Kinetic Energy and Momentum
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Kinetic energy and momentum for JEE Main and Advanced: K = ½mv², the relation K = p²/2m and p = √(2mK), which body has more kinetic energy at the same momentum and more momentum at the same kinetic energy, scaling and small-change rules, the zero total momentum trap, and two solved problems: a bullet against a sprinter, and a 300% rise in kinetic energy.
Chapters
- 0:00Introduction
- 0:36Kinetic energy, and its link to momentum
- 1:48Comparing two bodies
- 2:36Scaling and small changes
- 3:44Trap: zero momentum, so zero kinetic energy?
- 4:26Example 1: bullet vs sprinter, K and p compared
- 6:21Example 2: K rises 300 percent, how much does p rise
- 7:48Quick revision: K = p^2/2m and comparing two bodies
Transcript
0:00Introduction
Hello everyone! Let's start with a small contest. On one side, a fifty gram bullet flying at four hundred metres per second. On the other side, a fifty kilogram sprinter running at eight metres per second. Which one has more kinetic energy? And which one has more momentum? The bullet, for both, right? Hmm, not so fast. By the end of this lesson, you will see the answer is split. Kinetic energy and momentum come up often in JEE problems, so this link between them is worth knowing well. Let's begin.
0:36Kinetic energy, and its link to momentum
So, the energy of motion: kinetic energy. For a body of mass m moving with speed v, the kinetic energy, capital K, equals half m v squared. That is one half, times m, times v squared, okay? Now tell me: can kinetic energy ever be negative? No, never! Mass is positive, and v squared can never be negative. So kinetic energy is a scalar, and it is never negative. And it depends on the frame of reference, because the speed v depends on who is measuring it. Right? Now bring in momentum: p equals m times v. Can you write the kinetic energy using p instead of v? Yes, multiply the top and the bottom by m. Then K equals m squared v squared over two m. And m squared v squared is just p squared. So, K equals p squared over two m. Clear? Turn it around, and p equals the square root of two m K; that is the square root sign on screen. Keep both forms ready: a question may give you the kinetic energy and ask for the momentum, or the other way round. With me?
1:48Comparing two bodies
Now, a comparison that comes up often. Two bodies, one light and one heavy, with the same momentum. Which one has more kinetic energy? The lighter one! Yes, exactly! Look at K equals p squared over two m. With p fixed, K is proportional to one over m. The sign that looks like a stretched Greek alpha means proportional to, okay? Smaller mass, more kinetic energy. Now flip it: the same kinetic energy. From p equals root two m K, p is proportional to root m. So now the heavier body has more momentum. Got it? And the speed: v is p over m, so v is proportional to one over root m. With the same kinetic energy, the lighter body is faster. Right?
2:36Scaling and small changes
Next, scaling. Suppose p becomes lambda times p. Lambda, the Greek letter, is just a number. The single arrow means becomes, and the double arrow means implies. Since K goes as p squared, K becomes lambda squared times K, okay? Now the reverse. If the kinetic energy becomes lambda times K, what does the momentum become? Root lambda times p. Correct! Because p goes as the square root of K, right? Now, small changes in the same body. Delta, the little triangle, means a change. Delta K over K, the fractional change in K, is approximately two times delta p over p, which equals two times delta v over v. The wavy equals sign means approximately. The square doubles the percentage, but only for small changes. Remember that word: small. Got it? And for errors in measurement, the fractional errors add: delta K over K equals delta m over m, plus two times delta v over v. The power two on v becomes a factor of two on its error. With me?
3:44Trap: zero momentum, so zero kinetic energy?
Now an important trap. For one body, kinetic energy and momentum go together: if it has one, it has the other. Both are zero only when the body is at rest. Okay? Now take two equal balls moving towards each other with equal speeds. Their momenta are equal and opposite, so the total momentum is zero. So the total kinetic energy is zero too, right? No, no, careful! Momentum is a vector, so opposite momenta cancel. But kinetic energy is a scalar and never negative, so the two energies simply add. Each ball has K greater than zero, so the total is greater than zero. Clear?
4:26Example 1: bullet vs sprinter, K and p compared
Now, remember our contest from the start? Let's settle it. Compare the kinetic energies and the momenta of a fifty gram bullet, small g on screen, moving at four hundred metres per second, and a fifty kilogram sprinter running at eight metres per second. The m s to the minus one on screen means metres per second. Pause the video, and try it first. Done? Okay, let's check. Bullet first. Its mass is fifty, so we put m equals fifty, right? Oh no, careful! Fifty grams, not fifty kilograms. In S I units, m equals zero point zero five kilogram. Easy marks are lost right here. Got it? Now, K equals one half times zero point zero five times four hundred squared. Four hundred squared is one hundred and sixty thousand; times zero point zero five gives eight thousand; and half of that is four thousand joules, capital J for joule. Okay? And its momentum: p equals zero point zero five times four hundred, that is twenty kilogram metre per second. With me? Now the sprinter. K equals one half times fifty times eight squared: half of fifty times sixty four, so one thousand six hundred joules. And p equals fifty times eight: four hundred kilogram metre per second. Right? Compare the energies. Four thousand over one thousand six hundred is two point five. So the bullet has two point five times the kinetic energy. Clear? Now the momenta. Four hundred over twenty is twenty. The sprinter has twenty times the momentum! So our contest really is split: the light, fast bullet wins on energy, and the heavy sprinter wins on momentum. Speed is squared in K, but not in p. That's it!
6:21Example 2: K rises 300 percent, how much does p rise
Now a slightly harder one. The kinetic energy of a body increases by three hundred percent; the percent sign is on screen. By what percentage does its momentum increase? Pause and try. Hint: first find what the kinetic energy becomes. Done? Okay, let's check. It increases by three hundred percent. So the new kinetic energy is three times K, right? No, no, wait! That is the first trap. Increase by three hundred percent means we add three K to the original K, so K becomes four K; the arrow again means becomes. Okay? Now, it is the same body, so the mass is fixed. If K becomes four times K, what does the momentum become? Yes, exactly! p equals root two m K, so p becomes root four times p, that is two p. The momentum doubles. Right? So the increase is two p minus p, over p, times one hundred percent: one hundred percent. That is the answer. Got it? And now the second trap. Some students use the small-change rule: half of three hundred, so one hundred and fifty percent. Wrong! That rule is only for small changes, and three hundred percent is not small. For big changes, find the new value exactly, as we just did. Clear?
7:48Quick revision: K = p^2/2m and comparing two bodies
So, quick revision. K equals half m v squared, which equals p squared over two m, and p equals root two m K, okay? Same momentum: the lighter body has more kinetic energy. Same kinetic energy: the heavier body has more momentum. And for big changes, scale exactly: K becoming four K means p becomes two p. Now go and try the practice problems on this page. You will do them well, I am sure. All the best!
More videos in Unit 4 · Work, Energy & Power
- Work Done by a Constant Force
- Work Using Components and Along Paths
- Work Done by a Variable Force
- Work Done by Springs and by Friction
- Conservative and Non-conservative Forces
- The Work–Energy Theorem
- Using the Theorem with Position, Velocity and Time Data
- Systems of Bodies, Strings and Internal Work
- Energy Conversion, Heat and Efficiency
- Potential Energy and Conservative Forces
- Elastic Potential Energy of a Spring
- Conservation of Mechanical Energy
- Non-conservative Forces: W_(nc)=ΔE
- Potential-Energy Curves and Equilibrium
- Average and Instantaneous Power
- Vehicles, Lifts and Pumps
- Motion Under Constant Power
- Power in Flows: Conveyor Belts, Wind and Water
- Speed and Tension in a Vertical Circle
- When the String Slackens; Rods and Beads
- Loops, Humps and Dips on Tracks
- Sliding Off a Smooth Sphere
- Impulse and Momentum
- Perfectly Inelastic Collisions
- Elastic Collisions in One Dimension
- Coefficient of Restitution
- Collisions Through Springs and on Wedges; Chains of Collisions
- Momentum Conservation in Two Dimensions
- Oblique Impact: Walls, Floors and Smooth Spheres
- Overview
- Set 1 (Work and Energy)
- Set 2 (Power, Vertical Circles and Potential-Energy Curves)
- Set 3 (Impulse, Collisions and Explosions)
- Overview
- Part A: JEE Main Level
- Part B: Harder Problems
- Part C: Concept Checks