Circular/rotational motion problem - Waterwheel with bucket

  • Thread starter Oshada
  • Start date
  • Tags
    Motion
In summary, a water-wheel with a single bucket fixed in a specific orientation and filled with water has a mass of 100 kg, radius of 10m, and a bucket with a capacity of 20 litres of water. The initial angular acceleration after release was found to be 0.39 rad/s^2. The torque experienced by the wheel was determined to be 1960cosθ over the range of θ from 0 to π/2, assuming no water is lost from the bucket. The final angular velocity of the wheel at θ = π/2 was calculated to be 0.87 rad/s using integration methods. The wheel has four identical buckets attached to the rim with equal spacing, and if attached to
  • #1
Oshada
41
0

Homework Statement



A water-wheel equipped with a single bucket is fixed in the orientation shown in the diagram below, while the bucket is filled with water. When the bucket is full, the wheel is released so that it can rotate freely. The wheel has a uniform density and a mass of 100 kg, radius 10m and the bucket has a capacity of 20 litres of water (with mass 20 kg). The mass of the bucket is negligible compared to the mass of the water.

2moqpg1.jpg


(a) Determine the initial angular acceleration of the water wheel immediately after it is
released (i.e. when θ = 0).

(b) Determine the torque experienced by the wheel as a function of 9 over the range from
θ = 0 to θ = π/2 assuming no water is lost from the bucket.

(c) Determine the final angular velocity of the wheel assuming the water runs out of the
wheel at θ = π/2.

(d) Assume the wheel has four identical buckets to the one in the diagram, attached to the
rim with equal spacing. The buckets are all filled and emptied on the same basis as
described above. If the wheel is attached to an electric generator that exerts a torque of
1000 Nm on the wheel, and the wheel then rotates at an average angular speed of
0.5 rad/s, determine the average power being generated by the wheel.


Homework Equations



All the usually relevant circular motion equations involving θ, I, ⍺, τ and ω


The Attempt at a Solution



For part a), I found τ from τ = r x F and found ⍺ from τ = I⍺. Since v = 0 at the start I ignored centripetal force. I got ⍺ = 0.40 rad/s^2, but the answer given is 0.39 rad/s^2. Due to this I haven't really worked out the rest of the sections. Also, I'm lacking a plan of attack for section c). In section d), since our course did not include P = τ.ω I think I might have to derive it.

Any help is most appreciated!
 
Physics news on Phys.org
  • #2
a)Let the moment of inertia of the wheel = mwr2/2

The moment of inertia of the bucket = mbr2

The torque acting on the system = 20gr=2000

Using the equation,
Torque = moment of inertia X angular acceleration
200r = (20r+100/2r2 ) X angular acceleration
angular acceleration = 0.38rads-2
 
  • #3
Thanks a lot! However, the answer was 0.39 rad/s^2, which makes me think that the moment of inertia of the bucket might be something different?
 
  • #4
But I think that the bucket and the water inside can be consider as point mass, the little difference can be ignored, right?
 
Last edited:
  • #5
In section c), you have to use the result from b) and using integration by in ⍺dt = ω+ω0
 
  • #6
Thanks a lot! If you can show me how to get torque in terms of angular displacement it'd be very helpful :D
 
  • #7
b) τ = R X F R is the perpendicular distance between the force vector and the centre of rotation
τ = mgrcosθ
=2000cosθ

where 0<= θ<= π/2
 
Last edited:
  • #8
OH right, I didn't think about the r changing D: Thanks a lot! (The answer is 1960cosθ but that's just g = 9.8 m/s^2). As for section c), how can I use the factor that all the water has run out at the bottom (θ = π/2)?
 
  • #9
In c) the assumption of all water run out at bottom means that there is no water run between θ=0 and θ=pi/2
Do you want me to show you how to calculate c)?
 
  • #10
The answer to c) is 0.87 rad/s. I think the water runs out gradually, from 0 to π/2.
 
  • #11
That may not be the case, the water should run out when θ=pi/2, I tried to calculate(base on my assumption), I get the right answer
 
  • #12
Which formulas did you use? If you could show your working that'd be great!
 
  • #13
I have used integration for c)

⍺=τ/I = 1960cosθ / (20r+100/2r2 ) = (49/130)cosθ

ω= ∫ ⍺ dt
= ∫ (49/130)cosθ dt
= 49/130 ∫ cosθ dt
Because ω=dθ/dt

ω= 49/130 ∫ (cosθ)/ω dθ

derivative both side,

dω/dθ = 49/130 (cosθ)/ω
ωdω = 49/130 cosθdθ

integrate both side

∫ ωdω = 49/130 ∫ cosθdθ
(1/2)ω2 = (49/130)sinθ
ω = √(49/65)sinθ
when θ=π/2,
ω = √(49/65)sin(π/2) = 0.87rads-1
 
  • #14
Oh wow, that's tricky... is that the only way to do it? But thank you very much!
 

FAQ: Circular/rotational motion problem - Waterwheel with bucket

What is circular/rotational motion and how does it apply to a waterwheel with a bucket?

Circular/rotational motion is the movement of an object around a circular path. In the case of a waterwheel with a bucket, the waterwheel rotates around its central axis, causing the bucket to move in a circular motion as well.

How does the waterwheel with a bucket work?

The waterwheel with a bucket works by harnessing the energy of falling water to rotate the wheel. As the wheel turns, the buckets attached to it collect water from a lower source and then release it onto a higher source. This creates a continuous cycle of rotation, which can be used to power machinery or generate electricity.

What factors affect the rotational speed of the waterwheel with a bucket?

The rotational speed of the waterwheel with a bucket can be affected by several factors, such as the force of gravity pulling the water down, the weight and size of the wheel, the angle at which the buckets are positioned, and the amount of water flowing onto the wheel.

How does the waterwheel with a bucket use the concept of torque?

The waterwheel with a bucket uses the concept of torque to rotate the wheel. Torque is a force that causes an object to rotate around a fixed point, and in this case, the force of the falling water creates a torque that turns the wheel.

What are some real-world applications of waterwheels with buckets?

Waterwheels with buckets have been used for centuries to power various types of machinery, such as grain mills, sawmills, and textile mills. In modern times, they are also used in hydroelectric power plants to generate electricity from falling water. Additionally, waterwheels with buckets are often used in irrigation systems to transport water from lower sources to higher fields.

Similar threads

Back
Top