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The velocity vector of a typical projectile can be broken into two components: horizontal component of velocity and vertical component of velocity. Assuming negligible air

The velocity vector of a typical projectile can be broken into two components: horizontal component of velocity and vertical component of velocity. Assuming negligible air resistance, there will be no horizontal force acting on the projectile. This means during projectile motion the horizontal component of its velocity will increase O decrease not change O increase first, and then become zero

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