Vector Mechanics For Engineers
Vector Mechanics For Engineers
12th Edition
ISBN: 9781259977305
Author: BEER, Ferdinand P. (ferdinand Pierre), Johnston, E. Russell (elwood Russell), Cornwell, Phillip J., SELF, Brian P.
Publisher: Mcgraw-hill Education,
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Chapter 11.5, Problem 11.164P
To determine

(a)

The magnitude of the velocity of the parasailer as a function of time.

Expert Solution
Check Mark

Answer to Problem 11.164P

Vector Mechanics For Engineers, Chapter 11.5, Problem 11.164P , additional homework tip  1

Explanation of Solution

Given information:

Vector Mechanics For Engineers, Chapter 11.5, Problem 11.164P , additional homework tip  2

Length of rope is defined as,

r=60018t5/2

Constant velocity of the boat is 15kn

The angle is increasing at 2°s

The velocity in radial and transverse components,

v=vrer+vθeθ=r˙er+rθ˙eθ

The acceleration in radial and transverse components,

a=arer+aθeθ=(r¨rθ˙2)er+(rθ¨+2r˙θ˙)eθ

Calculation:

Vector Mechanics For Engineers, Chapter 11.5, Problem 11.164P , additional homework tip  3

According to given information,

Convert,

vB=15kn=25.3ft/saB=0

We know that,

r=60018t5/2

θ˙=2°s=0.0349rad/s

Therefore,

r˙=516t3/2r¨=1532t1/2

θ¨=0

According to the explanation, the relative velocity of parasailer with respect to boat is,

vP/B=r˙er+rθ˙eθ

The relative co-ordinates of the relative velocity is equal to,

vP/B=r˙(cosθi+sinθj)+rθ˙(sinθi+cosθj)

Therefore the velocity of parasailer is equal to,

vP=vB+vP/BvP=vB+r˙(cosθi+sinθj)+rθ˙(sinθi+cosθj)vP=(vBr˙cosθ+rθ˙sinθ)i+(r˙sinθ+rθ˙cosθ)j

We can rewrite this as,

vP=vPxi+vPyj

Where,

vPx=vBr˙cosθ+rθ˙sinθvPy=r˙sinθ+rθ˙cosθ

To find the magnitude,

vP=vPx2+vPy2

Now, plot the graph,

Vector Mechanics For Engineers, Chapter 11.5, Problem 11.164P , additional homework tip  4

Conclusion:

The magnitude of velocity of the parasailer is equal to,

vP=vPx2+vPy2

The relevant graph is shown above.

To determine

(b)

The magnitude of acceleration of parasailer at t=5s

Expert Solution
Check Mark

Answer to Problem 11.164P

aP=1.7871m/s2

Explanation of Solution

Given information:

Vector Mechanics For Engineers, Chapter 11.5, Problem 11.164P , additional homework tip  5

Length of rope is defined as,

r=60018t5/2

Constant velocity of the boat is 15kn

The angle is increasing at 2°s

The velocity in radial and transverse components,

v=vrer+vθeθ=r˙er+rθ˙eθ

The acceleration in radial and transverse components,

a=arer+aθeθ=(r¨rθ˙2)er+(rθ¨+2r˙θ˙)eθ

Calculation:

Vector Mechanics For Engineers, Chapter 11.5, Problem 11.164P , additional homework tip  6

According to given information,

Convert,

vB=15kn=25.3ft/saB=0

We know that,

r=60018t5/2

θ˙=2°s=0.0349rad/s

Therefore,

r˙=516t3/2r¨=1532t1/2

θ¨=0

According to the explanation, the relative acceleration of parasailer with respect to boat is,

aP/B=(r¨rθ˙2)er+(rθ¨+2r˙θ˙)eθaP/B=[1532t1/2(60018t5/2)(0.0349rad/s)2]er+[2(516t3/2)(0.0349rad/s)]eθ

The acceleration of parasailer is equal to,

aP=aB+aP/BaP=0+[(1532t1/2(60018t5/2)(0.0349rad/s)2)er+(2(516t3/2)(0.0349rad/s))eθ]

At, t=5s

aP=[(1532(5)1/2(60018(5)5/2)(0.0349rad/s)2)er+(2(516(5)3/2)(0.0349rad/s))eθ]aP=1.7704er0.2439eθ

Therefore the magnitude is equal to,

aP=(1.7704)2+(0.2439)2aP=1.7871m/s2

Conclusion:

The magnitude of acceleration of the parasailer is equal to,

aP=1.7871m/s2

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Chapter 11 Solutions

Vector Mechanics For Engineers

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