Triple Integral of y^2z^2 over a Paraboloid: Polar Coordinates Method

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SUMMARY

The discussion focuses on evaluating the triple integral of y²z² over a region bounded by the paraboloid x = 1 - y² - z² and the plane x = 0. Participants clarify the conversion to polar coordinates, emphasizing the use of non-standard polar coordinates where y = r cos(θ) and z = r sin(θ). The volume element is defined as dV = r dr dθ dx. Key challenges include correctly applying these transformations and integrating within the specified limits.

PREREQUISITES
  • Understanding of triple integrals and volume elements in calculus
  • Familiarity with polar coordinate transformations
  • Knowledge of paraboloid equations and their geometric implications
  • Basic skills in multivariable calculus
NEXT STEPS
  • Study the conversion of Cartesian coordinates to polar coordinates in three dimensions
  • Learn about the geometric interpretation of paraboloids and their applications in integrals
  • Practice evaluating triple integrals using non-standard coordinate systems
  • Explore volume elements in different coordinate systems, focusing on cylindrical and spherical coordinates
USEFUL FOR

Students and educators in calculus, particularly those focusing on multivariable calculus and integral evaluation techniques. This discussion is beneficial for anyone seeking to deepen their understanding of coordinate transformations in triple integrals.

stolencookie

Homework Statement


Evaluate the triple integral y^2z^2dv. Where E is bounded by the paraboloid x=1-y^2-z^2 and the place x=0.

Homework Equations


x=r^2cos(theta) y=r^2sin(theta)

The Attempt at a Solution


I understand how to find these three limits, -1 to 1 , -sqrt(1-y^2) to sqrt(1-y^2) , 0 to 1-y^2-z^2. I then solved the first integral and got y^2z(1-y^2-z^2) I know I need to convert to polar coordinates. I am able to do that 0 to 2pi, 0 to 1.
I am having trouble converting the equation y^2z(1-y^2-z^2) to polar coordinates.
 
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stolencookie said:

Homework Statement


Evaluate the triple integral y^2z^2dv. Where E is bounded by the paraboloid x=1-y^2-z^2 and the place x=0.

Homework Equations


x=r^2cos(theta) y=r^2sin(theta)
What are these equations? They aren't the equations to convert from cartesian to polar.
stolencookie said:

The Attempt at a Solution


I understand how to find these three limits, -1 to 1 , -sqrt(1-y^2) to sqrt(1-y^2) , 0 to 1-y^2-z^2. I then solved the first integral and got y^2z(1-y^2-z^2) I know I need to convert to polar coordinates. I am able to do that 0 to 2pi, 0 to 1.
I am having trouble converting the equation y^2z(1-y^2-z^2) to polar coordinates.
 
yes they are I am having trouble converting it do I leave the z that left over in?
 
stolencookie said:

Homework Statement


Evaluate the triple integral y^2z^2dv. Where E is bounded by the paraboloid x=1-y^2-z^2 and the place x=0.

Homework Equations


x=r^2cos(theta) y=r^2sin(theta)

The Attempt at a Solution


I understand how to find these three limits, -1 to 1 , -sqrt(1-y^2) to sqrt(1-y^2) , 0 to 1-y^2-z^2. I then solved the first integral and got y^2z(1-y^2-z^2) I know I need to convert to polar coordinates. I am able to do that 0 to 2pi, 0 to 1.
I am having trouble converting the equation y^2z(1-y^2-z^2) to polar coordinates.[/B]

It looks like the x-axis in your problem plays the role usually reserved for the z-axis in similar problems. So, you will find it easier to use un-standard polar coordinates ##y = r \cos \theta## and ##z = r \sin \theta##, with volume element ##dV = r\, dr \,d\theta \, dx##.
 
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Thank you :).
 
Mark44 said:
They aren't the equations to convert from cartesian to polar.

stolencookie said:
yes they are
No, they aren't. In the usual conversions, ##x = r\cos(\theta)## and ##y = r\sin(\theta)##, not with ##r^2## as you show. Use Ray's advice to treat x as you would normally do for z
 
Mark44 said:
No, they aren't. In the usual conversions, ##x = r\cos(\theta)## and ##y = r\sin(\theta)##, not with ##r^2## as you show. Use Ray's advice to treat x as you would normally do for z
that was a mistype .
 

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