The position vector of a particle is r⃗ = 2t 2 x̂ + 3t ŷ + 4 ẑ. The

The position vector of a particle is r⃗ = 2t2 x̂ + 3t ŷ + 4 ẑ. Then the instantaneous velocity v⃗ and acceleration a⃗ respectively lie

on xy-plane and along z-direction
on yz-plane and along x-direction
on yz-plane and along y-direction
on xy-plane and along x-direction
This question was previously asked in
UPSC CDS-2 – 2018
The position vector is given by r⃗ = 2t² x̂ + 3t ŷ + 4 ẑ.
The instantaneous velocity vector v⃗ is the first derivative of the position vector with respect to time:
v⃗ = dr⃗/dt = d/dt (2t² x̂ + 3t ŷ + 4 ẑ) = (d/dt 2t²) x̂ + (d/dt 3t) ŷ + (d/dt 4) ẑ = 4t x̂ + 3 ŷ + 0 ẑ = 4t x̂ + 3 ŷ.
A vector of the form Ax̂ + Bŷ has components only in the x and y directions. Such a vector lies in the xy-plane.
The instantaneous acceleration vector a⃗ is the first derivative of the velocity vector with respect to time:
a⃗ = dv⃗/dt = d/dt (4t x̂ + 3 ŷ) = (d/dt 4t) x̂ + (d/dt 3) ŷ = 4 x̂ + 0 ŷ = 4 x̂.
A vector of the form Ax̂ has a component only in the x direction. Such a vector lies along the x-direction.
Therefore, the instantaneous velocity v⃗ lies on the xy-plane, and the instantaneous acceleration a⃗ lies along the x-direction.
– Velocity is the time derivative of the position vector.
– Acceleration is the time derivative of the velocity vector.
– A vector is in a plane if it has non-zero components only in the directions defining that plane.
– A vector is along an axis if it has a non-zero component only in the direction of that axis.
In this case, the position vector has a constant z-component (4). This means the particle is always located on the plane z=4, which is parallel to the xy-plane. The motion is confined to this plane z=4. The velocity vector (4t x̂ + 3 ŷ) correctly reflects motion in the x and y directions within this plane. The acceleration vector (4 x̂) indicates that the acceleration is constant and directed purely in the positive x-direction.