Rate of Change — Volume of Sphere When Radius Increases

easy CBSE JEE-MAIN NCERT Class 12 3 min read

Question

The radius of a sphere is increasing at the rate of 0.2 cm/s. At what rate is the volume of the sphere increasing when the radius is 15 cm?


Solution — Step by Step

We have drdt=0.2\frac{dr}{dt} = 0.2 cm/s (radius increasing over time), and we need dVdt\frac{dV}{dt} when r=15r = 15 cm. This is a classic “related rates” setup — two quantities both changing with time, connected through a formula.

Volume of a sphere: V=43πr3V = \frac{4}{3}\pi r^3

We differentiate both sides with respect to time tt, not with respect to rr. This is where the chain rule enters.

dVdt=ddt(43πr3)=43π3r2drdt\frac{dV}{dt} = \frac{d}{dt}\left(\frac{4}{3}\pi r^3\right) = \frac{4}{3}\pi \cdot 3r^2 \cdot \frac{dr}{dt}

Simplifying: dVdt=4πr2drdt\frac{dV}{dt} = 4\pi r^2 \cdot \frac{dr}{dt}

Notice that 4πr24\pi r^2 is simply the surface area of the sphere — that’s not a coincidence, and we’ll come back to it.

At r=15r = 15 cm and drdt=0.2\frac{dr}{dt} = 0.2 cm/s:

dVdt=4π(15)2×0.2=4π×225×0.2=180π\frac{dV}{dt} = 4\pi (15)^2 \times 0.2 = 4\pi \times 225 \times 0.2 = 180\pi

The volume is increasing at 180π180\pi cm³/s ≈ 565.5 cm³/s.


Why This Works

When we differentiate V=43πr3V = \frac{4}{3}\pi r^3 with respect to tt, the chain rule forces us to multiply by drdt\frac{dr}{dt}. We’re not asking “how does VV change as rr changes?” — we’re asking “how does VV change as time passes?” That extra drdt\frac{dr}{dt} converts the spatial relationship into a time-based one.

The result dVdt=4πr2drdt\frac{dV}{dt} = 4\pi r^2 \cdot \frac{dr}{dt} has a beautiful interpretation: the surface area of the sphere acts as the multiplier. Think of it this way — a thin shell of thickness drdr added to a sphere of radius rr has volume 4πr2dr\approx 4\pi r^2 \cdot dr. That’s exactly what we’re computing when rr grows by drdr in time dtdt.

This formula appears in NCERT Chapter 6 and has shown up in CBSE board papers almost every alternate year since 2018. At large rr, even a slow drdt\frac{dr}{dt} produces a huge dVdt\frac{dV}{dt} — because the surface area is large.


Alternative Method

If you’re comfortable with direct substitution, skip the general formula and differentiate directly after substituting r=15r = 15. Warning: this only works when rr is a constant value at the specific instant — you cannot simplify rr before differentiating if it’s a function of time.

Alternatively, express VV in terms of tt symbolically. If r(t)=r0+0.2tr(t) = r_0 + 0.2t, then V(t)=43π(r0+0.2t)3V(t) = \frac{4}{3}\pi(r_0 + 0.2t)^3. Differentiating: dVdt=43π3(r0+0.2t)20.2\frac{dV}{dt} = \frac{4}{3}\pi \cdot 3(r_0 + 0.2t)^2 \cdot 0.2, which at r=15r = 15 gives the same 180π180\pi.

This approach is more verbose but makes the time-dependence explicit — useful if you want to verify your chain rule work.


Common Mistake

Differentiating with respect to rr instead of tt.

Students write dVdr=4πr2\frac{dV}{dr} = 4\pi r^2 and then just multiply by 0.2 without justification. This accidentally gives the right answer here — but only because dVdt=dVdrdrdt\frac{dV}{dt} = \frac{dV}{dr} \cdot \frac{dr}{dt} and drdt=0.2\frac{dr}{dt} = 0.2. In an exam, you must show the chain rule step explicitly: write dVdt=4πr2drdt\frac{dV}{dt} = 4\pi r^2 \cdot \frac{dr}{dt}, then substitute. Skipping this step costs marks in CBSE board evaluation.

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