The local bases in cylindrical coordinates (r ,

\theta

, z) are given by $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ = cos(

\theta

) i + sin(

\theta

) j, $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ = - sin(

\theta

) i + cos(

\theta

) j, and $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ = k.Express the velocity v of a moving particle in space in terms of the local bases above.
A) $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$
B) $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ + $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$
C) $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ + $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$
D) $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ + r $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ + $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$
E) $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ + r $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ + $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$ $The local bases in cylindrical coordinates (r , \theta , z) are given by = cos( \theta ) i + sin( \theta ) j, = - sin( \theta ) i + cos( \theta ) j, and = k.Express the velocity v of a moving particle in space in terms of the local bases above. A) B) + C) + D) + r + E) + r +$

Evaluate the Integral of Over the Portion

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