This solution details the calculation for centrifugal force per unit mass acting on air within a low-pressure centre.
Centrifugal force per unit mass is equivalent to centrifugal acceleration ($a_c$). This outward force arises from the inertia of the air moving along a curved path around the low-pressure centre.
The formula for centrifugal acceleration is:
$a_c = \frac{v^2}{r}$
Where:
Wind speed, $v = 10 \text{ m.s}^{-1}$.
Distance from centre, $r = 250 \text{ km}$.
Convert the distance $r$ to meters for consistency:
$r = 250 \text{ km} \times 1000 \text{ m/km} = 250,000 \text{ m} = 2.5 \times 10^5 \text{ m}$.
Substitute the values into the formula:
$a_c = \frac{(10 \text{ m.s}^{-1})^2}{2.5 \times 10^5 \text{ m}} = \frac{100 \text{ m}^2\text{s}^{-2}}{2.5 \times 10^5 \text{ m}}$
$a_c = \frac{1 \times 10^2}{2.5 \times 10^5} \text{ m.s}^{-2} = 0.4 \times 10^{-3} \text{ m.s}^{-2}$
$a_c = 4 \times 10^{-4} \text{ m.s}^{-2}$
In atmospheric dynamics concerning low-pressure systems, forces directed towards the centre (like the pressure gradient force) are often considered positive. Since centrifugal force acts outwards, it is conventionally represented with a negative sign in this context.
Therefore, the centrifugal force per unit mass is $-4 \times 10^{-4} \text{ m.s}^{-2}$.