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The height of a river above a fixed point on the riverbed was monitored over a 7-day period.
The height of the river, 
H metres, 
t days after monitoring began, was given by


H=(sqrtt)/(20)(20+6t-t^(2))+17quad0 <= t <= 7
Given that 
H has a stationary value at 
t=alpha
(a) use calculus to show that 
alpha satisfies the equation

5alpha^(2)-18 alpha-20=0

The height of a river above a fixed point on the riverbed was monitored over a 77-day period. The height of the river, HH metres, tt days after monitoring began, was given by\newlineH=t20(20+6tt2)+170t7H=\frac{\sqrt{t}}{20}(20+6t-t^{2})+17\quad 0 \leq t \leq 7\newlineGiven that HH has a stationary value at t=αt=\alpha\newline(a) use calculus to show that α\alpha satisfies the equation\newline5α218α20=05\alpha^{2}-18\alpha-20=0

Full solution

Q. The height of a river above a fixed point on the riverbed was monitored over a 77-day period. The height of the river, HH metres, tt days after monitoring began, was given by\newlineH=t20(20+6tt2)+170t7H=\frac{\sqrt{t}}{20}(20+6t-t^{2})+17\quad 0 \leq t \leq 7\newlineGiven that HH has a stationary value at t=αt=\alpha\newline(a) use calculus to show that α\alpha satisfies the equation\newline5α218α20=05\alpha^{2}-18\alpha-20=0
  1. Differentiate with Quotient Rule: To find the stationary value of HH, we need to differentiate HH with respect to tt and set the derivative equal to 00.
  2. Calculate Derivatives: Differentiate HH with respect to tt using the quotient rule: ddt[t20(20+6tt2)]\frac{d}{dt}\left[\frac{\sqrt{t}}{20}(20+6t-t^2)\right].
  3. Apply Quotient Rule Formula: Let u=tu = \sqrt{t} and v=(20)(20+6tt2)v = (20)(20+6t-t^2). Then dudt=12t\frac{du}{dt} = \frac{1}{2\sqrt{t}} and dvdt=62t\frac{dv}{dt} = 6 - 2t.
  4. Simplify Derivative: Using the quotient rule, dHdt=v(dudt)u(dvdt)v2\frac{dH}{dt} = \frac{v\left(\frac{du}{dt}\right) - u\left(\frac{dv}{dt}\right)}{v^2}.
  5. Set Derivative Equal to Zero: Substitute uu, dudt\frac{du}{dt}, vv, and dvdt\frac{dv}{dt} into the quotient rule formula: dHdt=(20)(20+6tt2)(12t)(t)(62t)(20)(20+6tt2)2\frac{dH}{dt} = \frac{(20)(20+6t-t^2)(\frac{1}{2\sqrt{t}}) - (\sqrt{t})(6 - 2t)}{(20)(20+6t-t^2)^2}.
  6. Clear Denominators: Simplify the derivative: dHdt=400+120t20t240t6t2tt400+120t20t2\frac{dH}{dt} = \frac{400 + 120t - 20t^2}{40\sqrt{t}} - \frac{6\sqrt{t} - 2t\sqrt{t}}{400 + 120t - 20t^2}.
  7. Final Equation: To find the stationary points, set dHdt\frac{dH}{dt} equal to zero: 400+120t20t240t6t2tt400+120t20t2=0\frac{400 + 120t - 20t^2}{40\sqrt{t}} - \frac{6\sqrt{t} - 2t\sqrt{t}}{400 + 120t - 20t^2} = 0.
  8. Final Equation: To find the stationary points, set dHdt\frac{dH}{dt} equal to zero: 400+120t20t240t6t2tt400+120t20t2=0\frac{400 + 120t - 20t^2}{40\sqrt{t}} - \frac{6\sqrt{t} - 2t\sqrt{t}}{400 + 120t - 20t^2} = 0. Multiply both sides by (40t)(400+120t20t2)(40\sqrt{t})(400 + 120t - 20t^2) to clear the denominators.
  9. Final Equation: To find the stationary points, set dHdt\frac{dH}{dt} equal to zero: 400+120t20t240t6t2tt400+120t20t2=0\frac{400 + 120t - 20t^2}{40\sqrt{t}} - \frac{6\sqrt{t} - 2t\sqrt{t}}{400 + 120t - 20t^2} = 0. Multiply both sides by (40t)(400+120t20t2)(40\sqrt{t})(400 + 120t - 20t^2) to clear the denominators. After multiplying, we get: (400+120t20t2)(6t2t2)(40t)=0(400 + 120t - 20t^2) - (6t - 2t^2)(40\sqrt{t}) = 0.

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