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lawyer [7]
3 years ago
9

A student slides a book across a desk, with a velocity of +8 m/s. When her friend catches the book, it has a velocity of +7.4 m/

s. If the acceleration was a constant -5.6 m/s2, how wide is the desk?
A. 0.05 m
B. 0.60 m
C. 0.83 m
D. 1.65 m
Physics
1 answer:
marin [14]3 years ago
5 0

Because acceleration was constant throughout the slide, we can show the slide lasted

a=\dfrac{\Delta v}{\Delta t}\iff-5.6\,\dfrac{\mathrm m}{\mathrm s^2}=\dfrac{7.4\,\frac{\mathrm m}{\mathrm s}-8\,\frac{\mathrm m}{\mathrm s}}{\Delta t}

\implies\Delta t=0.107\,\mathrm s

Also because accleration was constant, we know the average velocity of the book was

\bar v=\dfrac{7.4\,\frac{\mathrm m}{\mathrm s}+8\,\frac{\mathrm m}{\mathrm s}}2=7.7\,\dfrac{\mathrm m}{\mathrm s}

Average velocity is also given by

\bar v=\dfrac{\Delta x}{\Delta t}\iff7.7\,\dfrac{\mathrm m}{\mathrm s}=\dfrac{\Delta x}{0.107\,\mathrm s}

so the width of the desk must have been

\Delta x=0.824\,\mathrm m

which means C is the most likely answer.

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Answer:

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Explanation:

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Weight force mg pulling straight down.

Normal force N pushing perpendicular to the slope.

Friction force F pushing parallel up the slope.

Sum of forces in the parallel direction:

∑F = ma

mg sin θ − F = ma

Sum of torques about the cylinder's axis:

∑τ = Iα

Fr = ½ mr²α

F = ½ mrα

Since the cylinder rolls without slipping, a = αr.  Substituting:

F = ½ ma

Two equations, two unknowns (a and F).  Substituting the second equation into the first:

mg sin θ − ½ ma = ma

Multiply both sides by 2/m:

2g sin θ − a = 2a

Solve for a:

2g sin θ = 3a

a = ⅔ g sin θ

a = ⅔ (9.8 m/s²) (sin 30°)

a = 3.27 m/s²

Solving for F:

F = ½ ma

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3 years ago
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nexus9112 [7]

(a) The man comes to a halt in 1.99 ms = 1.99 × 10⁻³ s, so his average acceleration slowing him from 6.33 m/s to a rest is

<em>a</em> = (6.33 m/s - 0) / (1.99 × 10⁻³ s) ≈ 3180 m/s²

so that the average net force on the man during the landing is

<em>F</em> = (70.8 kg) <em>a</em> ≈ 225,000 N

i.e. with magnitude 225,000 N.

(b) With knees bent, the man has an average acceleration of

<em>a</em> = (6.33 m/s - 0) / (0.147 s) ≈ 43.1 m/s²

and hence an average net force of

<em>F</em> = (70.8 kg) <em>a</em> ≈ 3050 N

(c) The net force on the man is

∑ <em>F</em> = <em>n</em> - <em>w</em> = <em>m a</em>

where

<em>n</em> = magnitude of the normal force, i.e. the force of the ground pushing up on the man

<em>w</em> = the man's weight, <em>m g</em> ≈ 694 N

<em>m</em> = the man's mass, 70.8 kg

<em>g</em> = mag. of the acceleration due to gravity, 9.80 m/s²

<em>a</em> = the man's acceleration

Using the acceleration in part (b), we have

<em>n</em> = <em>m g</em> + <em>m a</em> = <em>m</em> (<em>g</em> + <em>a</em>)

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Missing figure: find it in attachment.

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It follows immediately that in the figure, the force of gravity is the only force acting downward: therefore, force D.

The other forces are called:

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