r(0) = (a cos 0)i + (a sin 0)j + b0k (a, b > 0) under the influence of gravity, as in the accompanying figure. The O in this equation is the cylindrical coordinate 0 and the helix is the curve r = a, z = b0, 0 z 0, in cylindrical coordinates. We assume 0 to be a differentiable function of t for the motion. The law of conservation of energy tells us that the particle's speed after it has fallen straight down a distance z is V2gz, where g is the constant acceleration of gravity. a. Find the angular velocity de/ dt when 0 = 2. b. Express the particle's 0- and z-coordinates as functions of t. c. Express the tangential and normal components of the velocity dr/ dt and acceleration d'r/dt² as functions of t. Does the acceleration have any nonzero component in the direction of the binormal vector B? The helix r = a, z = b0 Positive z-axis
r(0) = (a cos 0)i + (a sin 0)j + b0k (a, b > 0) under the influence of gravity, as in the accompanying figure. The O in this equation is the cylindrical coordinate 0 and the helix is the curve r = a, z = b0, 0 z 0, in cylindrical coordinates. We assume 0 to be a differentiable function of t for the motion. The law of conservation of energy tells us that the particle's speed after it has fallen straight down a distance z is V2gz, where g is the constant acceleration of gravity. a. Find the angular velocity de/ dt when 0 = 2. b. Express the particle's 0- and z-coordinates as functions of t. c. Express the tangential and normal components of the velocity dr/ dt and acceleration d'r/dt² as functions of t. Does the acceleration have any nonzero component in the direction of the binormal vector B? The helix r = a, z = b0 Positive z-axis
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A frictionless particle P, starting from rest at time t = 0 at the point (a, 0, 0), slides down the helix
![r(0) = (a cos 0)i + (a sin 0)j + b0k (a, b > 0)
under the influence of gravity, as in the accompanying figure. The
O in this equation is the cylindrical coordinate 0 and the helix
is the curve r = a, z = b0, 0 z 0, in cylindrical coordinates. We
assume 0 to be a differentiable function of t for the motion. The
law of conservation of energy tells us that the particle's speed after
it has fallen straight down a distance z is V2gz, where g is the
constant acceleration of gravity.
a. Find the angular velocity de/ dt when 0 = 2.
b. Express the particle's 0- and z-coordinates as functions of t.
c. Express the tangential and normal components of the velocity
dr/ dt and acceleration d'r/dt² as functions of t. Does the
acceleration have any nonzero component in the direction of
the binormal vector B?
The helix
r = a, z = b0
Positive z-axis](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F0dcf9413-c8cb-49e1-a0ab-1657c4692689%2Fd139e8e4-a3b2-4555-92db-f480942e4669%2Fvbslg58.png&w=3840&q=75)
Transcribed Image Text:r(0) = (a cos 0)i + (a sin 0)j + b0k (a, b > 0)
under the influence of gravity, as in the accompanying figure. The
O in this equation is the cylindrical coordinate 0 and the helix
is the curve r = a, z = b0, 0 z 0, in cylindrical coordinates. We
assume 0 to be a differentiable function of t for the motion. The
law of conservation of energy tells us that the particle's speed after
it has fallen straight down a distance z is V2gz, where g is the
constant acceleration of gravity.
a. Find the angular velocity de/ dt when 0 = 2.
b. Express the particle's 0- and z-coordinates as functions of t.
c. Express the tangential and normal components of the velocity
dr/ dt and acceleration d'r/dt² as functions of t. Does the
acceleration have any nonzero component in the direction of
the binormal vector B?
The helix
r = a, z = b0
Positive z-axis
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