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Elodia [21]
3 years ago
10

The bearing of a lighthouse from a ship was found to be N 37 degrees E. After the ship sailed 2.5 miles due south, the new beari

ng was N 25 degrees East. Find the distance between the ship and the lighthouse at each location.

Physics
1 answer:
ella [17]3 years ago
5 0

Answer:

The distance between the lighthouse and the ship

from the start position A = 5.08 miles

from the Final point B = 7.23 miles

Explanation:

Note: Refer the figure

Let the position of the lighthouse be 'L'  

Given:

When the ship is at the position A, ∠DAL=37°

Now, when the ship sails through a distance of 2.5 i.e at position B

mathematically,

AB=2.5 miles

∠ABL=25°

Now,

∠DAL + ∠LAB = 180°

or

37° +  ∠LAB = 180°

or

∠LAB = 180° - 37° = 143°

Also, In ΔLAB

∠LAB + ∠ABL + ∠ALB = 180°

or

143° + 25° + ∠ALB = 180°

or

∠ALB = 180° - 143° - 25° = 12°

Now using the concept of the sin law

In ΔLAB

\frac{AL}{sin25^o}=\frac{2.5}{sin12^o}

or

AL = 5.08 miles

and,

\frac{BL}{sin143^o}=\frac{2.5}{sin12^o}

or

BL = 7.23 miles

hence,

The distance between the lighthouse and the ship

from the start position A = 5.08 miles

from the Final point B = 7.23 miles

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A jet engine pushes air at high velocity toward the rear of the plane. Thrust is created moving the plane forward. Which stateme
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3 years ago
If two light waves are coherent a) their amplitudes are the same their phase difference is constant their frequencies are the sa
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Answer:

a) their amplitudes are the same their phase difference is constant their frequencies are the same

Explanation:

Coherent waves are the waves that have constant phase difference, equal frequency, amplitude and waveform.

Frequency denotes the number of cycles a wave completes in one second.

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3 years ago
A worker pushes a 50 kg crate a distance of 7.5 m across a level floor. He
Taya2010 [7]

a) 73.5 N

b) 551.3 J

c) -551.3 J

d) 0 J

e) 0 J

f) 0 J

g) 0 J

Explanation:

a)

There are two forces acting on the crate:

- The push of the worker, F, in the forward direction

- The frictional force, F_f=\mu mg, in the backward direction, where  

\mu=0.15 is the coefficient of friction

m = 50 kg is the mass of the crate

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

According to Newton's second law of motion, the net force on the crate must be equal to the product of mass and acceleration, so:

F-F_f=ma

However, the crate here is moving with constant velocity, so its acceleration is zero:

a=0

So the previous equation becomes:

F-F_f=0

And we can find the magnitude of the applied force:

F=F_f=\mu mg=(0.15)(50)(9.8)=73.5 N

b)

The work done by the applied force on the crate is

W_F=Fd cos \theta

where:

F is the magnitude of the force

d is the displacement of the crate

\theta is the angle between the direction of the force and of the displacement

Here we have:

F = 73.5 N

d = 7.5 m

\theta=0^{\circ} (the force is applied in the same direction as the displacement)

Therefore,

W_F=(73.5)(7.5)(cos 0^{\circ})=551.3 J

c)

The work done by friction on the  crate is:

W_{F_f}=F_f d cos \theta

where in this case:

F_f=73.5 N is the magnitude of the force of friction

d = 7.5 m is the displacement of the crate

\theta=180^{\circ}, because the displacement is forward and the  force of friction is backward, so they are in opposite direction

Therefore, the work done by the force of friction is:

W_{F_f}=(73.5)(7.5)(cos 180^{\circ})=-551.3 J

d)

To find the normal force, we analyze the situation of the force along the vertical direction.

We have two forces on the vertical direction:

- The normal force, N, upward

- The force of gravity, mg, downward, where

m = 50 kg is the mass of the crate

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

Since the crate is in equilibrium in this direction, the vertical acceleration is zero, so the two forces balance each other:

N-mg=0\\N=mg=(50)(9.8)=490 N

The work done by the normal force is:

W_N=Nd cos \theta

In this case, \theta=90^{\circ}, since the normal force is perpendicular to the displacement of the crate; therefore, the work done is

W_N=(490)(7.5)(cos 90^{\circ})=0

e)

The work done by the gravitational force is:

W_g=F_g d cos \theta

where:

F_g=mg=(50)(9.8)=490 N is the gravitational force

d = 7.5 m is the displacement of the crate

\theta=90^{\circ} is the angle between the direction of the gravitational force (downward) and the displacement (forward)

Therefore, the work done by gravity is

W_g=(490)(7.5)(cos 90^{\circ})=0 J

f)

The total work done on the crate can be calculated by adding the work done by each force:

W=W_F+W_{F_f}+W_N+W_g

where we have:

W_F=+551.3 J is the work done by the applied force

W_{F_f}=-551.3 J is the work done by the frictional force

W_N=0 is the work done by the normal force

W_g=0 is the work done by the force of gravity

Substituting,

W=+551.3+(-551.3)+0+0=0 J

So, the total work is 0 J.

g)

According to the work-energy theorem, the change in kinetic energy of the crate is equal to the work done on it, therefore:

W=\Delta E_K

where

W is the work done on the crate

\Delta E_K is the change in kinetic energy of the crate

In this problem, we have:

W=0 (total work done on the crate is zero)

Therefore, the change in kinetic energy of the crate is:

\Delta E_K = W = 0

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