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A particle is dropped from a tower in a uniform gravitational field at t = 0. The particle is blown over by a horizontal wind with constant velocity. The slope (m) of the trajectory of the particle with horizontal and its kinetic energy vary according to curves. Here, x is the horizontal displacement and h is the height of particle from ground at time t. |
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Answer»
Hence, for the particle, initial velocity `u = v_0` and angle of projection `theta = 0^@`. We know equation of trajectory is `y = x tan theta - (gx^2)/(2 u^2 cos^2 theta)` Here, `y = -(gx^2)/(2 v_0^2)` `("putting" theta = 0^@)` The slope of the trajectory of the particle is `(dy)/(dx) = -(2gx)/(2 v_0^2) = -(g)/(v_0^2) x` Hence, the curve between slope and `x` will be a straight line passing through the origin and will have a NEGATIVE slope. It means that option (b) is correct. Since horizontal velocity of the particle remains constant, `x = v_0 t`. We get `(dy)/(dx) = - ("gt")/(v_0)` So the graph between `m` and time `t` will have the same shape as the graph between `m and x`. Hence, option (a) is wrong. The vertical component of velocity OD the particle at time `t` is equal to `"gt"`. Hence, at time `t`, `KE = (1)/(2)m [("gt")^2 + (v_0)^2]` It means, the graph between `KE` and time `t` should be a parabola having value `(1)/(2) mv_0^2 at t = 0`. Therefore, option ( c) uis correct. As the particle falls, its HEIGHT decreases and `kE` increases. `KE = (1)/(2) mv_0^2 + mg (H - h)`, where `H` is the initial height. The `KE` increases linearly with height of its fall or the graph between `KE` and height of the particle will be a straight line having negative slope. Hence, option (d) is wrong. |
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