Respuesta :
1) Angular velocity: D) 73.3 rev/s
2) Centripetal acceleration: D) [tex]5053 m/s^2[/tex]
3) Net force on the car: E) [tex]2.19\cdot 10^4 N[/tex]
4) Orbital speed: D) [tex](\frac{GM}{r})^{\frac{1}{2}}[/tex]
5) Total mechanical energy: E) [tex]-\frac{GMm}{2r}[/tex]
6) Gravitational force: C) [tex]1.32\cdot 10^{-10}N[/tex]
7) Upward force: C) 188 N
8) Total upward force at B: C) 122 N
Explanation:
1)
The relationship between centripetal acceleration and angular velocity is given by
[tex]a_c = \omega^2 r[/tex]
where:
[tex]a_c[/tex] is the centripetal acceleration
[tex]\omega[/tex] is the angular velocity
r is the radius of the circular path
In this problem,
[tex]a_c = 1950 g = 1950(9.8)=19,110 m/s^2[/tex]
r = 9 cm = 0.09 m
Solving for [tex]\omega[/tex],
[tex]\omega=\sqrt{\frac{a_c}{r}}=\sqrt{\frac{19,110}{0.09}}=460.8 rad/s[/tex]
And keeping in mind that [tex]1 rev = 2 \pi rad[/tex], we can convert into rev/s:
[tex]\omega=460.8 rad/s \cdot \frac{1}{2\pi rad/rev}=73.3 rev/s[/tex]
2)
Again, the centripetal acceleration is given by
[tex]a_c = \omega^2 r[/tex]
where in this problem we have:
[tex]\omega=16 rev/s \cdot 2\pi (rad/rev) = 100.5 rad/s[/tex] is the angular velocity of the piece of dust
r = 0.50 m is the distance of the piece of dust from the axis of rotation
And substituting into the equation, we find the centripetal acceleration of the piece of dust:
[tex]a_c = (100.53)^2(0.5)=5053 m/s^2[/tex]
3)
Since the car is moving in circular motion, the net force is equal to the centripetal force, so it is given by:
[tex]F=m\frac{v^2}{r}[/tex]
where
m = 732 kg is the mass of the car
v = 20.0 m/s is the linear speed of the car
r = 13.0 m is the radius of curvature of the loop-the-loop
Here we have
m = 732 kg
v = 20.0 m/s
r = 13.0 m
Substituting into the equation, we find:
[tex]F=(732)\frac{20.0^2}{13.0}=2.25\cdot 10^4 N[/tex]
The closest option is E) [tex]2.19\cdot 10^4 N[/tex]
4)
The gravitational force between the satellite and the Earth provides the centripetal force that keeps the satellite in circular motion, therefore we can write:
[tex]m\frac{v^2}{r}=G\frac{Mm}{r^2}[/tex]
where the term on the left is the centripetal force while the term on the right is the gravitational force, and where
m is the mass of the satellite
v is its speed
r is the orbital radius
G is the gravitational constant
M is the Earth's mass
Solving for v,
[tex]v=\sqrt{\frac{GM}{r}} = (\frac{GM}{r})^{\frac{1}{2}}[/tex]
5)
The kinetic energy of the satellite is given by
[tex]K=\frac{1}{2}mv^2[/tex]
And substituting its speed, [tex]v=\sqrt{\frac{GM}{r}}[/tex], we get
[tex]K=\frac{GMm}{2r}[/tex]
The potential energy of the satellite is equal to the work that must be done against gravity to bring the satellite from r to infinite, and it is
[tex]U=-\frac{GMm}{r}[/tex]
The total mechanical energy is equal to the sum of kinetic and potential energy:
[tex]E=K+U=\frac{GMm}{2r}+(-\frac{GMm}{r})=-\frac{GMm}{2r}[/tex]
6)
The gravitational force between two objects is given by
[tex]F=G\frac{m_1 m_2}{r^2}[/tex]
where
[tex]G=6.67\cdot 10^{-11} m^3 kg^{-1}s^{-2}[/tex] is the gravitational constant
m1, m2 are the masses of the two objects
r is the separation between them
Here we have:
[tex]m_1 = 12 kg\\m_2 = 14 kg[/tex]
and
r = 9.22 m
Substituting,
[tex]F=(6.67\cdot 10^{-11})\frac{(12)(14)}{(9.22)^2}=1.32\cdot 10^{-10}N[/tex]
7)
To solve the problem, we can apply the equation of the equilibrium of momenta about point B:
[tex]Wx_W - F_A x_A=0[/tex]
where:
W = 300 N is the weight of the plank
[tex]x_W = 5 m[/tex] is the distance of the point of application of the weight from B (half the length of the plank)
[tex]F_A[/tex] is the upward force applied at A
[tex]x_A = 10 - 2 = 8 m[/tex] is the distance of the point of application of [tex]F_A[/tex] from B
Solving for [tex]F_A[/tex],
[tex]F_A = \frac{W x_W}{x_A}=\frac{(300)(5)}{8}=188 N[/tex]
8)
We can solve this part instead by applying the equation of equilibrium of moments around point A:
[tex]-Wx_W - W_B x_B + F_B x_{F_B} = 0[/tex]
where
W = 300 N is the weight of the plank
[tex]x_W = 5 - 2 = 3 m[/tex] is the distance of the point of application of the weight from A
[tex]W_B = 9.0 N[/tex] is the weight of the can of paint at B
[tex]x_B = 10 - 2 = 8 m[/tex] is the distance of the can of paint from A
[tex]F_B[/tex] is the upward force exerted by block B
[tex]x_{F_B}= 10 -2 = 8 m[/tex] is the distance of the point of application of [tex]F_B[/tex] from A
Solving for [tex]F_B[/tex],
[tex]F_B = \frac{W_B x_B + W x_A}{x_{F_B}}=\frac{(9)(8)+(300)(3)}{8}=122 N[/tex]
Learn more about circular motion:
brainly.com/question/2562955
brainly.com/question/6372960
About gravitation:
brainly.com/question/1724648
brainly.com/question/12785992
About moments:
brainly.com/question/5352966
#LearnwithBrainly