Further Mechanics: Impulse, Momentum, and Circular Motion

0.0(0)
Studied by 0 people
call kaiCall Kai
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
GameKnowt Play
Card Sorting

1/12

flashcard set

Earn XP

Description and Tags

Flashcards covering vocabulary and key concepts for Impulse, Momentum conservation, Collisions, and Circular Motion based on the lecture notes.

Last updated 9:19 AM on 5/13/26
Name
Mastery
Learn
Test
Matching
Spaced
Call with Kai

No analytics yet

Send a link to your students to track their progress

13 Terms

1
New cards

Impulse

The product of a constant force and impact time (F×tF\times\text{t}), which is equivalent to the change in momentum (Δp\text{Δp} ). Where F is a constant force, t is impact time and p is momentum.

2
New cards

Conservation of linear momentum

The principle stating that momentum is always conserved in any interaction where no external forces act, meaning momentum before an event equals momentum after. Important to note that momentum can be conserved differently along different dimensions. Approach required to solve problems in relation to the conservation of momentum in 2 dimensions is to resolve motion into components along perpendicular axis and solve thee resultant pair of problems in one dimension simultaneously.

<p>The principle stating that momentum is always conserved in any interaction where no external forces act, meaning momentum before an event equals momentum after. Important to note that momentum can be conserved differently along different dimensions. Approach required to solve problems in relation to the conservation of momentum in 2 dimensions is to resolve motion into components along perpendicular axis and solve thee resultant pair of problems in one dimension simultaneously.</p>
3
New cards

Elastic collision

A type of collision where both momentum and kinetic energy are conserved.

4
New cards

Inelastic collision

A type of collision where only momentum is conserved, while some kinetic energy is converted into other forms like heat, sound, or gravitational potential and may be larger or smaller after the collision. If objects which collide stick together after the collision then this is an inelastic collision.

5
New cards

Explosion

An example of an inelastic collision where the kinetic energy after the event is greater than the kinetic energy before.

6
New cards

Non-relativistic particle

A particle traveling at speeds below those comparable to the speed of light.

7
New cards

Kinetic energy (non-relativistic formula)

The formula used to calculate energy for particles below relativistic speeds, expressed as Ek=p22mE_k = \frac{p^2}{2m}.

<p>The formula used to calculate energy for particles below relativistic speeds, expressed as $$E_k = \frac{p^2}{2m}$$.</p>
8
New cards

Radian

The unit of angle defined as the angle in the sector of a circle when the arc length of that sector is equal to the radius of the circle. One complete circle is 2π\pi rad.

<p>The unit of angle defined as the angle in the sector of a circle when the arc length of that sector is equal to the radius of the circle. One complete circle is 2$$\pi$$ rad.</p>
9
New cards

Angular displacement (θ\theta)

The angle turned through by an object in any given direction, measured in radians or degrees.

<p>The angle turned through by an object in any given direction, measured in radians or degrees.</p>
10
New cards

Angular velocity (ω\text{ω})

The angle an object moves through per unit time, calculated by dividing linear velocity by radius (ω=vr\text{ω} = \frac{v}{r}) or dividing 2π2\text{π} by the time period (ω=2πT\text{ω} = \frac{2\text{π}}{T}).

11
New cards

Centripetal acceleration

The acceleration experienced by objects moving in a circular path, expressed as a=v2ra = \frac{v^2}{r} or a=rω2a = r\text{ω}^2.

<p>The acceleration experienced by objects moving in a circular path, expressed as $$a = \frac{v^2}{r}$$ or $$a = r\text{ω}^2$$.</p>
12
New cards

Circular motion

Object moving in a circular path at a constant speed has a constantly changing velocity therefore the object must be accelerating (known as centripetal acceleration). Newton’s first law states that to accelerate, an object must experience a resultant force, therefore object moving in a circle must experience centripetal force.

<p>Object moving in a circular path at a constant speed has a constantly changing velocity therefore the object must be accelerating (known as centripetal acceleration). Newton’s first law states that to accelerate, an object must experience a resultant force, therefore object moving in a circle must experience centripetal force.</p>
13
New cards

Centripetal force

The resultant force required to produce and maintain circular motion, which always acts towards the centre of the circle (F=mv2rF = \frac{mv^2}{r} or F=mrω2F = mr\text{ω}^2).

<p>The resultant force required to produce and maintain circular motion, which always acts towards the centre of the circle ($$F = \frac{mv^2}{r}$$ or $$F = mr\text{ω}^2$$).</p>