โˆซCalculus I

Related Rates Problems

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Why This Matters

Related rates problems test whether you can apply derivative rules to real-world scenarios, not just compute them mechanically. You start with a physical situation where multiple quantities change over time, connect those quantities through an equation, then use implicit differentiation and the chain rule to find how fast one quantity changes given information about another.

The core skills here are implicit differentiation, the chain rule, and geometric reasoning. Whether it's a ladder sliding down a wall or water draining from a tank, the underlying principle is the same: if two quantities are related by an equation, their rates of change are also related. Don't just memorize problem types. Understand why you set up each equation and how the chain rule connects dVdt\frac{dV}{dt} to drdt\frac{dr}{dt} or dhdt\frac{dh}{dt}.

  1. Draw a diagram and label all quantities that change with time as variables (not numbers).
  2. Write an equation relating the variables. This comes from geometry, physics, or whatever the problem describes.
  3. Eliminate extra variables if possible. Use a constraint (like similar triangles) to reduce to fewer variables before differentiating.
  4. Differentiate both sides with respect to tt, applying the chain rule to every variable that depends on time.
  5. Substitute known values (the specific measurements and rates given in the problem) after differentiating.
  6. Solve for the unknown rate.

A very common mistake is plugging in numbers before differentiating. Once you substitute a constant for a variable, its derivative becomes zero, and you lose information.


Pythagorean Relationship Problems

These problems involve right triangles where two sides change over time while satisfying a2+b2=c2a^2 + b^2 = c^2. Differentiating this constraint links the rates of change of perpendicular distances.

Ladder Sliding Down a Wall

The Pythagorean theorem x2+y2=L2x^2 + y^2 = L^2 relates the distance from the wall (xx), height on the wall (yy), and ladder length (LL). Since LL is constant, implicit differentiation gives:

2xdxdt+2ydydt=02x\frac{dx}{dt} + 2y\frac{dy}{dt} = 0

Notice the rates have opposite signs. As the base slides out (dxdt>0\frac{dx}{dt} > 0), the top slides down (dydt<0\frac{dy}{dt} < 0). The ladder also accelerates as it falls: dydt\frac{dy}{dt} approaches negative infinity as yโ†’0y \to 0. Exam problems sometimes ask you to explain this behavior.

Distance Between Two Moving Objects

Set up coordinates so each object's position is a function of time. The distance formula D=(x2โˆ’x1)2+(y2โˆ’y1)2D = \sqrt{(x_2-x_1)^2 + (y_2-y_1)^2} must be differentiated using the chain rule.

A useful trick: square both sides first to get D2=(x2โˆ’x1)2+(y2โˆ’y1)2D^2 = (x_2-x_1)^2 + (y_2-y_1)^2. This avoids messy square root derivatives. Then differentiate:

2DdDdt=2(x2โˆ’x1)(dx2dtโˆ’dx1dt)+2(y2โˆ’y1)(dy2dtโˆ’dy1dt)2D\frac{dD}{dt} = 2(x_2-x_1)\left(\frac{dx_2}{dt}-\frac{dx_1}{dt}\right) + 2(y_2-y_1)\left(\frac{dy_2}{dt}-\frac{dy_1}{dt}\right)

Compare: Ladder problems vs. distance problems: both use Pythagorean relationships, but ladders have a constant hypotenuse while distance problems often have all three quantities changing. On FRQs, check whether any length is fixed before differentiating.


Similar Triangle Problems

When objects cast shadows or light creates geometric relationships, similar triangles provide the equation you need. The ratios of corresponding sides remain equal, giving you a proportion to differentiate.

Shadow Length Problems

Similar triangles relate the height of the light source, object height, and shadow length through proportional ratios. A typical setup:

Hx+s=hs\frac{H}{x+s} = \frac{h}{s}

where HH is the light height, hh is the object height, ss is the shadow length, and xx is the distance from the light to the object. Cross-multiply before differentiating to eliminate fractions, which makes the implicit differentiation much cleaner.

Angle Change in a Triangle with Moving Sides

When a problem involves a changing angle in a non-right triangle, the Law of Cosines provides the relationship:

c2=a2+b2โˆ’2abcosโก(ฮธ)c^2 = a^2 + b^2 - 2ab\cos(\theta)

Differentiating implicitly connects dฮธdt\frac{d\theta}{dt} to the rates of change of the sides. Remember that ddt[cosโก(ฮธ)]=โˆ’sinโก(ฮธ)dฮธdt\frac{d}{dt}[\cos(\theta)] = -\sin(\theta)\frac{d\theta}{dt}, so trigonometric derivatives will appear.

Compare: Shadow problems vs. angle problems: shadow problems typically use ratios from similar triangles while angle problems require the Law of Cosines or Sines. If the problem mentions an angle explicitly, reach for trig laws.


Spherical Volume Problems

Spheres appear frequently because V=43ฯ€r3V = \frac{4}{3}\pi r^3 creates a clean relationship between volume and radius. Applying the chain rule:

dVdt=4ฯ€r2drdt\frac{dV}{dt} = 4\pi r^2 \frac{dr}{dt}

The coefficient 4ฯ€r24\pi r^2 is the surface area of the sphere. This isn't a coincidence: volume changes occur through the surface.

Changing Radius of a Sphere or Circle

  • For spheres: V=43ฯ€r3V = \frac{4}{3}\pi r^3 differentiates to dVdt=4ฯ€r2drdt\frac{dV}{dt} = 4\pi r^2 \frac{dr}{dt}
  • For circles: A=ฯ€r2A = \pi r^2 gives dAdt=2ฯ€rdrdt\frac{dA}{dt} = 2\pi r \frac{dr}{dt}
  • Watch your units: if rr is in cm and tt is in seconds, dVdt\frac{dV}{dt} is in cm3/s\text{cm}^3/\text{s}

Expanding or Contracting Balloon

The formula is the same as any sphere problem, but context determines the sign. Air pumped in means dVdt>0\frac{dV}{dt} > 0; air escaping means dVdt<0\frac{dV}{dt} < 0.

An important conceptual point: the rate of radius change decreases as the balloon grows. Even with constant dVdt\frac{dV}{dt}, a larger rr means a larger 4ฯ€r24\pi r^2 in the denominator when you solve for drdt\frac{dr}{dt}, so drdt\frac{dr}{dt} gets smaller.

Growing Snowball

The setup is identical to balloon problems, but snow accumulation is typically given as a volume rate. If the problem describes snow sticking to the surface at a rate per unit area, you'll need to multiply by the surface area 4ฯ€r24\pi r^2 to get dVdt\frac{dV}{dt}.

A common variation: "the radius grows at a constant rate." Here you're finding dVdt=4ฯ€r2drdt\frac{dV}{dt} = 4\pi r^2 \frac{dr}{dt}, which increases over time because rr is growing while drdt\frac{dr}{dt} stays fixed.

Compare: Balloon vs. snowball problems are mathematically identical, but balloons often give dVdt\frac{dV}{dt} and ask for drdt\frac{dr}{dt}, while snowball problems sometimes reverse this. Always identify what's given vs. what's asked.


Conical Tank Problems

Cones are trickier than cylinders because radius and height are both changing. You must use similar triangles to eliminate one variable before differentiating.

Filling or Draining Tanks (Cylindrical, Conical, or Spherical)

  • For cylinders with fixed radius: V=ฯ€r2hV = \pi r^2 h simplifies to dVdt=ฯ€r2dhdt\frac{dV}{dt} = \pi r^2 \frac{dh}{dt}
  • For cones: the ratio rh\frac{r}{h} is fixed by the tank's shape. If the tank has radius RR at height HH, then r=RHhr = \frac{R}{H}h. Substituting gives V=13ฯ€(RH)2h3V = \frac{1}{3}\pi \left(\frac{R}{H}\right)^2 h^3
  • Differentiate the simplified formula: dVdt=ฯ€(RH)2h2dhdt\frac{dV}{dt} = \pi \left(\frac{R}{H}\right)^2 h^2 \frac{dh}{dt}, then solve for the unknown rate

Water Leaking from an Inverted Conical Tank

"Inverted cone" means vertex at the bottom, so water forms a smaller cone that is similar to the tank. Find the ratio rh=RH\frac{r}{h} = \frac{R}{H} where RR and HH are the tank's full dimensions, then substitute to eliminate rr.

Height changes faster when water is low (small hh) because the cross-sectional area ฯ€r2\pi r^2 is smaller there. The same volume leaving the tank causes a bigger drop in height when the cone is narrow near the bottom. This is a frequent conceptual question.

Compare: Cylindrical vs. conical tanks: cylinders have constant cross-sectional area, so dhdt\frac{dh}{dt} is constant for constant dVdt\frac{dV}{dt}. Cones have variable cross-sections, making dhdt\frac{dh}{dt} depend on the current water level. FRQs love asking why the rate changes.


Cylindrical Volume Problems

Cylinders with changing dimensions require the product rule since V=ฯ€r2hV = \pi r^2 h involves two variables. When both rr and hh change:

dVdt=ฯ€(2rhdrdt+r2dhdt)\frac{dV}{dt} = \pi\left(2rh\frac{dr}{dt} + r^2\frac{dh}{dt}\right)

Volume Change in a Cylinder with Varying Dimensions

  • Product rule is essential when both radius and height vary. The formula above comes from differentiating r2โ‹…hr^2 \cdot h as a product (where r2r^2 itself requires the chain rule).
  • If only height changes (fixed radius), this simplifies to dVdt=ฯ€r2dhdt\frac{dV}{dt} = \pi r^2 \frac{dh}{dt}
  • Check for constraints: sometimes rr and hh are related (e.g., r=2hr = 2h), requiring substitution before differentiation, just like in cone problems

Compare: Single-variable vs. multi-variable cylinder problems: when only one dimension changes, you get a simple chain rule application. When both change, you need the product rule and the chain rule together. Read carefully to determine which case applies.


Quick Reference Table

ConceptBest Examples
Pythagorean constraintLadder, distance between objects
Similar trianglesShadow length, conical tanks
Spherical volume (V=43ฯ€r3V = \frac{4}{3}\pi r^3)Balloon, snowball, sphere radius
Conical volume with ratio constraintInverted cone, draining tanks
Product rule for multiple variablesCylinder with varying rr and hh
Trigonometric relationshipsAngle change, rotating objects
Constant quantity identificationLadder length, tank dimensions
Sign interpretationDraining (negative) vs. filling (positive)

Self-Check Questions

  1. Both the ladder problem and the distance-between-objects problem use the Pythagorean theorem. What's the key difference in how you set up the differentiation for each?

  2. In a conical tank problem, why must you express rr in terms of hh (or vice versa) before differentiating? What geometric principle allows you to do this?

  3. Compare a balloon being inflated at a constant volume rate to a snowball whose radius grows at a constant rate. In which scenario does dVdt\frac{dV}{dt} increase over time, and why?

  4. An FRQ asks: "Explain why the water level in a conical tank drops faster when the tank is nearly empty than when it's nearly full, even if water drains at a constant rate." How would you answer this using your related rates setup?

  5. For a cylinder where both radius and height change over time, write out dVdt\frac{dV}{dt} and identify which differentiation rule(s) you used. How does this differ from the sphere case?