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loris [4]
3 years ago
5

Two horizontal curves on a bobsled run are banked at the same angle, but one has twice the radius of the other. The safe speed (

no friction needed to stay on the run) for the smaller radius curve is v. What is the safe speed on the larger radius curve?
A) v/2
B) v /√ 2
C) 2v
D) v√2



I shall answer it here so this can help other students out
First, FN = mg/cos
On a banked curve, FNx is the only acceleration force
FNx = mv^2/r
FNx = FNsin
mg/cos * sin = mv^2/r
cancel out the mass (m) and sin*1/cos is tan
gtan = v^2/r
rgtan = v^2
√(rgtan) = v (this is the velocity for the smaller radius.)
call larger radius velocity X

for larger radius, it becomes 2r, so √(2rgtan) = X

understand you can do √xy = √x * √y

√(rgtan) * √2 = X (√(rgtan) = v)
v * √2 = X (where X is velocity with larger radius)
Physics
1 answer:
konstantin123 [22]3 years ago
4 0

Answer:

Answer:

safe speed for the larger radius track u= √2 v

Explanation:

The sum of the forces on either side is the same, the only difference is the radius of curvature and speed.

Also given that r_1= smaller radius

r_2= larger radius curve

r_2= 2r_1..............i

let u be the speed of larger radius curve

now, \sum F = \frac{mv^2}{r_1} =\frac{mu^2}{r_2}∑F=

r

1

mv

2

=

r

2

mu

2

................ii

form i and ii we can write

v^2= \frac{1}{2} u^2v

2

=

2

1

u

2

⇒u= √2 v

therefore, safe speed for the larger radius track u= √2 v

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Explanation:

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A student pulls on a rope attached to a box of books and moves the box down the hall. The student pulls with a force of 185N at
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Answer:

2.75 m/s^2

Explanation:

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T cos \theta - \mu N = ma (1)

where

T cos \theta is the horizontal component of the tension, where

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\theta=25^{\circ} is the angle between the rope and the horizontal

\mu N is the force of friction, where

\mu=0.27 is the coefficient of friction

N is the normal reaction of the floor on the box

m = 35.0 kg is the mass of the box

a is the acceleration

Along the vertical direction we have:

N+T sin \theta-mg=0 (2)

where

N is the normal force (upward direction)

T sin \theta is the vertical  component of the tension in the rope (upward direction)

mg is the weight of the box (downward direction), where

m = 35.0 kg is the mass of the box

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

From eq.(2) we get:

N=mg-T sin \theta

And substituting into (1), we can find the acceleration:

T cos \theta - \mu (mg-T sin \theta) = ma\\Tcos \theta -\mu mg + \mu T sin \theta = ma\\a=\frac{T cos \theta- \mu mg + \mu T sin \theta}{m}=\\=\frac{(185)(cos 25^{\circ})-(0.27)(35.0)(9.8)+(0.27)(185)(sin 25^{\circ})}{35.0}=2.75 m/s^2

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