A coin just remains on a disc rotating at a steady rate of 180r.p.m .A coin is kept at a distance of 2 cm from the axis of rotationn . The coefficient of fricition between the coin and the disc is _____ `[ gg= 9.8 m//s^(2)]`
A coin just remains on a disc rotating at a steady rate of 180r.p.m .A coin is kept at a distance of 2 cm from the axis of rotationn . The coefficient of fricition between the coin and the disc is _____ `[ gg= 9.8 m//s^(2)]`
A
`0.524`
B
`0.624`
C
`0.724`
D
`0.824`
Text Solution
AI Generated Solution
The correct Answer is:
To find the coefficient of friction between the coin and the disc, we can follow these steps:
### Step 1: Convert RPM to RPS
Given that the disc rotates at 180 revolutions per minute (RPM), we need to convert this to revolutions per second (RPS).
\[
\text{RPS} = \frac{180 \text{ RPM}}{60} = 3 \text{ RPS}
\]
### Step 2: Calculate Angular Velocity (ω)
The angular velocity (ω) in radians per second can be calculated using the formula:
\[
\omega = 2\pi \times \text{RPS}
\]
Substituting the value of RPS:
\[
\omega = 2\pi \times 3 = 6\pi \text{ rad/s}
\]
### Step 3: Identify the Radius
The distance of the coin from the axis of rotation is given as 2 cm. We need to convert this to meters:
\[
r = 2 \text{ cm} = 0.02 \text{ m}
\]
### Step 4: Apply the Centripetal Force Equation
The centripetal force required to keep the coin in circular motion is given by:
\[
F_c = \frac{mv^2}{r}
\]
Where \( v \) can be expressed in terms of angular velocity (ω):
\[
v = r\omega
\]
Substituting this into the centripetal force equation:
\[
F_c = \frac{m(r\omega)^2}{r} = m r \omega^2
\]
### Step 5: Relate Centripetal Force to Frictional Force
The frictional force (F_f) that provides the necessary centripetal force is given by:
\[
F_f = \mu mg
\]
Where \( \mu \) is the coefficient of friction and \( mg \) is the weight of the coin.
### Step 6: Set the Forces Equal
For the coin to remain on the disc without slipping, the frictional force must equal the centripetal force:
\[
\mu mg = m r \omega^2
\]
### Step 7: Cancel Mass (m)
Since mass (m) appears on both sides of the equation, we can cancel it out:
\[
\mu g = r \omega^2
\]
### Step 8: Solve for the Coefficient of Friction (μ)
Rearranging the equation to solve for μ gives:
\[
\mu = \frac{r \omega^2}{g}
\]
### Step 9: Substitute Known Values
Now we can substitute the values we have:
- \( r = 0.02 \) m
- \( \omega = 6\pi \) rad/s
- \( g = 9.8 \) m/s²
Calculating \( \omega^2 \):
\[
\omega^2 = (6\pi)^2 = 36\pi^2
\]
Now substituting into the equation for μ:
\[
\mu = \frac{0.02 \times 36\pi^2}{9.8}
\]
### Step 10: Calculate the Value
Calculating the value:
\[
\mu = \frac{0.02 \times 36 \times 9.87}{9.8} \approx 0.725
\]
### Conclusion
The coefficient of friction between the coin and the disc is approximately **0.725**.
---
To find the coefficient of friction between the coin and the disc, we can follow these steps:
### Step 1: Convert RPM to RPS
Given that the disc rotates at 180 revolutions per minute (RPM), we need to convert this to revolutions per second (RPS).
\[
\text{RPS} = \frac{180 \text{ RPM}}{60} = 3 \text{ RPS}
\]
...
Topper's Solved these Questions
Similar Questions
Explore conceptually related problems
A disc rotates about its aixs of symmetry in a horizontal plane at a steady rate of 3.5 revolutions per second A coin placed at a distance fo 1.25 cm form the axis of ratation remains at rest on the disc The coefficient of friction between the coin and the disc is : (g=10//s^(2))
A coin of 4 g mass is placed at a distance of 2 cm from the axis of rotation a disc,. If the frequancy of disc is 180 rpm, then the coefficient of friction between the coin at rest and disc will be
A gramophone disc is set revolving in a horizontal plane at the rate of 33(1)/(2) revolutions per minute. It is found that a small coin placed on the disc will remain there if its centre is not more than 5 cm from the axis of rotation. Calculate the coefficient of friction between the coin and the disc [Hint : Centripetal force = m omega^(2)r= Frictional force = mu N=mu mg ]
A disc rotates at 60 rev//min around a vertical axis.A body lies on the disc at the distance of 20cm from the axis of rotation.What should be the minimum value of coefficient of friction between the body and the disc,so that the body will not slide off the disc
A coin placed on a horizontal rotating disc, with its centre at 10 cm from the centre of the disc, is about to slip off when the disc performs 60 rpm. Find the coefficient of friction between the coin and the disc.
A coin kept at a distance of 5 cm from the centre of a turntable of radius 1.5 m just begins to slip when the turntable rotates at a speed of 90 r.p.m. Calculate the coefficient of static friction between the coin and the turntable [g = 9.8 m//s^(2)]
A coins kept on a horizontal rotating disc has its centre at a distance of 0.25 m from the axis of rotation of the disc .If mu is 0.2 , then the angular velocity of the disc at which the coion will slip off, (g=9.8m//s^(2))
A disc starts rotating with a constant angular acceleration of 1 rad//s^(2) about a fixed vertical axis perpendicular to its plane and passing through its centre. A coin of mass 10 gm is placed on the disc at a distance of 10cm from the axis. The coefficent of friction between the disc and the coin is 0.2 . The value of the frictional force on the coin at t=1s will be
A gramphone record is revolving with an angular velocity omega . A coin is placed at a distance R from the centre of the record. The static coefficient of friction is mu . The coin will revolve with the record if
A small coin of mass 40 g is placed on the horizontal surface of a rotating disc. The disc starts from rest and is given a constant angular acceleration alpha="2 rad s"^(-2) . The coefficient of static friction between the coin and the disc is mu_(s)=3//4 and the coefficient of kinetic friction is mu_(k)=0.5. The coin is placed at a distance r=1m from the centre of the disc. The magnitude of hte resultant force on the coin exerted by the disc just before it starts slipping on the disc is :