6.2 - Circular Motion Flashcards

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1
Q

What units can we measure angles in

A

Angles can be measured in radians as well as in degrees

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2
Q

When may we use radians

A

When we are measuring rotation, we often use the radian to measure angles

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3
Q

How can we calculate the distance/circumference/ arc length an object has travelled on a circular path

A

The distance the object travels around the circumference (in metres) would be equal to the angle swept out in radians.

angle (in radians ) = arc length/radius of arc

So, theta = s/r

So, for a complete circle, in which the circumference is equal to 2pi x r, the angle swept out will be equal to

= 2 x pi x r/ r = 2 pi radians

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4
Q

What is angular displacement

A

Angular displacement is the vector measurement of the angle through which something has moved. The standard convention is that anti-clockwise rotation is a positive number and clockwise rotation is a negative number.

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5
Q

How do we convert from radians to degrees

A

Radians to degrees = multiply by 180/pi

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6
Q

How do we convert from degrees to radians

A

Multiply by pi/180

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7
Q

How does the British army use a system for angle measurements

A

The British army uses a system for angle measurement in which a complete circle is divided into 6400 ‘mils’. This is an abbreviation for milliradian. The idea is that at a distance/radius of 1km, an angle of 1 mil would represent a distance of 1 metre.

So when aiming artillery fire, a horizontal adjustment of 1 mil in angle of fire should move to a target 1 metre sideways for every kilometre distance away.

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8
Q

What is angular velocity

A

An object moving in a circle sweeps out a certain angle in a certain time, depending upon how fast it is moving. The rate at which angular displacement changes is called the angular velocity, (omega, w)

So w = theta / t

It’s measured in rads^-1

If an object completes a full circle (2pi radians) in a time period, T (it’s capital T now because it’s the time period for a full circle) then the angular velocity can be rearranged and given by

T = 2pi/w

Since in an earlier chapter we found f = 1/T

Therefore, w = 2pi x f
^the frequency of rotation is the reciprocal of the time period.

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9
Q

What is the instantaneous velocity

A

Also known as the actual velocity, we know that v = s/t and since theta = s/r (arc length/radius)

So s = r x theta

Thus, v = r x theta / t

And so, v = r x w

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10
Q

Tell me about centripetal acceleration/ velocity

A

Velocity is a vector, and so it is correctly described by quoting both its magnitude and direction. An acceleration can change either of these, or both. An object moving in a ⭕️ circle may travel at a constant speed (and a constant angular velocity) but the direction it is moving in must constantly change. This means it is constantly accelerating. As this acceleration represents represents the changes in direction around the circle, it is called the centripetal acceleration, a.

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11
Q

How can we derive the formula for centripetal acceleration - you need to be able to do this

A

Check the image on page 24 for it to make sense

In order to determine how to calculate the centripetal acceleration, we must consider how quickly the direction, and therefore, velocity is changing.

At the arbitrary positions of the rotating object, A, and at s time t, later B, we consider the components of the objects velocity, in the x and y directions.

Point C is equal to the midpoint of AB, so as A and B are equal distances above and below point C, the vertical velocity component, v(subscript y), is the same at A and at B v(subscript y) = v x cos theta

So, the vertical acceleration is zero, a(subscript y) = 0

Horizontally, the magnitude of the velocity is equal at both parts but in opposite directions,

At A: v(subscript x) = v x sin theta
At B: v(subscript x) = -v x sin theta

So the acceleration in the horizontal direction, calculated as change in velocity over time

a(subscript x) = 2vsin theta / t

Since v = r theta / t, this can be rearranged to give t = r x theta / v

Here the angle moved in time t, is labelled as 2 theta,

So t = r x 2theta /v

Therefore,

a(subscript x) = v2vsin theta/ r2 theta = v^2 x sin theta / r theta

This must be true for all values of theta, and as we want to find the instantaneous acceleration at any point on the circumference, we must consider the general answer as we reduce theta to zero. In the limit as theta tends to zero,
Sin theta /theta = 1, so sin theta =0

Therefore, we can simplify the equation before to make a = v^2/r

From thus definition v = rw

a is also equal to a = r x w^2

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12
Q

Why is the centripetal acceleration always directed towards the centre of the circle

A

The centripetal acceleration in this case is just the horizontal acceleration, as we considered the object in a position along a horizontal radius. Following a similar derivation at any point around the circle will always have identical components of velocity that are perpendicular to the radius on either side of the point being considered. Thus, the centripetal acceleration is always directed towards the centre of the circle.

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13
Q

Define radian

A

A radian is a unit of angle measurement, equivalent to 57.3 degrees

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14
Q

Define angular displacement

A

Angular displacement is the vector measurement of the angle through which something has moved

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15
Q

Define angular velocity

A

Angular velocity, w is the rate at which the angular displacement changes, unit is radians per second

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16
Q

Define centripetal acceleration

A

Centripetal acceleration, a is the acceleration towards the centre of a circle that corresponds to the changes in direction to maintain an objects motion around that circle

17
Q

How does circular motion work

A

When a hammer thrower whirls an athletic hammer around in a circle, the hammer has an angular velocity. Yet when the thrower lets the hammer go, it will fly off, following a straight line which is the direction in which it was moving at the instant of release.

The direction is always along the edge of the circle (a tangent) at the point when it was released

18
Q

Tell me about an example with centripetal force - a hammer thrower/ what is centripetal force

A

As the hammer is whirled at a constant speed, the magnitude of the velocity is always the same. However, the direction of the velocity is constantly working. This means that the vector of velocity is constantly changing, and a change in velocity is an acceleration. Newton’s first law tells us that acceleration will only happen if there is a resultant force. The hammer is constantly being pulled towards the centre of the circle. In this example, the force providing this pull is the tension in the string (or chain).

For any object moving in a circle, there must be a resultant force to cause this acceleration, and it is called centripetal force

19
Q

Are there any special centripetal forces?

A

No, there is no special centripetal force, any resultant force that makes an object move in a circle is labelled as a centripetal force

Eg tension, weight etc.

20
Q

How can we find the formula for the centripetal force

A

The formula for the centripetal force on an object moving in a circle can be found from Newton’s second law, and we already derived the formula for centripetal acceleration

F = ma

a = v^2/r

So 
Centripetal force (f) = mv^2/r

Since v = r w

Centripetal force is also equal to

F = mrw^2

21
Q

When will the resultant centripetal force needed be larger

A

The resultant centripetal force needed will be larger if…

The rotating object has more mass

The object rotated faster

The object is further away from the centre of the circle.

22
Q

Formula for angular displacement

A

Theta = s/r

23
Q

Formula for angular velocity

A

w = 2 x pi x f = 2pi/T

Therefore, w = v/r

24
Q

Formula for centripetal acceleration

A

a = r w^2 = v^2/r

25
Q

What’s the formula for centripetal force

A

F = mrw^2

Or F = mv^2/r

26
Q

How can we investigate centripetal force practical

A

This is about verifying the centripetal force equation. Eye protection should be worn during this investigation.

You can investigate the centripetal force equation by spinning a rubber bung on a string around in a circle. The tension In the string, which is the centripetal force, will be provided by the hanging masses at the bottom of the vertical string and thus will be known. Spin the rubber bung around in a circle that keeps a paper clip marker in a constant position near the handle. The paperclip marker allows you to maintain a fixed length of string (radius) which you can measure. You will also need to measure the mass of the rubber bung. Your partner can then time ten revolutions in order to give you the angular velocity. Take angular velocity measurements for different forces (different numbers of hanging masses)

F = mrw^2
Therefore

W^2 = F/mr

A graph of w^2 plotted against F should give a straight line of best fit. The gradient is 1/mr - these are both constants

27
Q

Define centripetal force

A

Centripetal force is the resultant force towards the centre of the circle to maintain an objects circular motion.