Before you begin
- Chain rule and elementary plane and solid geometry.
Learning objectives
- Differentiate an equation that defines a local function implicitly.
- Distinguish derivative failure from failure of a chosen coordinate representation.
- Solve related-rate models with correct signs and units.
A circle cannot be represented by one real function over its entire horizontal span: most horizontal positions have two vertical coordinates. It can nevertheless have well-defined tangent lines on its local branches. An equation relating the variables can retain information that solving explicitly would split into cases.
Differentiating a constraint
For , treat as a differentiable function of on a branch. Differentiation gives , hence
At , the slope is , so the tangent is . At , the formula cannot produce a finite slope for as a function of . The circle still has a tangent, namely the vertical line . A failure of this coordinate representation is not a disappearance of the geometric curve.
For a general differentiable equation , the chain rule gives when the partial derivatives are defined, leading formally to where . A local implicit function theorem supplies sufficient conditions for such a branch to exist. In this course, polynomial and elementary examples will also be checked directly when possible; the displayed ratio should not be treated as an unconditional existence theorem.
A second derivative needs the chain rule again
From the circle’s , the quotient rule gives
The first equality differentiates as a function rather than freezing it as a constant. At , this is . The upper branch is concave down there, consistent with its geometry.
Rates share a clock
In a related-rate problem, several quantities depend on the same time variable. Write the constraint between them, then differentiate with respect to time. For a spherical balloon with radius and volume ,
If the radius is centimetres and volume is increasing at cubic centimetres per second, then centimetres per second. Substituting before differentiating would turn volume into a constant and destroy the time dependence we need.
A sliding ladder
A rigid ladder of length metres touches a horizontal floor and vertical wall. Let be the foot’s distance from the wall and the top’s height. While the geometric model applies, and
At , , and metres per second, the top moves at metres per second. The sign describes downward motion. Its downward speed is metres per second.
As with fixed positive , the formula predicts unbounded downward rate. That signals a limitation of extending this idealized contact-and-constant-foot-speed model to the final configuration. Real mechanics, contact forces, and finite energy may invalidate the imposed rate before that limit. Mathematics can expose a model’s consequences without certifying its physical continuation.
Organizing a modeling solution
Define variables and units; identify the instant; draw or describe the geometry; write the constraint; differentiate while quantities are still functions; substitute the instant’s values; solve for the requested rate; interpret its sign and domain. A clear equation often does more work than a memorized “related rates” formula.
Exercises
- Find the tangent slope to at by implicit differentiation.
- Find for , wherever the denominator is nonzero.
- A circle’s radius increases at centimetres per second. Find its area rate when centimetres.
- Repeat the ladder calculation when , .
- Explain why a rate measured in cubic metres per second cannot be reported as a radius rate without an additional geometric factor.
- For the upper semicircle , verify the implicit derivative by explicit differentiation.
Worked solutions
- gives .
- , so .
- square centimetres per second.
- , hence metres per second.
- Volume and length are different quantities. For a sphere the conversion factor is , with inverse-area units.
- The chain rule gives for .