Straight Wire Slide

A massive bead is positioned on a smooth straight wire whose ( x , y , z ) (x,y,z) end point coordinates are:

P 1 = ( 1 , 2 , 3 ) P 2 = ( 15 , 5 , 7 ) \vec{P_1} = (1,2,3) \\ \vec{P_2} = (-15,5,7)

There is an ambient gravity of 10 m/s 2 10 \, \text{m/s}^2 in the z -z direction. At time t = 0 t = 0 , the bead starts at rest at P 2 \vec{P_2} and slides toward P 1 \vec{P_1} .

At what time does the bead reach P 1 \vec{P_1} ?

Note: All quantities are in SI units


The answer is 3.7483.

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1 solution

An energy analysis is easiest. The increase in kinetic energy is equal to the decrease in potential energy: 1 2 m v f 2 = m g Δ z \tfrac12 mv_f^2 = -mg\Delta z . Thus v f = 2 g Δ z . v_f = \sqrt{-2g\Delta z}. Since the acceleration is constant, the average velocity is the mean of initial and final velocity, i.e. v = 1 2 v f \langle v \rangle = \tfrac12v_f . Thus v = 1 2 g Δ z . \langle v \rangle = \sqrt{-\tfrac12g\Delta z}.

The distance traveled by the bead is s = ( Δ x ) 2 + ( Δ y ) 2 + ( Δ z ) 2 ; s = \sqrt{(\Delta x)^2 + (\Delta y)^2 + (\Delta z)^2}; finally, the time it takes to travel this distance is Δ t = s v = ( Δ x ) 2 + ( Δ y ) 2 + ( Δ z ) 2 1 2 g Δ z . \Delta t = \frac{s}{\langle v \rangle} = \sqrt{\frac{(\Delta x)^2 + (\Delta y)^2 + (\Delta z)^2}{-\tfrac12g\Delta z}}. Substituting Δ x = 16 \Delta x = 16 , Δ y = 3 \Delta y = -3 , Δ z = 4 \Delta z = -4 , and g = 10 g = 10 , we obtain Δ t = 1 6 2 + ( 3 ) 2 + ( 4 ) 2 5 ( 4 ) = 281 20 = 14.05 = 3.7483 s . \Delta t = \sqrt{\frac{16^2 + (-3)^2 + (-4)^2}{-5\cdot(-4)}} = \sqrt{\frac{281}{20}} = \sqrt{14.05} = \boxed{3.7483}\ \mathrm{s}.

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