Fluid Mechanics, 8 Ed
Fluid Mechanics, 8 Ed
8th Edition
ISBN: 9789385965494
Author: Frank White
Publisher: MCGRAW-HILL HIGHER EDUCATION
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Chapter 7, Problem 7.59P
To determine

(a)

An equation for the speed which Joe can pedal into the wind.

Expert Solution
Check Mark

Answer to Problem 7.59P

V3+2VwV2+(Vw2+2C rrmgCDAρ)V(2C rrmgCDAρVb+Vb3)=0

Explanation of Solution

Given information:

Joe pedals his bike at 10m/s without the effect of wind

The rolling resistance is equal to 0.8N.s/m

The drag area is 0.422m2

Weight of Joe is 80kg

Weight of bike is 15kg

The speed of headwind is 5m/s

The rolling force FR is defined as,

FR=Crrmg

Where,

Crr - rolling resistance co-efficient

m - Total mass acting normal to the plane

The air drag is defined as,

Fdrag=CDρ2V2A

Where,

CD - Drag co-efficient

ρ - Density of the fluid

V - Velocity

A - Characteristic area

The power is defined as,

P=FV

Calculation:

Evaluate the total force,

F=FR+Fdrag

For drag force the relative velocity is equal to,

Vrelative=V+Vwind

Substitute for forces,

F=Crrmg+CDAρ2(V+V wind)2

Calculate the power,

P=FV

Substitute for total force,

P=FV={Crrmg+CDAρ2(V+ V wind)2}V

Evaluate the power required without head wind,

P=FV={Crrmg+CDAρ2Vbike2}Vbike

But, we can say the power output will be same at both occasions,

Therefore,

{Crrmg+CDAρ2Vbike2}Vbike={Crrmg+CDAρ2(V+ V wind)2}V

Solve further,

V3+2VwV2+(Vw2+2C rrmgCDAρ)V(2C rrmgCDAρVb+Vb3)=0

Conclusion:

The equation for the speed at which Joe has to ride into the wind can be given as,

V3+2VwV2+(Vw2+2C rrmgCDAρ)V(2C rrmgCDAρVb+Vb3)=0.

To determine

(b)

Speed V.

Expert Solution
Check Mark

Answer to Problem 7.59P

V=9.64m/s

Explanation of Solution

Given information:

Joe pedals his bike at 10m/s without the effect of wind

The rolling resistance is equal to 0.8N.s/m

The drag area is 0.422m2

Weight of Joe is 80kg

Weight of bike is 15kg

The speed of headwind is 5m/s

According to sub-part A,

We have found a cubic equation for speed V

V3+2VwV2+(Vw2+2C rrmgCDAρ)V(2C rrmgCDAρVb+Vb3)=0

In above equation,

Vw - Speed of wind

Vb - Speed of bike

Assume, the air at 20°C will have,

ρ=1.2kg/m3

Calculation:

The cubic equation for speed V is given as,

V3+2VwV2+(Vw2+2C rrmgCDAρ)V(2C rrmgCDAρVb+Vb3)=0

Substitute given values,

V3+2(5m/s)V2+( ( 5m/s )2+ 2( 0.8N.s/m )( 95kg )( 9.81m/ s 2 ) ( 0.422 m 2 )( 1.2kg/ m 3 ))V( 2( 0.8N.s/m )( 95kg )( 9.81m/ s 2 ) ( 0.422 m 2 )( 1.2kg/ m 3 )( 10m/s)+ ( 10m/s )3)=0

Solve further,

V3+10V2+2970V30445.5V=0

Therefore,

V=9.64m/s

Conclusion:

Joe should ride at 9.64m/s into the headwind.

To determine

(c)

The reason the result is not simplified 105=5m/s, as one might first suspect.

Expert Solution
Check Mark

Answer to Problem 7.59P

Since, FdragV2

We cannot able to estimate that,

V=VbikeVwind=10m/s5m/s

Explanation of Solution

Given information:

Joe pedals his bike at 10m/s without the effect of wind

The rolling resistance is equal to 0.8N.s/m

The drag area is 0.422m2

Weight of Joe is 80kg

Weight of bike is 15kg

The speed of headwind is 5m/s

The drag force is defined as,

Fdrag=CDρ2V2A

Therefore, we can say that,

FdragV2

Hence, we cannot say that,

V=VbikeVwind

The rolling resistance will also have an effect on the velocity.

Conclusion:

Since, FdragV2

We cannot able to estimate that,

V=VbikeVwind=10m/s5m/s.

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Chapter 7 Solutions

Fluid Mechanics, 8 Ed

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