The Geometry of Growth
An Expanding Cube
Imagine you are standing in a laboratory, watching a perfect, crystalline cube grow. It is not just getting bigger; it is expanding uniformly, maintaining its perfect cubic symmetry at every single microsecond.
This is the essence of a 'related rates' problem in calculus. We are not just looking at static shapes; we are looking at the dynamic, living pulse of geometry.
The Foundation
To understand this expansion, we must first define the 'DNA' of our cube. Let a be the side length of the cube at any given moment t.
The surface area
A is the sum of the areas of its six square faces, giving us the elegant relation:
A=6a2
Simultaneously, the volume
V, the space contained within this expanding boundary, is defined by:
V=a3
These two equations are the bedrock of our journey. They link the two-dimensional 'skin' of the cube to its three-dimensional 'heart.'
The Chain Rule Bridge
We are given that the surface area is increasing at a constant rate: dtdA=3.6 cm2/sec. Our mission is to find the rate of change of the volume, dtdV, at the exact instant when a=10 cm.
To get from the surface area to the volume, we need a translator. That translator is the rate of change of the side length, dtda.
We start by differentiating our surface area equation with respect to time
t. Using the chain rule, we get:
dtdA=dtd(6a2)=12adtda
This is the moment where many students stumble. Do not forget that a is a function of time! The derivative of a2 is not just 2a; it is 2a⋅dtda. This is the heartbeat of the problem.
The Connection
Now, we substitute our known rate,
dtdA=3.6, into our derivative equation:
3.6=12adtda
Solving for
dtda, we find:
dtda=12a3.6=a0.3
This expression, dtda=a0.3, is our golden key. It tells us exactly how fast the side length is growing at any size a.
The Volume Synthesis
Now, we turn to the volume. We differentiate
V=a3 with respect to time
t:
dtdV=3a2dtda
Here is the magic. We can substitute our expression
dtda=a0.3 directly into this equation:
dtdV=3a2(a0.3)
Watch the algebra collapse beautifully. One
a in the denominator cancels one
a in the numerator, leaving us with:
dtdV=3a×0.3=0.9a
The Final Climax
We have arrived at a simple, linear relationship: the rate of change of volume is exactly
0.9 times the current side length. Now, we simply plug in the value given in the problem,
a=10 cm:
dtdV=0.9×10=9 cm3/sec
And there it is. At the moment the side length is 10 cm, the volume is expanding at 9 cm3/sec. You have successfully navigated the relationship between surface area and volume, using the chain rule to bridge the gap.