Moderate -0.3 This is a standard first-order linear vector differential equation (despite being written in second-order form, it reduces immediately by substituting v = dr/dt). The solution requires routine integration and application of initial conditions—slightly easier than average due to the straightforward structure and lack of non-homogeneous terms, though the vector notation and logarithmic time value add minor complexity.
2. At time \(t\) seconds, the position vector of a particle \(P\) is \(\mathbf { r }\) metres, where \(\mathbf { r }\) satisfies the differential equation
$$\frac { \mathrm { d } ^ { 2 } \mathbf { r } } { \mathrm {~d} t ^ { 2 } } + 3 \frac { \mathrm {~d} \mathbf { r } } { \mathrm {~d} t } = \mathbf { 0 }$$
When \(t = 0\), the velocity of \(P\) is \(( 8 \mathbf { i } - 12 \mathbf { j } ) \mathrm { m } \mathrm { s } ^ { - 1 }\).
Find the velocity of \(P\) when \(t = \frac { 2 } { 3 } \ln 2\).
(7)