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kogti [31]
3 years ago
13

If we decrease the distance an object moves we will

Physics
2 answers:
emmasim [6.3K]3 years ago
6 0
... without changing the speed of the object, then
we will not have to wait so long for the object to get
where it is going.
aleksley [76]3 years ago
4 0
If we decrease the distance an object moves, we will decrease the amount of work done.
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You have been hired to help improve the material movement system at a manufacturing plant. Boxes containing 16 kg of tomato sauc
pickupchik [31]

a) 15.4^{\circ}

b) 5.2 m/s

c) 151.2 N

Explanation:

a)

When the box is on the frictionless ramp, there is only one force acting in the direction along the ramp: the component of the forc of gravity parallel to the ramp, which is given by

mg sin \theta

where

m =16 kg is the mass of the box

g=9.8 m/s^2 is the acceleration due to gravity

\theta is the angle of the ramp

According to Newton's second law of motion, the net force on the box is equal to the product of mass and acceleration, so:

F=ma\\mgsin \theta = ma

where a is the acceleration.

From the equation above we get

a=g sin \theta

And we are told that the acceleration must not exceed

a=2.6 m/s^2

Substituting this value and solving for \theta, we find the maximum angle of the ramp:

\theta=sin^{-1}(\frac{a}{g})=sin^{-1}(\frac{2.6}{9.8})=15.4^{\circ}

b)

Here we are told that the vertical distance of the ramp is

h=1.4 m

Since there are no frictional forces acting on the box, the total mechanical energy of the box is conserved: this means that the initial gravitational potential energy of the box at the top must be equal to the kinetic energy of the box at the bottom of the ramp.

So we have:

GPE=KE\\mgh=\frac{1}{2}mv^2

where:

m = 16 kg is the mass of the box

g=9.8 m/s^2

h = 1.4 m height of the ramp

v = final speed of the box at the bottom of the ramp

Solving for v,

v=\sqrt{2gh}=\sqrt{2(9.8)(1.4)}=5.2 m/s

c)

There are two forces acting on the box in the direction perpendicular to the ramp:

- The normal force, N, upward

- The component of the weight perpendicular to the ramp, downward, of magnitude

mg cos \theta

Since the box is in equilibrium along the perpendicular direction, the net force is zero, so we can write:

N-mg cos \theta

and by substituting:

m = 16 kg

g=9.8 m/s^2

\theta=15.4^{\circ}

We can find the normal force:

N=mg cos \theta=(16)(9.8)cos(15.4^{\circ})=151.2 N

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Because it records speed of the car at a certain time, the independent variable should be time and dependent would be speed or velocity. Since it's taken every second, it would be considered instantaneous velocity, which is D.
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Mass divided by volume
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