Two Rotating Discs Coupled: Finding the Common Angular Speed

Physics · System Of Particles And Rotational Motion · NEET

When two discs spinning on the same axis are pressed face-to-face, no outside torque acts, so total angular momentum stays the same. The common speed is ω = (I1·ω1 + I2·ω2) / (I1 + I2). Memory hook: "momentum shares out, energy is lost" — L is conserved, but kinetic energy always drops because friction does the coupling.
Two coaxial discs coupled on a common axisaxisI1, ω1I2, ω2pressed togetherI1+I2, ωone bodyL conservedω = (I1ω1+I2ω2)/(I1+I2)
Two discs on the same axis are pressed together. Internal friction gives no external torque, so angular momentum is conserved: the final common speed is ω = (I1·ω1 + I2·ω2)/(I1 + I2). Kinetic energy drops because the faces slide.

Your doubts, answered

Why is angular momentum conserved but kinetic energy is not?

During coupling, the only torque is the internal friction between the two disc faces. Internal torques come in action-reaction pairs, so they cancel and do NOT change total L. That is why L1 + L2 stays constant. But that same friction slides the surfaces against each other and turns some rotational kinetic energy into heat. So use L conservation to find ω, never energy conservation. Energy is lost unless ω1 = ω2 to begin with.

Two discs on the SAME axis vs two discs touching at their RIMS - are they the same problem?

No, and NEET mixes them up on purpose. Same-axis (coaxial, face-to-face): they end at ONE common ω, use L1 + L2 = (I1+I2)ω. Rim-in-contact (edges touch, like gears): the discs keep separate axes and DO NOT reach one common ω. Instead their contact-point speeds match: R1·ω1 = R2·ω2, so ω1/ω2 = R2/R1. Read the question: 'brought face-to-face' or 'common axis' = coaxial; 'edges/rims touch' = surface-speed matching.

How do I get the common angular speed step by step?

Step 1: write total angular momentum before = I1·ω1 + I2·ω2 (add signs if directions differ). Step 2: after coupling both move as one body with moment of inertia I1 + I2 at speed ω. Step 3: set before = after: I1·ω1 + I2·ω2 = (I1+I2)·ω. Step 4: solve ω = (I1·ω1 + I2·ω2)/(I1+I2). For two identical discs (I1 = I2 = I) this becomes the simple average ω = (ω1+ω2)/2.

What if the discs spin in opposite directions?

Give one direction + and the other -. If disc 2 spins the opposite way, ω2 is negative in the formula: ω = (I·ω1 - I·ω2)/(2I). If they are equal and opposite (ω1 = ω, ω2 = -ω), the common speed is zero - they stop each other. All the initial kinetic energy is then lost as heat.

Can I find the energy lost quickly?

Yes. Energy lost = KE(before) - KE(after). For two identical discs, this reduces to a clean form: loss = (1/4)·I·(ω1 - ω2)². Notice it depends on the DIFFERENCE in speeds, so if ω1 = ω2 there is zero loss (nothing slides), and the loss is largest when they spin oppositely.

⚠️ The NEET trap
Using kinetic energy conservation: (1/2)I1ω1² + (1/2)I2ω2² = (1/2)(I1+I2)ω² to solve for the common speed.
Use angular momentum conservation: I1ω1 + I2ω2 = (I1+I2)ω. Kinetic energy is NOT conserved because friction between the faces dissipates energy as heat.
🧠 Coupling = collision. Just like a perfectly inelastic collision conserves momentum (not KE), coupled discs conserve angular momentum (not KE).

Real NEET questions

NEET 2017

Two discs of equal moment of inertia I, rotating about their common axis with angular speeds ω1 and ω2, are brought face-to-face into contact (axes coinciding). The loss of energy in the process is:

A · (1/2) I (ω1 - ω2)²
B · (1/4) I (ω1 - ω2)²
C · I (ω1 - ω2)²
D · (1/8) I (ω1 - ω2)²
Solution: Conserve angular momentum (only internal friction acts): Iω1 + Iω2 = (2I)ωf, so ωf = (ω1 + ω2)/2. Initial KE = (1/2)I ω1² + (1/2)I ω2² = (1/2)I(ω1² + ω2²). Final KE = (1/2)(2I)ωf² = I·[(ω1+ω2)/2]² = (I/4)(ω1+ω2)². Loss = (1/2)I(ω1²+ω2²) - (I/4)(ω1+ω2)². Expand: (I/4)[2ω1²+2ω2² - (ω1²+2ω1ω2+ω2²)] = (I/4)(ω1² - 2ω1ω2 + ω2²) = (1/4)I(ω1 - ω2)². Answer B.

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Frequently asked

What is the formula for the common angular speed of two coupled discs?

ω = (I1·ω1 + I2·ω2)/(I1 + I2). For two identical discs it simplifies to the average ω = (ω1 + ω2)/2.

Is angular momentum conserved when two discs couple?

Yes. The coupling force is internal friction, which produces no net external torque, so total angular momentum before equals total after.

Why does the system lose kinetic energy?

The two faces slide against each other while gripping. This kinetic friction converts rotational kinetic energy into heat, so final KE is always less than initial KE (unless the discs already had the same speed).

How is the rim-contact (gear) case different?

When discs touch at their rims and keep separate axes, they do NOT share one ω. Their contact points have equal linear speed: R1·ω1 = R2·ω2, giving ω1/ω2 = R2/R1 (smaller disc spins faster).

What happens if the discs spin in opposite directions?

Take one direction as negative in the formula. Equal and opposite speeds give ω = 0 (they stop), and all the kinetic energy is lost as heat.