In the realm of vector applications to kinematics, we begin by examining linear motion with constant velocity in two and three dimensions. This fundamental concept forms the basis for more complex motion analysis.
In a two-dimensional plane, we can represent the position of an object at any time $t$ using the vector equation:
$$\mathbf{r}(t) = \mathbf{r}_0 + \mathbf{v}t$$
Where:
Consider a car moving with a constant velocity of 5 m/s east and 3 m/s north. If its initial position is at (2, 1), its position after 4 seconds can be calculated as:
$\mathbf{r}(4) = (2, 1) + (5, 3) \cdot 4 = (2, 1) + (20, 12) = (22, 13)$
The car will be at position (22, 13) after 4 seconds.
The same principle extends to three-dimensional space, where we add a z-component to our vectors:
$$\mathbf{r}(t) = \mathbf{r}_0 + \mathbf{v}t = (x_0, y_0, z_0) + (v_x, v_y, v_z)t$$
The beauty of vector notation is that it allows us to treat multi-dimensional motion with the same simplicity as one-dimensional motion.
Using the vector equation of motion, we can solve various problems related to positions and intersections of moving objects.
To find where two objects' paths intersect, we set their position vectors equal to each other and solve for time:
$$\mathbf{r}_1(t) = \mathbf{r}_2(t)$$
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