equation (1), we get
`int(dW)/(dt)dt = int (vec(F).vec(v))dt int((dW)/(dt)-vec(F).vec(v))dt = 0`
(iii)This relation is true for any ARBITRARY value of dt. This implies that the term within the bracket MUST be equal to zero, i.e.,
`(dW)/(dt)= vec(F).vec(v)=0`(or)`(dW)/(dt)=vec(F).vec(v)`


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