You are riding in a school bus. as the bus rounds a flat curve at constant speed, a lunch box with a mass of 0.470 kg suspended from the ceiling of the bus by a string of length 1.75 m is found to hang at rest relative to the bus when the string makes an angle of 30.0 ∘ with the vertical. in this position the lunch box is a distance 49.0 m from the center of curvature of the curve.

Respuesta :

Missing question: " What is the speed v of the bus?"

Solution:
Let's solve the problem by writing the equilibrium conditions on both x- and y- axis:
[tex]mg=T cos \alpha[/tex]
[tex]m \frac{v^2}{r}=T sin \alpha [/tex]
where [tex]mg[/tex] is the weight of the lunch box, [tex]m \frac{v^2}{r} [/tex] is the centripetal force, T is the tension of the string and [tex]\alpha=30^{\circ}[/tex].

The radius r is the one with respect to the vertical position of the string, therefore
[tex]r=L sin30^{\circ}=0.875 m[/tex].

From the first equation we find
[tex]T= \frac{mg}{cos \alpha} [/tex]
and if we replace this into the second one, we find
[tex]m \frac{v^2}{r}=mg \tan \alpha [/tex]
from which we can find the velocity:
[tex]v= \sqrt{rg \tan \aplha}= \sqrt{(0.875m)(9.81m/s^2)(\tan 35^{\circ})}=2.45 m/s [/tex]

Here as we know that

m = mass of the box = 0.470 kg

L = Length of the string = 1.75 m

r = radius of the path = 49 m

[tex]\theta [/tex] = angle of the thread

Now from the condition of equilibrium of lunch box with respect to bus we can say

[tex]Tsin30 = \frac{mv^2}{r}[/tex]

[tex]Tcos30 = mg[/tex]

now divide the above two equations

[tex]tan30 = \frac{v^2}{rg}[/tex]

solving the above equation for velocity

[tex]v^2 = rg tan30[/tex]

[tex]v = \sqrt{rgtan30}[/tex]

[tex]v = \sqrt{49\times 9.8\times tan30}[/tex]

[tex]v = 16.65 m/s[/tex]

ACCESS MORE