Rotor rooter and Solution to 181. What goes up does not necessarily stay up, as this problem by John Olson of Shelton, Conn., demonstrates.
Problem 182 — What goes up doesn’t necessarily stay up, as this month’s problem by John Olson of Shelton, Conn., demonstrates.
“Our usual bet?” quipped Phineas Gotrocks.
One of the semi-annual model plane races of the Squaunder Club was just getting underway, and Gotrock’s bet with fellow member Lottie Dough as to who would win the race was a club legend.
“I’ve made some modifications this time,” continued Gotrocks. “I’ll be entering a radio-controlled model helicopter, instead.”
“Why, you ...” muttered Lottie. “Never mind! I’ll still beat you, especially at that stretch where the models fly up the 720- ft-high cliff.”
Gotrocks panicked. “I hadn’t thought of that! It’ll never make the climb.”
Lottie chuckled, “That’ll be cash, Gotrocks. No checks!”
The helicopter Gotrocks had made to specification features a 40-ft-diam main rotor and an 8-ft-diam tail rotor. The rotors are geared together, and the clearance between their blade-tip paths is 6 in. Tail rotor thrust moment-arm is 24.5 ft perpendicular to the main rotor shaft. At 100% rpm, the tip speed of both rotors is 700 fps. The engine produces 1,200 hp, 90% of which goes to the main rotor by means of a multiple-reduction belt drive with a reduction ratio of 12.5:1. Engine power does not change with rpm.
The race began. When the models reached the cliff, the helicopter was 20 ft off the ground, and its engine rpm was down to 90% and continuing to drop at a rate of 8% per min. The chopper’s rate of climb is a constant 500 fpm. Tail rotor’s maximum available thrust decreases proportionally to the square of the quotient of beginning and ending rpm percentage. At the start of the climb, tail rotor’s maximum available thrust is down to 1,150 lb.
Ignore wind and other aerodynamic forces on the helicopter’s fuselage. Also, neglect drive train losses. Will the helicopter be able to climb the cliff? Compute both the necessary and available tail rotor thrusts during the climb to see if Gotrocks needs to stop at the bank before the awards ceremony.
Technical consultant, Jack Couillard, Menasha, Wis.
Solution to last month’s problem 181 — You are a champion clock watcher, if you answered 1:05:27. Here’s how Baath and McBean ended up doing time. Let:
Vm = Speed of minute hand, is 1/60 rpm
Vh = Speed of hour hand, is 1/720 rpm
t = Time from 1:00 p.m. until hands line up, min
Dm Distance traveled by minute hand during time t, rev
Dh Distance traveled by hour hand during time t, rev
Since time is distance divided by speed:
We also know that the hour hand moves 1/12 rev or “5 min” for every revolution of the minute hand, or:
Insert the value for Dm into (1) to get:
Cross multiply and solve for Dh:
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Use the value of Dh to solve for t:
Baath and McBean get caught by the 1:05:30 downloading and thus their own futures are in jeopardy!
Contest winner — There were a variety of correct answers, and we included anyone who came up with a logical combination of coins in the drawing. Congratulations to R. Roberts of Emporia, Ky., who won our February contest by having his name drawn from the 147 contestants who answered out of a total of 189 for that month. A TI-68 calculator is in the mail to him.
The TI-68 Advanced Scientific Calculator by Texas Instruments can solve five simultaneous equations with real and complex coefficients and has 40 number functions that can be used in both the rectangular and polar coordinate systems. Other functions include formula programming, integration, and polynomial root finding. The calculator also features a last-equation replay function that lets you double-check your work.