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(i) Order and Degree:
The given differential equation is $\frac{dV}{dt} = kS$. Since it involves the first derivative of V with respect to t, the order is 1. The power of the highest order derivative is also 1, so the degree is 1.
(ii) Solving the differential equation:
Given $V = \pi r^3$ and $S = 2\pi r^2$, we have $\frac{dV}{dt} = \frac{dV}{dr} \cdot \frac{dr}{dt} = 3\pi r^2 \frac{dr}{dt}$.
Substituting into the given differential equation: $3\pi r^2 \frac{dr}{dt} = k(2\pi r^2)$.
Simplifying, we get $\frac{dr}{dt} = \frac{2}{3}k$.
Integrating both sides with respect to t: $\int dr = \int \frac{2}{3}k dt$.
This gives $r = \frac{2}{3}kt + C$, where C is the constant of integration.
Given $r(0) = 5$ mm, we substitute $t = 0$ and $r = 5$ into the equation: $5 = \frac{2}{3}k(0) + C$, so $C = 5$.
Thus, the solution is $r = \frac{2}{3}kt + 5$.
(iii) (a) Finding k and t for r = 0:
Given $r = 3$ mm when $t = 1$ hour, we substitute these values into the equation: $3 = \frac{2}{3}k(1) + 5$.
Solving for k: $\frac{2}{3}k = -2$, so $k = -3$ mm/hour.
Now, we want to find t when $r = 0$: $0 = \frac{2}{3}(-3)t + 5$, which simplifies to $0 = -2t + 5$.
Solving for t: $2t = 5$, so $t = \frac{5}{2} = 2.5$ hours.
OR (iii) (b) Finding k and t for r = 0:
Given $r = 1$ mm when $t = 1$ hour, we substitute these values into the equation: $1 = \frac{2}{3}k(1) + 5$.
Solving for k: $\frac{2}{3}k = -4$, so $k = -6$ mm/hour.
Now, we want to find t when $r = 0$: $0 = \frac{2}{3}(-6)t + 5$, which simplifies to $0 = -4t + 5$.
Solving for t: $4t = 5$, so $t = \frac{5}{4} = 1.25$ hours.
Correct Answer: (i) Order: 1, Degree: 1 (ii) r = (2/3)kt + 5 (iii) (a) k = -3, t = 2.5 hours OR (iii) (b) k = -6, t = 1.25 hours <\/strong>