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svetoff [14.1K]
3 years ago
5

The crate, which sets on a 10 degree incline, has a weight of 3433.5 N and is subjected to a towing force P acting at a 20 degre

e angle with the horizontal. If the coefficient of static friction is µs = 0.5, determine the force P needed to just start the crate moving down the plane.

Physics
1 answer:
sp2606 [1]3 years ago
6 0

Answer:

P = 981 N

Explanation:

Given

Angle of the incline θ = 10°

Angle of the towing force φ =20°

Weight of the crate W = 3433.5 N

The coefficient of static friction µ = 0.5

Solution

Forces Acting along the ramp

\mu N = Pcos(10^{o}+10^{o})+Wsin10^{0} \\\mu N = Pcos30^{o}+Wsin10^{0}

Forces acting perpendicular to the ramp

N + Psin30^{o}=Wcos10^{0}\\\\N=Wcos10^{0}-Psin30^{o}\\

Substituting the value of N we get

\mu[Wcos10^{0}-Psin30^{o}] =Pcos30^{o}+Wsin10^{0}\\\\\mu Wcos10^{0}- \mu Psin30^{o} =Pcos30^{o}+Wsin10^{0}\\\\\mu Wcos10^{0}- Wsin10^{0}=Pcos30^{o}+\mu Psin30^{o} \\\\P=W\frac{\mu cos10^{0}- sin10^{0}}{cos30^{o}+\mu sin30^{o}} \\\\P=3433.5\frac{0.5 \times cos10^{0}- sin10^{0}}{cos30^{o}+0.5 \times  sin30^{o}}\\\\P=980.66\\\\ P = 981 N

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The gravitational potential energy of a body is the energy possessed by the object due to its position in a gravitational field, and it is given by:

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The total mechanical energy of Mr.Leppold is the sum of the potential and the kinetic energy:

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During the fall, the height of Leppold decreases: this means that as h decreases, the potential energy decreases  too.

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A particle with a mass of 0.500 kg is attached to a horizontal spring with a force constant of 50.0 N/m. At the moment t = 0, th
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a) x(t)=2.0 sin (10 t) [m]

The equation which gives the position of a simple harmonic oscillator is:

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where

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t is the time

Let's start by calculating the angular frequency:

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The amplitude, A, can be found from the maximum velocity of the spring:

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b)  t=0.10 s, t=0.52 s

The potential energy is given by:

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While the kinetic energy is given by:

K=\frac{1}{2}mv^2

The velocity as a function of time t is:

v(t)=v_{max} cos(\omega t)

The problem asks as the time t at which U=3K, so we have:

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However, \frac{m}{k}=\frac{1}{\omega^2}, so we have

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\omega t= \frac{5\pi}{3}\\t=\frac{5\pi}{3\omega}=\frac{5\pi}{3(10 rad/s)}=0.52 s

c) 3 seconds.

When x=0, the equation of motion is:

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so, t=0.

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So, the time needed is 3 seconds.

d) 0.097 m

The period of the oscillator in this problem is:

T=\frac{2\pi}{\omega}=\frac{2\pi}{10 rad/s}=0.628 s

The period of a pendulum is:

T=2 \pi \sqrt{\frac{L}{g}}

where L is the length of the pendulum. By using T=0.628 s, we find

L=\frac{T^2g}{(2\pi)^2}=\frac{(0.628 s)^2(9.8 m/s^2)}{(2\pi)^2}=0.097 m






5 0
3 years ago
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