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
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