Row, Row, Row Your Boat

You and n 1 n-1 friends decide to take a trip to an island in a row boat. You'd like to get an idea of how long it will take you to get there.

Assume that you and each of your friends are perfectly identical, some kind of cookie cutter people, who can each provide a given level of power P p P_p to row the boat. We'll suppose that the drag force is proportional to the submerged area of the boat, the square of the velocity, and the density of the water: F d ρ A b o a t v b o a t 2 F_d\sim\rho A_{boat} v_{boat}^2 , i.e. skin drag. Finally, let's assume the boat is made of n n identical sections, of volume V p V_p , that each contribute equally to the surface area, i.e. A b o a t ( n V p ) 2 / 3 A_{boat}\sim \left(nV_p\right)^{2/3} .

Under these assumptions, the steady state velocity of the boat can be written as v b o a t n α P p β V p γ ρ δ v_{boat} \sim n^{\alpha}P_p^{\beta}V_p^{\gamma}\rho^{\delta} . The product of the exponents, α β γ δ \alpha \beta \gamma \delta , can be written as a / b a/b where a a and b b are two coprime integers, what is a + b a+b ?

Hint : Think of how energy is lost by the boat.

This is not an original

Image credit: Wikimedia.


The answer is 731.

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7 solutions

Sanat Anand
Jan 15, 2014

Power delivered by the rowers is lost due to drag force in steady state and there is no net increment in velocity.

Therefore, n × P p = F d × v b o a t n \times P_{p} = F_{d} \times v_{boat}

So, ρ A b o a t v b o a t 3 = n × P p \rho A_{boat} v_{boat}^{3} = n \times P_{p} -Equation 1

Puting A b o a t = ( n V p ) 2 / 3 A_{boat}=(n V_{p})^{2/3} in Equation , we get

ρ ( n V p ) 2 / 3 v b o a t 3 = n × P p \rho (n V_{p})^{2/3} v_{boat}^{3} = n \times P_{p}

On simplifying and taking v b o a t v_{boat} on Left hand side,

v b o a t = ρ 1 / 3 P p 1 / 3 n 1 / 9 V p 2 / 9 v_{boat}=\rho^{-1/3} P_{p}^{1/3} n^{1/9} V_{p}^{-2/9}

Therefore, α = 1 / 9 \alpha=1/9 , β = 1 / 3 \beta=1/3 , γ = 2 / 9 \gamma=-2/9 , δ = 1 / 3 \delta=-1/3

α β γ δ = 2 / 729 \alpha \beta \gamma \delta= 2/729

so, a = 2 a=2 and b = 729 b=729

Therefore, a + b = 731 a+b= \boxed{731}

thanks a lot, cool solution bro!

amgalan amgaa - 7 years, 4 months ago
Anish Puthuraya
Jan 15, 2014

To get a Steady State Velocity, Clearly,

P i n p u t = P d r a g P_{input} = P_{drag}

Thus,

n P p = F d v b o a t nP_p = F_d v_{boat}
n P p = ρ A b o a t V b o a t 3 \Rightarrow nP_p = \rho A_{boat} V_{boat}^3

Simplifying,

v b o a t n 1 / 9 P p 1 / 3 V p 2 / 9 ρ 1 / 3 v_{boat} ~ n^{1/9} P_p^{1/3} V_p^{-2/9} \rho^{-1/3}

Thus,

α β γ δ = 2 729 \alpha\beta\gamma\delta = \frac {2}{729}

Finally,

a + b = 731 a+b = 731

Jatin Yadav
Jan 14, 2014

In steady state, energy lost/second is same as the power supplied,

Clearly, energy lost/sec = work done by drag force/sec = k ρ A b o a t v b o a t 2 × v b o a t k \rho A_{boat} v_{boat}^2 \times v_{boat}

Hence, n × P p = k ρ A b o a t v b o a t 3 n \times P_{p} = k \rho A_{boat} v_{boat}^3 , A b o a t = k ( n V p ) 2 3 A_{boat} = k' (n V_{p})^{\frac{2}{3}}

Hence, ve get v b o a t n 1 / 9 P p 1 / 3 ρ 1 / 3 V p 2 / 9 v_{boat} \propto n^{1/9} P_{p}^{1/3} \rho^{-1/3} V_{p}^{-2/9}

Hence, α β γ δ = 2 729 \alpha \beta \gamma \delta = \frac{2}{729}

Iit Jee Aspirants
May 24, 2014

sum of power of persons=power of drag force

Siddharth Shah
Jan 29, 2014

using the simple fact that Power = Force . Velocity,

we get n × P p n \times P_{p} = F p × v p F_{p} \times v_{p} plugging in the values using any constants can get the answer as we only need the proportionality relation 731 \boxed{731}

Iam Mangod96
Jan 21, 2014

This question is actually a simple dimensions problem. We start with what we are given as : The drag force, F d F_{d} = ρ \rho v b o a t 2 v^{2}_{boat} n 2 3 n^{\frac {2}{3}} V p 2 3 V^{\frac {2}{3}}_{p} Now we know that P o w e r = F o r c e × v e l o c i t y Power = Force \times velocity And we are also given that each man exerts a power of P p P_{p} . So, total power exerted by all men = n × P p = n \times P_{p} . Therefore substituting in our original equation : n P p = F d × v b o a t nP_{p} = F_{d} \times v_{boat} n P p = ρ \Rightarrow nP_{p} = \rho v b o a t 2 v^{2}_{boat} n 2 3 n^{\frac {2}{3}} V p 2 3 V^{\frac {2}{3}}_{p} v b o a t = n 1 9 P p 1 3 V p 2 9 ρ 1 3 \Rightarrow v_{boat} = n^{\frac {1}{9}}P^{\frac {1}{3}}_{p}V^{\frac {-2}{9}}_{p}\rho^{\frac {-1}{3}} Now I am sure you can do the rest and enjoy the mathematics. Thank you.

Tan Kiat
Jan 18, 2014

Note that for a power P P , it is defined as the work done per unit time. Thus, P = W o r k D o n e t P = \frac{Work Done}{t} . As work done is defined as the product of force and distance, we have P = ( F ) ( x ) t = ( F ) ( v ) P = \frac{(F)(x)}{t} = (F)(v) , where v v represents the speed.

As each person provides a power P, the net power provided is defined as n P p nP_p . At the steady state velocity, v v is constant, implying that F n e t = 0 N F_{net} = 0 N . Hence, as the applied force = drag force. , at a constant speed, the power applied = power loss due to drag force. Thus n P p = P d = ( F d ) ( v ) nP_p = P_d = (F_d)(v) .

Hence, n P p = ( F d ) ( v ) nP_p = (F_d)(v)

= p A v 3 pAv^3 , by substituting the expression for F d F_d .

Thus, n P p = p n 2 3 V p 2 3 v 3 nP_p = pn^{\frac{2}{3}}V_p^{\frac{2}{3}}v^3 , by substituting the expression for A b o a t A_{boat}

Hence, v = n 1 9 P p 1 3 V p 2 9 p 1 3 v = n^{\frac{1}{9}}P_p^{\frac{1}{3}}V_p^{-\frac{2}{9}}p^{-\frac{1}{3}}

Thus, the product of the exponents is given by 1 9 \frac{1}{9} x 1 3 \frac{1}{3} x ( 2 9 ) (-\frac{2}{9}) x ( 1 3 ) (-\frac{1}{3}) = 2 729 \frac{2}{729}

Hence, 2 + 729 = 731 2 + 729 = \boxed{731}

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