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Miscellaneous Examples · Example 31

Q.A water tank has the shape of an inverted right circular cone with its axis vertical and vertex lowermost. Its semi-vertical angle is tan⁡−1(0.5)\tan^{-1}(0.5). Water is poured into it at a constant rate of 55 cubic metre per hour. Find the rate at which the level of the water is rising at the instant when the depth of water in the tank is 44 m.

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Figure 6.20
Figure 6.20

The key idea is to relate the volume of water in the cone to its depth using the geometry of the cone, then differentiate with respect to time. The rate at which the water level rises when the depth is 4 m is 54π\frac{5}{4\pi} m/h.

This is a classic related rates problem. The core idea is simple: we know how fast the volume is changing (dV/dt=5dV/dt = 5 m³/h), and we want to find how fast the depth is changing (dh/dtdh/dt) at a specific moment. The bridge between these two rates is the geometric relationship between volume and depth for a cone.

The trick is that as water fills the cone, both the depth hh and the radius rr of the water's surface change together. But they aren't independent — the cone's fixed shape ties them together through the semi-vertical angle.

  1. Set up the geometry. The cone has a semi-vertical angle α\alpha where tan⁡α=0.5\tan \alpha = 0.5. From the figure, tan⁡α=r/h\tan \alpha = r/h, so:

rh=0.5⇒r=h2\frac{r}{h} = 0.5 \quad \Rightarrow \quad r = \frac{h}{2}

This is the crucial relation — at any depth hh, the radius of the water surface is exactly half of hh.

  1. Write the volume in terms of hh only. The volume of a cone is V=13πr2hV = \frac{1}{3}\pi r^2 h. Substitute r=h/2r = h/2:

V=13π(h2)2h=13π⋅h24⋅h=πh312V = \frac{1}{3}\pi \left(\frac{h}{2}\right)^2 h = \frac{1}{3}\pi \cdot \frac{h^2}{4} \cdot h = \frac{\pi h^3}{12}

V=πh312V = \frac{\pi h^3}{12}

This expresses the volume of water entirely in terms of its depth — no separate rr needed.

  1. Differentiate with respect to time. Both VV and hh are functions of time tt. Differentiate both sides:

dVdt=π12⋅3h2⋅dhdt=πh24⋅dhdt\frac{dV}{dt} = \frac{\pi}{12} \cdot 3h^2 \cdot \frac{dh}{dt} = \frac{\pi h^2}{4} \cdot \frac{dh}{dt}

  1. Plug in the known values. We are given dVdt=5\frac{dV}{dt} = 5 m³/h (constant), and we want dhdt\frac{dh}{dt} when h=4h = 4 m:

5=π(4)24⋅dhdt=π⋅164⋅dhdt=4π⋅dhdt5 = \frac{\pi (4)^2}{4} \cdot \frac{dh}{dt} = \frac{\pi \cdot 16}{4} \cdot \frac{dh}{dt} = 4\pi \cdot \frac{dh}{dt}

  1. Solve for the rate.

dhdt=54π m/h\frac{dh}{dt} = \frac{5}{4\pi} \text{ m/h}

Watch out

A common mistake is to treat rr as constant when differentiating V=13πr2hV = \frac{1}{3}\pi r^2 h. But rr changes with hh! Always eliminate rr (or hh) using the cone's geometry before differentiating — otherwise you'll need the product rule and an extra relation.

Tip

Notice that the answer doesn't depend on the cone's full size — only on its shape (the semi-vertical angle). The rate 54π\frac{5}{4\pi} is about 0.398 m/h, which makes sense: a wide, shallow cone (tan α = 0.5 means the radius grows slowly with depth) would have the water level rise relatively fast for a given inflow.

✓Final answer

The rate at which the water level is rising when the depth is 4 m is 54π m/h\boxed{\frac{5}{4\pi} \text{ m/h}}.

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