Vector Mechanics for Engineers: Dynamics
Vector Mechanics for Engineers: Dynamics
11th Edition
ISBN: 9780077687342
Author: Ferdinand P. Beer, E. Russell Johnston Jr., Phillip J. Cornwell, Brian Self
Publisher: McGraw-Hill Education
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Chapter 11.5, Problem 11.181P
To determine

(a)

The direction of the binomial pathat t=0.

Expert Solution
Check Mark

Answer to Problem 11.181P

θx=90°,θy=123.7°,θz=33.7°

Explanation of Solution

Given information:

According to problem 11.96,

r=(Atcost)i+(A t2+1)j+(Btsint)k

A=3,B=1

The first derivative of motion is equal to velocity

v=dxdt

The first derivative of velocity is equal to acceleration

a=dvdt

Calculation:

According to the given information,

r=(Atcost)i+(A t2+1)j+(Btsint)k

Substitute,

r=(3tcost)i+(3t2+1)j+(tsint)k

Differentiate to find the velocity,

v=drdt=3(costtsint)i+3(12(t2+1)12(2t))j+(sint+tcost)k

v=drdt=3(costtsint)i+3tt2+1j+(sint+tcost)k

Differentiate to find the acceleration,

a=dvdt=3(sintsinttcost)i+3t2+13t(12(t2+1)12(2t))t2+1j+(cost+costtsint)k

a=dvdt=3(sintsinttcost)i+3[t2+1t(tt2+1)t2+1]j+(cost+costtsint)k

We know that,

eb=v×a|v×a|

At t=0

v=(3ft/s)ia=(3ft/s)j+(2ft/s)k

Then,

v×a=3i[3j+2k]v×a=3(2j+3k)

Find,

|v×a|=3(2)2+(3)2=313

Therefore,

eb=v×a|v×a|=3(2j+3k)313=113(2j+3k)

According to the above result,

cosθx=0cosθy=213cosθz=313

Therefore,

θx=90°,θy=123.7°,θz=33.7°

Conclusion:

The direction of binomial path at t=0 ,

θx=90°,θy=123.7°,θz=33.7°

To determine

(b)

The direction of the binomial path at t=π2.

Expert Solution
Check Mark

Answer to Problem 11.181P

θx=103.4°,θy=134.4°,θz=47.4°

Explanation of Solution

Given information:

According to problem 11.96,

r=(Atcost)i+(A t2+1)j+(Btsint)k

A=3,B=1

The first derivative of motion is equal to velocity

v=dxdt

The first derivative of velocity is equal to acceleration

a=dvdt

Calculation:

According to the given information,

r=(Atcost)i+(A t2+1)j+(Btsint)k

Substitute,

r=(3tcost)i+(3t2+1)j+(tsint)k

Differentiate to find the velocity,

v=drdt=3(costtsint)i+3(12(t2+1)12(2t))j+(sint+tcost)k

v=drdt=3(costtsint)i+3tt2+1j+(sint+tcost)k

Differentiate to find acceleration,

a=dvdt=3(sintsinttcost)i+3t2+13t(12(t2+1)12(2t))t2+1j+(cost+costtsint)k

a=dvdt=3(sintsinttcost)i+3t2+1t(tt2+1)t2+1j+(cost+costtsint)k

We know that,

eb=v×a|v×a|

At t=π2

v=(3π2ft/s)i+(3ππ2+4ft/s)j+(1ft/s)ka=dvdt=(6ft/s2)i+(24(π2+4)3/2ft/s2)j(π2ft/s2)k

Therefore,

v×a=[3π22π2+4+24(π2+4)3/2]i[6+3π44]j+[36π(π2+4)3/2+18π(π2+4)1/2]k=4.4398i13.4022j+12.9946k

Then,

|v×a|=[(4.4398)2+(13.4022)2+(12.9946)2]1/2=19.1883

Now substitute to find,

eb=v×a|v×a|

eb=v×a|v×a|=4.4398i13.4022j+12.9946k19.1883

Then,

cosθx=4.439819.1883cosθy=13.402219.1883cosθz=12.994619.1883

Finally we get,

θx=103.4°,θy=134.4°,θz=47.4°

Conclusion:

The direction of binomial path at t=π2

θx=103.4°,θy=134.4°,θz=47.4°

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Chapter 11 Solutions

Vector Mechanics for Engineers: Dynamics

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