00:01
Hi students, the components of acceleration on the particle, ax equal to g goes alpha and a is equal to minus g sine alpha.
00:17
Initial components of velocity, v0x is equal to v0 sine theta and v0 z equal to v0 cos theta.
00:32
Using the kinematic equations of motion, the x and z components of velocity as a function of time, vx is equal to v0x plus a xt implies vx equal to v0 sine theta plus g cos alpha t and vz equal to v0.
01:04
Z plus a zz of t which implies vzz equal to v0 cos theta minus g sine alpha t let this be equation number one and this be two and the displacement as a function of time x is equal to v0 x plus a x t square by two x x is equal to v0 x plus a x t square by two x x is equal to to v0 sine theta into t plus g cosa alpha t square by 2 that is this equation number 3 and is that equal to v0 cos theta into t plus minus of g sine alpha t square by 2 that can be written as v0 cost theta into t minus g sine alpha t square by 2 this be equation number 4 again components of velocity as a function of distance is v x square equal to v0 x square plus 2 a x into x therefore vx square equal to v x x squared equal to v0 sine theta the whole square plus 2g cos alpha x this is equation number 5 and vz square equal to v0 cos theta the whole square minus 2 g sine alpha z this is equation number 6 for the a part at maximum separation between the projectile and the hill, z will be z max and vz equal to 0.
03:26
From equation number 6, 0 equal to v0 cos theta the whole square minus 2g sine alpha z max where z max is equal to v0 cost theta of the whole square divided by 2g sine alpha which is equal to 4 into cos 30 the whole square divided by 2 into 9 .8 into sine 45 which on solving is obtained as 0 .87 meters.
04:13
Moving on to the b part, let the projectile lands at time t equal to t...