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 12.3, Problem 12.106P
To determine

(a)

The distance from the center of Venus to point B

Expert Solution
Check Mark

Answer to Problem 12.106P

The distance from the center of Venus to point B ,

rB=5.35×104mi

Explanation of Solution

Given information:

rA=9.3×103mi

vA=20,000ft/s

rC=5600mi

MVenus=0.82MEarth

Vector Mechanics for Engineers: Dynamics, Chapter 12.3, Problem 12.106P , additional homework tip  1

If the trajectory is an elliptical orbit,

1r0+1r1=2GMh2

Calculation:

g=9.81 m s2

R=6.37×106m 

1 mi=1609.344 m

1ft/s=0.3048 m/s

Consider the first transfer elliptical orbit,

h1=rA.vA

h1=9.3×103mi×1609.344m/mi×20,000fts1×0.3048 ms1/fts1

h1=9.124×1010 m2s1

Consider the first transfer elliptical orbit,

1rA+1rB=2GMVenush12

Since, GMEarth=gREarth2 and MVenus=0.82MEarth ,

1rA+1rB=2G×0.82MEarthh12=2×0.82×gREarth2h12

[19.3×103mi+1rB]×11609.344 m/mi=2×0.82×9.81 m s2×(6.37×106m )2(9.124×1010 ms1)2

rB=5.35×104mi

The distance from the center of Venus to point B ,

rB=5.35×104mi

To determine

(b)

The amounts by which the velocity of the probe should be reduced at B and C respectively.

Expert Solution
Check Mark

Answer to Problem 12.106P

The velocity reduction at point B ,

vB=212ms1

The velocity reduction at point C ,

vC=2082 ms1

Explanation of Solution

Given information:

rA=9.3×103mi

vA=20,000ft/s

MVenus=0.82MEarth

rC=5600mi

Vector Mechanics for Engineers: Dynamics, Chapter 12.3, Problem 12.106P , additional homework tip  2

Angular momentum of a unit mass,

h=r.v

If the trajectory is an elliptical orbit,

1r0+1r1=2GMh2

Initial velocity corresponding to a circular orbit,

vcirc=GMr0

Calculation:

g=9.81 m s2

R=6.37×106m 

1 mi=1609.344 m

From Part (a),

h1=9.124×1010 m2s1

rB=5.35×104mi

Consider the first transfer elliptical orbit,

h1=rB.vB

9.124×1010 m2s1=5.35×104mi×1609.344m/mi×vB

vB=1060 ms1

Then consider the second transfer elliptical orbit,

1rB+1rC=2GMVenush22

Since, GMEarth=gREarth2 and MVenus=0.82MEarth ,

1rB+1rC=2GMVenush22=2G×0.82MEarthh22=2×0.82×gREarth2h22

[15.35×104mi+15600mi+]×11609.344 m/mi=2×0.82×9.81 m s2×(6.37×106m )2h22

h2=7.3×1010m2s1

Applying angular momentum equation for second elliptic orbit,

h2=rB.vB'

7.3×1010m2s1=5.35×104mi×1609.344m/mi×vB'

vB'=848 ms1

Therefore the velocity reduction at point B ,

vB=vBvB'vB=1060848

vB=212ms1

Consider the second transfer elliptical orbit,

h2=rC.vC

7.3×1010m2s1=5600mi×1609.344m/mi×vC

vC=8100 ms1

Then consider the circular orbit at C ,

vC=vcirc=GMVenusrC

Since, GMEarth=gREarth2 and MVenus=0.82MEarth ,

vC,=vcirc=G×0.82MEarthrC=0.82gREarth2rC

vC'=0.82×9.81 m s2×(6.37×106m)2 5600mi×1609.344m/mi

vC'=6018 ms1

Therefore, the velocity reduction at point B ,

vC=vCvC'vC=81006018 ms1vC= 2082 ms1

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Chapter 12 Solutions

Vector Mechanics for Engineers: Dynamics

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