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A-small-particle-of-mass-m-is-projected-at-an-angle-with-the-x-axis-with-an-initial-velocity-v-0-in-the-x-y-plane-as-shown-in-the-Figure-At-a-time-t-lt-v-0-sin-g-the-angular-momentum-of-




Question Number 20375 by Tinkutara last updated on 26/Aug/17
A small particle of mass m is projected  at an angle θ with the x-axis with an  initial velocity v_0  in the x-y plane as  shown in the Figure. At a time  t < ((v_0  sin θ)/g), the angular momentum of  the particle is
$$\mathrm{A}\:\mathrm{small}\:\mathrm{particle}\:\mathrm{of}\:\mathrm{mass}\:{m}\:\mathrm{is}\:\mathrm{projected} \\ $$$$\mathrm{at}\:\mathrm{an}\:\mathrm{angle}\:\theta\:\mathrm{with}\:\mathrm{the}\:{x}-\mathrm{axis}\:\mathrm{with}\:\mathrm{an} \\ $$$$\mathrm{initial}\:\mathrm{velocity}\:{v}_{\mathrm{0}} \:\mathrm{in}\:\mathrm{the}\:{x}-{y}\:\mathrm{plane}\:\mathrm{as} \\ $$$$\mathrm{shown}\:\mathrm{in}\:\mathrm{the}\:\mathrm{Figure}.\:\mathrm{At}\:\mathrm{a}\:\mathrm{time} \\ $$$${t}\:<\:\frac{{v}_{\mathrm{0}} \:\mathrm{sin}\:\theta}{{g}},\:\mathrm{the}\:\mathrm{angular}\:\mathrm{momentum}\:\mathrm{of} \\ $$$$\mathrm{the}\:\mathrm{particle}\:\mathrm{is} \\ $$
Commented by Tinkutara last updated on 26/Aug/17
Answered by ajfour last updated on 26/Aug/17
L^� =∫_0 ^(  t) (xi^� +yj^� )×(−mgj^� )dt      =−∫_0 ^(  t) [(v_0 cos θ)(mg)k^� ]tdt     =−(mgv_0 cos θ)(t^2 /2)k^�      ∣L^� ∣=(1/2)(mgv_0 cos θ)t^2  .
$$\bar {{L}}=\int_{\mathrm{0}} ^{\:\:{t}} \left({x}\hat {{i}}+{y}\hat {{j}}\right)×\left(−{mg}\hat {{j}}\right){dt} \\ $$$$\:\:\:\:=−\int_{\mathrm{0}} ^{\:\:{t}} \left[\left({v}_{\mathrm{0}} \mathrm{cos}\:\theta\right)\left({mg}\right)\hat {{k}}\right]{tdt} \\ $$$$\:\:\:=−\left({mgv}_{\mathrm{0}} \mathrm{cos}\:\theta\right)\frac{{t}^{\mathrm{2}} }{\mathrm{2}}\hat {{k}}\: \\ $$$$\:\:\mid\bar {{L}}\mid=\frac{\mathrm{1}}{\mathrm{2}}\left({mgv}_{\mathrm{0}} \mathrm{cos}\:\theta\right){t}^{\mathrm{2}} \:. \\ $$
Commented by Tinkutara last updated on 26/Aug/17
Thank you very much Sir!
$$\mathrm{Thank}\:\mathrm{you}\:\mathrm{very}\:\mathrm{much}\:\mathrm{Sir}! \\ $$

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