Challenging +1.2 This is a second-order vector differential equation requiring complementary function (CF) and particular integral (PI) with initial conditions. While it involves multiple steps (finding CF with auxiliary equation, finding PI for exponential forcing, applying two initial conditions), the techniques are standard for Further Maths mechanics. The vector form adds mild complexity but components separate independently. More challenging than routine integration but less demanding than proof-based or multi-concept synthesis questions.
2. At time \(t\) seconds, the position vector of a particle \(P\) is \(\mathbf { r }\) metres, where \(\mathbf { r }\) satisfies the vector differential equation
$$\frac { \mathrm { d } ^ { 2 } \mathbf { r } } { \mathrm {~d} t ^ { 2 } } + 4 \mathbf { r } = \mathrm { e } ^ { 2 t } \mathbf { j }$$
When \(t = 0 , P\) has position vector \(( \mathbf { i } + \mathbf { j } ) \mathrm { m }\) and velocity \(2 \mathbf { i } \mathrm {~m} \mathrm {~s} ^ { - 1 }\).
Find an expression for \(\mathbf { r }\) in terms of \(t\).
2. At time $t$ seconds, the position vector of a particle $P$ is $\mathbf { r }$ metres, where $\mathbf { r }$ satisfies the vector differential equation
$$\frac { \mathrm { d } ^ { 2 } \mathbf { r } } { \mathrm {~d} t ^ { 2 } } + 4 \mathbf { r } = \mathrm { e } ^ { 2 t } \mathbf { j }$$
When $t = 0 , P$ has position vector $( \mathbf { i } + \mathbf { j } ) \mathrm { m }$ and velocity $2 \mathbf { i } \mathrm {~m} \mathrm {~s} ^ { - 1 }$.
Find an expression for $\mathbf { r }$ in terms of $t$.\\
\hfill \mbox{\textit{Edexcel M5 2009 Q2 [11]}}