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Burka
2 days ago
7

Look at the diagram of the moon and three different paths that it could take. A planet with a moon in orbit. The moon has arrows

labeled 1 through 3. 1: Curves up and away from the planet. 2: Moves straight forward. 3: Curves down to follow planet's orbit. Which description applies best to pathway 2? the path of the moon toward the Sun the path of the moon’s orbit around Earth the path the moon would take if it had a larger mass than the Sun the path the moon would take if there was no force of Earth’s gravity
Physics
2 answers:
kicyunya [3.1K]2 days ago
7 0

Answer:

D on edg 2020

Explanation:

Yuliya22 [3.2K]2 days ago
6 0
is 3 and 2

Explanation: the first is 3 while the second is 2.

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You are at a train station, standing next to the train at the front of the first car. The train starts moving with constant acce
serg [3485]
The duration required for the seventh car to pass amounts to 13.2 seconds. The train's movement is characterized by uniform acceleration, enabling the application of suvat equations. Initially, we analyze the movement of the first car, utilizing the equation for distance s covered in time t, which corresponds to the length of one car, with u = 0 as the initial velocity and a representing acceleration, over t = 5.0 s. We can rearrange the equation reflecting L as the length of one car. This is similarly applicable for the initial seven cars, accounting for the distance of 7L and the required time t'. With constant acceleration retained, we can derive t' through substitution in the equation, leading to fundamental conclusions regarding the relationship exhibited in the graph of distance against time in uniformly accelerated motion.
8 0
23 days ago
Platinum (pt) has the fcc crystal structure, an atomic radius of 0.1387 nm, and an atomic weight of 195.08 g/mol. what is its th
inna [2995]
The formula to apply is expressed as:

ρ = nA/VcNₐ
where
ρ signifies density
n represents the number of atoms within a unit cell (for FCC, n=4)
A indicates the atomic weight
Vc stands for the cubic cell volume equal to a³, with a being the side length (for FCC, a = 4r/√2, where r is the radius)\
Nₐ denotes Avogadro's number, which is 6.022×10²³ atoms/mol

Calculating the radius: r = 0.1387 nm*(10⁻⁹ m/nm)*(100 cm/1m) = 1.387×10⁻⁸ cm
Then find a: a = 4(1.387×10⁻⁸ cm)/√2 = 3.923×10⁻⁸ cm
Then calculate V: V = a³ = (3.923×10⁻⁸ cm)³ = 6.0376×10⁻²³ cm³

Now compute density:
ρ = [(4 atoms)(195.08 g/mol)]/[(6.0376×10⁻²³ cm³)(6.022×10²³ atoms/mol)]Finally, we get ρ = 21.46 g/cm³
7 0
5 days ago
Read 2 more answers
On average, both arms and hands together account for 13% of a person's mass, while the head is 7.0% and the trunk and legs accou
Softa [2965]

Answer:

176.38 rpm

Explanation:

The proportion of mass for arms and legs is 13%.

For legs and trunk, it's 80% of the total mass.

Additionally, the head accounts for 7% of the total mass.

Overall, the mass of the skater is 74.0 kg.

Each arm length is 70 cm, or 0.7 m.

The skater's height is 1.8 m, and the trunk diameter measures 35 cm, or 0.35 m.

Starting angular momentum is 68 rpm.

We make the following assumptions:

  1. The skater is modeled as a vertical cylinder (head, trunk, and legs), with arms extending horizontally as two uniform rods.
  2. Friction between the skater and the ice is considered negligible.

To analyze her body, we divide it into two parts, treating the arms as spinning rods.

1. Each arm (rod) has a moment of inertia of \frac{1}{3} mL^{2}.

The arms comprise 13% of 74 kg, calculated as 0.13 x 74 = 9.62 kg.

Each arm is then evaluated as 9.62/2 = 4.81 kg.

Let L represent the length of each arm.

Thus,

I = \frac{1}{3} x 4.81 x 0.7^{2} = 0.79 kg-m for each arm.

2. The body, treated as a cylinder, has a moment of inertia of \frac{1}{2} mr^{2}.

For the body, the radius r is half of the trunk diameter: r = 0.35/2 = 0.175 m.

The mass of the trunk amounts to (80% + 7%) of 74 kg, which calculates to 0.87 x 74 = 64.38 kg.

Therefore, I = \frac{1}{2} x 64.38 x 0.175^{2} = 0.99 kg-m.

Two cases are considered:

case 1: Body spinning with arms extended.

Total moment of inertia equals the combined moments of inertia of both arms and the trunk.

I = (0.79 x 2) + 0.99 = 2.57 kg-m.

The angular momentum is given by Iω.

Here, ω = angular speed = 68.0 rpm = \frac{2\pi }{60} x 68 = 7.12 rad/s.

The angular momentum then becomes 2.57 x 7.12 = 18.29 kg-rad/m-s.

case 2: Arms drawn in alongside the trunk.

The moment of inertia is attributed solely to the trunk. This is 0.91 kg-m.

The angular momentum equals Iω.

= 0.99 x ω = 0.91ω.

By the principle of conservation of angular momentum, the two angular momentum quantities are equal. Therefore,

18.29 = 0.99ω.

Solving gives ω = 18.29/0.99 = 18.47 rad/s.

This leads to 18.47 ÷ \frac{2\pi }{60} = 176.38 rpm.

7 0
1 month ago
A mercury atom in the ground state absorbs 20.00 electronvolts of energy and is ionized by losing an electron. How much kinetic
Softa [2965]
We have a mercury atom in its ground state that absorbs 20 eV of energy, resulting in ionization by the loss of an electron. We need to compute the kinetic energy of the ejected electron. The initial energy here is 20 eV, which converts to 20 J/C. The charge of the electron is 1.60217662 × 10^{-19} coulombs. To find the kinetic energy, we can utilize the equation: KE = 20 Joules / Coulombs * 1.60217662 × 10^{-19} coulombs, yielding KE = 1.25x10^{20} Joules. Thus, after ionization, the electron possesses a kinetic energy of 1.25x10^{20} Joules or 1.25x10^{17} kJ.
8 0
5 days ago
. A magnetic field has a magnitude of 0.078 T and is uniform over a circular surface whose radius is 0.10 m. The field is orient
Keith_Richards [3153]

Response:

The magnetic flux across the surface amounts to 2.22 \times 10^{-3} Wb

Clarification:

Provided:

Strength of magnetic field B = 0.078 T

Circle's radius r = 0.10 m

Angle of incidence between the field and the surface normal \theta = 25°

Utilizing the flux formula,

\phi = B.A

\phi = BA\cos \theta

Where \theta = the angle represents the orientation of the magnetic field line relative to the surface normal, A = and the area pertains to the circular surface.

A = \pi r^{2}

A = 3.14 \times (0.10) ^{2}

A = 0.0314 m^{2}

The calculation for magnetic flux is expressed as

\phi = 0.078 \times 0.0314 \times \cos 25

\phi = 2.22 \times 10^{-3} Wb

Thus, the magnetic flux through the surface calculates to 2.22 \times 10^{-3} Wb

6 0
12 days ago
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