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erma4kov [3.2K]
3 years ago
8

A boat crosses a 200 m wide river at 3 ms-1, north relative to water. The river flows at 1 ms-1 as shown.

Physics
1 answer:
Vika [28.1K]3 years ago
8 0

Answer:

3.16 m·s⁻¹ at an angle of 71.6°  

Explanation:

Assume that the diagram is like Fig. 1 below.

The boat is heading straight across the river and the current is directed straight downstream.

We have two vectors at right angles to each other.

1. Calculate the magnitude of the resultant

We can use the Pythagorean theorem (Fig. 2).

R² = (3 m·s⁻¹)² + (1 m·s⁻¹)² = 9 m²·s⁻² + 1 m²·s⁻² = 10 m²·s⁻²

R = √(10 m²·s⁻²) ≈ 3.16 m·s⁻¹

2. Calculate the direction of the resultant

The direction of the resultant is the counterclockwise angle (θ) that it makes with due East .

tanθ = opposite/adjacent = 3/1 = 3

θ = arctan 3 = 71.6°

To an observer at point O, the velocity of the boat is 3.16 m·s⁻¹ at an angle of 71.6°.

 

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Drops of rain fall perpendicular to the roof of a parked car during a rainstorm. The drops strike the roof with a speed of 15 m/
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Answer: (a) 1.065 N  (b) 2.13 N

Explanation:

<h2>(a) average force exerted by the rain on the roof</h2><h2 />

According Newton's 2nd Law of Motion the force F is defined as <u>the variation of linear momentum</u> p <u>in time:</u>

F=\frac{dp}{dt}  (1)

Where the linear momentum is:

p=mV  (2) Being m the mass and V the velocity.

In the case of the rain drops, which initial velocity is V_{i}=15m/s and final velocity is  V_{f}=0 (we are told the drops come to rest after striking the roof). The momentum of the drops p_{drops} is:

p_{drops}=mV_{i}+mV_{f}  (3)

If V_{f}=0, then:

p_{drops}=mV_{i}  (4)

Now the force F_{drops} exerted by the drops is:

F_{drops}=\frac{dp_{drops}}{dt}=\frac{d}{dt}mV_{i}  (5)

F_{drops}=\frac{dm}{dt}V_{i}+m\frac{dV_{i}}{dt}  (6)

At this point we know the mass of rain per second (mass rate) \frac{dm}{dt}=0.071 kg/s and we also know the initial velocity does not change with time, because that is the velocity at that exact moment (instantaneous velocity). Therefore is a constant, and the derivation of a constant is zero.

This means (6) must be rewritten as:

F_{drops}=\frac{dm}{dt}V_{i}  (7)

F_{drops}=(0.071 kg/s)(15m/s)  (8)

F_{drops}=1.065kg.m/s^{2}=1.065N  (9) This is the force exerted by the rain drops on the roof of the car.

<h2>(b) average force exerted by hailstones on the roof </h2><h2 />

Now let's assume that instead of rain drops, hailstones fall on the roof of the car, and let's also assume these hailstones bounce back up off after striking the roof (this means they do not come to rest as the rain drops).

In addition, we know the hailstones fall with the same velocity as the rain drops and have the same mass rate.

So, in this case the linear momentum p_{hailstones} is:

p_{hailstones}=mV_{i}+mV_{f}   (9)  Being V_{i}=V_{f}

p_{hailstones}=mV+mV=2mV   (10)  

Deriving with respect to time to find the force F_{hailstones} exerted by the hailstones:

F_{hailstones}=\frac{d}{dt}p_{hailstones}=\frac{d}{dt}(2mV)   (10)  

F_{hailstones}=2\frac{d}{dt}(mV)=2(\frac{dm}{dt}V+m\frac{dV}{dt})   (11)  

Assuming \frac{dV}{dt}=0:

F_{hailstones}=2(\frac{dm}{dt}V)   (12)  

F_{hailstones}=2(0.071 kg/s)(15m/s)   (13)  

Finally:

F_{hailstones}=2.13kg.m/s^{2}=2.13N (14)   This is the force exerted by the hailstones  

Comparing (9) and (14) we can conclude the force exerted by the hailstones is two times greater than the force exerted by the raindrops.

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