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e-lub [12.9K]
3 years ago
11

In the International System of Units, the basic unit for measuring mass is what

Physics
1 answer:
nadezda [96]3 years ago
3 0

Answer:

Kilograms (kg)

Explanation:

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(i) a force of 35.0 n is required to start a 6.0-kg box moving across a horizontal concrete floor, (a) what is the coefficient o
Serjik [45]

a. The force applied would be equal to the frictional force.

F = us Fn

where, F = applied force = 35 N, us = coeff of static friction, Fn = normal force = weight

 

35 N = us * (6 kg * 9.81 m/s^2)

us = 0.595

 

b. The force applied would now be the sum of the frictional force and force due to acceleration

F = uk Fn + m a

where, uk = coeff of kinetic friction

 

35 N = uk * (6 kg * 9.81 m/s^2) + (6kg * 0.60 m/s^2)

uk = 0.533

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A heavy flywheel is accelerated (rotationally) by a motor that provides constant torque and therefore a constant angular acceler
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Answer:

a)t_1=\frac{w_1-w_o}{\alpha}=\frac{w_1}{\alpha}sec

b)\theta_1=\frac{w_1^2}{2\alpha}rad

c)t_2=\frac{\alpha t_1}{5\alpha}=\frac{t_1}{5}sec

Explanation:

1) Basic concepts

Angular displacement is defined as the angle changed by an object. The units are rad/s.

Angular velocity is defined as the rate of change of angular displacement respect to the change of time, given by this formula:

w=\frac{\Delat \theta}{\Delta t}

Angular acceleration is the rate of change of the angular velocity respect to the time

\alpha=\frac{dw}{dt}

2) Part a

We can define some notation

w_o=0\frac{rad}{s},represent the initial angular velocity of the wheel

w_1=?\frac{rad}{s}, represent the final angular velocity of the wheel

\alpha, represent the angular acceleration of the flywheel

t_1 time taken in order to reach the final angular velocity

So we can apply this formula from kinematics:

w_1=w_o +\alpha t_1

And solving for t1 we got:

t_1=\frac{w_1-w_o}{\alpha}=\frac{w_1}{\alpha}sec

3) Part b

We can use other formula from kinematics in order to find the angular displacement, on this case the following:

\Delta \theta=wt+\frac{1}{2}\alpha t^2

Replacing the values for our case we got:

\Delta \theta=w_o t+\frac{1}{2}\alpha t_1^2

And we can replace t_1from the result for part a, like this:

\theta_1-\theta_o=w_o t+\frac{1}{2}\alpha (\frac{w_1}{\alpha})^2

Since \theta_o=0 and w_o=0 then we have:

\theta_1=\frac{1}{2}\alpha \frac{w_1^2}{\alpha^2}

And simplifying:

\theta_1=\frac{w_1^2}{2\alpha}rad

4) Part c

For this case we can assume that the angular acceleration in order to stop applied on the wheel is \alpha_1 =-5\alpha \frac{rad}{s}

We have an initial angular velocity w_1, and since at the end stops we have that w_2 =0

Assuming that t_2 represent the time in order to stop the wheel, we cna use the following formula

w_2 =w_1 +\alpha_1 t_2

Since w_2=0 if we solve for t_2 we got

t_2=\frac{0-w_1}{\alpha_1}=\frac{-w_1}{-5\alpha}

And from part a) we can see that w_1=\alpha t_1, and replacing into the last equation we got:

t_2=\frac{\alpha t_1}{5\alpha}=\frac{t_1}{5}sec

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Answer:

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Explanation:

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