Jordans Math Work Apr 2026

We need: [ \frac{dr}{dt} \quad \text{when} \quad r = 4 , \text{cm}. ] For a sphere: [ V = \frac{4}{3} \pi r^3 ] Step 3: Differentiate with respect to time ( t ). Using the chain rule: [ \frac{dV}{dt} = \frac{dV}{dr} \cdot \frac{dr}{dt} = 4\pi r^2 \cdot \frac{dr}{dt} ] Step 4: Plug in known values. At the instant ( r = 4 , \text{cm} ): [ 4.5 = 4\pi (4^2) \cdot \frac{dr}{dt} ] [ 4.5 = 4\pi (16) \cdot \frac{dr}{dt} ] [ 4.5 = 64\pi \cdot \frac{dr}{dt} ] Step 5: Solve for ( \frac{dr}{dt} ). [ \frac{dr}{dt} = \frac{4.5}{64\pi} = \frac{9}{128\pi} , \text{cm/s} ] Step 6: Simplify and interpret. [ \frac{dr}{dt} \approx \frac{9}{402.1239} \approx 0.0224 , \text{cm/s} ] So the radius is increasing at about ( 0.0224 , \text{cm/s} ) when the diameter is 8 cm. Step 7: Check for reasonableness. The rate is positive (radius increases), and the number is small compared to the inflation rate, which makes sense because volume grows as ( r^3 ), so changes in ( r ) are slower. Conclusion: Jordan solved the related rates problem by differentiating the volume formula, substituting given values, and solving for ( \frac{dr}{dt} ). The final exact answer is ( \frac{9}{128\pi} , \text{cm/s} ), approximately ( 0.0224 , \text{cm/s} ). If you meant a different kind of “long write-up” (e.g., a personal reflection on math, a multi-step algebra problem, geometry proof, or statistics project), just let me know and I can tailor it exactly to what Jordan is working on.

Here’s a sample write-up for a calculus problem (related rates) as if written by Jordan: jordans math work

Air is being pumped into a spherical balloon at a rate of ( 4.5 , \text{cm}^3/\text{s} ). Find the rate at which the radius of the balloon is increasing when the diameter is ( 8 , \text{cm} ). Step 1: Understand the given and unknown quantities. We are given: [ \frac{dV}{dt} = 4.5 , \text{cm}^3/\text{s} \quad (\text{rate of change of volume}) ] Diameter ( D = 8 , \text{cm} ) means radius ( r = 4 , \text{cm} ) at the moment of interest. We need: [ \frac{dr}{dt} \quad \text{when} \quad r