CLASSICAL-MECHANICS Β· Interactive Practice | Unit 1 Β· Video 6

The Hidden Grammar of Physics: How M, L, and T Encode Every Quantity

IKey Formulas

Concept Dimensional Formula Notes
Velocity [v]=Lβ‹…Tβˆ’1[v] = L \cdot T^{-1} distance / time
Force [F]=Mβ‹…Lβ‹…Tβˆ’2[F] = M \cdot L \cdot T^{-2} mass Γ— acceleration
Work / Energy / Torque [E]=Mβ‹…L2β‹…Tβˆ’2[E] = M \cdot L^{2} \cdot T^{-2} the shared "fingerprint"
Power [P]=Mβ‹…L2β‹…Tβˆ’3[P] = M \cdot L^{2} \cdot T^{-3} energy / time

The Big Idea: Every derived quantity is a product of powers of MM, LL, TT. Sharing dimensions signals a relationship β€” but not necessarily equivalence.

IIVisualization 1 β€” The Dimensional Builder

Which powers of MM, LL, and TT produce the energy fingerprint β€” and which quantities share it?

πŸ’‘ Challenge: from the energy fingerprint Mβ‹…L2β‹…Tβˆ’2M \cdot L^{2} \cdot T^{-2}, drop the TT power once more to Mβ‹…L2β‹…Tβˆ’3M \cdot L^{2} \cdot T^{-3} β€” the dimensions of power.

IIIVisualization 2 β€” Building Quantities from the Ground Up

Each quantity inherits its dimensions from the one before it, one base dimension at a time.

IVVisualization 3 β€” Reverse-Engineering Constants

A constant's dimensions are forced on it by the law it lives in β€” isolate it, substitute, simplify.

Defining law
F=G m1m2r2F = \dfrac{G\, m_1 m_2}{r^{2}}
Isolate the constant
G=F r2m1m2G = \dfrac{F\, r^{2}}{m_1 m_2}
Substitute dimensions
[G]=(Mβ‹…Lβ‹…Tβˆ’2) L2M2[G] = \dfrac{(M \cdot L \cdot T^{-2})\, L^{2}}{M^{2}}
Simplify
[G]=L3β‹…Mβˆ’1β‹…Tβˆ’2[G] = L^{3} \cdot M^{-1} \cdot T^{-2}
Defining law
E=hfE = h f
Isolate the constant
h=Efh = \dfrac{E}{f}
Substitute dimensions
[h]=Mβ‹…L2β‹…Tβˆ’2Tβˆ’1[h] = \dfrac{M \cdot L^{2} \cdot T^{-2}}{T^{-1}}
Simplify
[h]=Mβ‹…L2β‹…Tβˆ’1[h] = M \cdot L^{2} \cdot T^{-1}
Defining law
F=14πΡ0e2r2F = \dfrac{1}{4\pi\varepsilon_0}\dfrac{e^{2}}{r^{2}}
Isolate the constant
14πΡ0=F r2e2\dfrac{1}{4\pi\varepsilon_0} = \dfrac{F\, r^{2}}{e^{2}}
Substitute dimensions
[14πΡ0]e2=(Mβ‹…Lβ‹…Tβˆ’2) L2\left[\tfrac{1}{4\pi\varepsilon_0}\right] e^{2} = (M \cdot L \cdot T^{-2})\, L^{2}
Simplify
[14πΡ0]=Mβ‹…L3β‹…Tβˆ’2Β (perΒ charge2)\left[\tfrac{1}{4\pi\varepsilon_0}\right] = M \cdot L^{3} \cdot T^{-2}\ (\text{per charge}^{2})

πŸ’‘ A constant's numerical value changes between unit systems, but its dimensional formula never does.

VQuiz Questions

Question 1

Velocity is distance divided by time. What is the dimensional formula of velocity?

βœ… Correct! Distance (L) over time (T) gives L Β· T⁻¹.

❌ Not quite. Dividing by time gives a negative power of T, and no mass is involved.

Show solution

Solution:

Velocity is distance over time: [v]=LT=Lβ‹…Tβˆ’1[v] = \frac{L}{T} = L \cdot T^{-1}

Dividing by time means a negative power of TT. There is no mass involved, so MM does not appear.

Question 2

Kinetic energy is 12mv2\tfrac{1}{2}mv^{2}. A common mistake is to forget that the velocity term is squared. What is the correct dimensional formula of kinetic energy?

βœ… Correct! Squaring velocity gives LΒ² Β· T⁻², times mass = M Β· LΒ² Β· T⁻².

❌ Not quite. That is the dimension of force. You forgot to square the velocity.

❌ Not quite. Remember velocity is squared, so both its L and T powers double.

Show solution

Solution:

The factor 12\tfrac{1}{2} is a pure number and carries no dimension. So: [KE]=Mβ‹…(Lβ‹…Tβˆ’1)2=Mβ‹…L2β‹…Tβˆ’2[KE] = M \cdot (L \cdot T^{-1})^{2} = M \cdot L^{2} \cdot T^{-2}

Squaring the velocity squares both the L and T powers. This is the same "fingerprint" shared by work and torque.

Question 3

Newton's law of gravitation is F=G m1m2r2F = \dfrac{G\, m_1 m_2}{r^{2}}. Isolating GG gives G=F r2m1m2G = \dfrac{F\, r^{2}}{m_1 m_2}.

Using [F]=Mβ‹…Lβ‹…Tβˆ’2[F] = M \cdot L \cdot T^{-2}, what is the dimensional formula of GG?

βœ… Correct! The two masses in the denominator give M⁻¹, and LΒΉΒ·LΒ² = LΒ³.

❌ Not quite. Watch the mass: dividing by m₁mβ‚‚ (= MΒ²) against the MΒΉ from force gives M⁻¹, not MΒΉ.

❌ Not quite. Combine L¹ (from force) with L² (from r²) to get L³, and track the mass powers carefully.

Show solution

Solution:

Substitute the dimensions into G=F r2m1m2G = \dfrac{F\, r^{2}}{m_1 m_2}: [G]=(Mβ‹…Lβ‹…Tβˆ’2)β‹…L2M2[G] = \frac{(M \cdot L \cdot T^{-2}) \cdot L^{2}}{M^{2}}

Combine the L powers: L1β‹…L2=L3L^{1} \cdot L^{2} = L^{3}. The mass powers: M1M2=Mβˆ’1\dfrac{M^{1}}{M^{2}} = M^{-1}.

[G]=L3β‹…Mβˆ’1β‹…Tβˆ’2[G] = L^{3} \cdot M^{-1} \cdot T^{-2}

Question 4

Work and torque both have the dimensional formula Mβ‹…L2β‹…Tβˆ’2M \cdot L^{2} \cdot T^{-2}.

True or False: Because they share the same dimensions, work and torque are physically the same quantity.

βœ… Correct! Same dimensions β‰  same thing. Work is a dot product; torque is a cross product.

❌ Not quite. Shared dimensions reveal a relationship, but work and torque are genuinely different quantities.

Show solution

Solution:

False. Sharing dimensions signals a relationship, not equivalence.

  • Work is a dot product (Fβƒ—β‹…dβƒ—\vec{F} \cdot \vec{d}) β€” a scalar measure of energy transfer.
  • Torque is a cross product (rβƒ—Γ—Fβƒ—\vec{r} \times \vec{F}) β€” a vector describing rotational tendency.

They carry the identical dimensional fingerprint Mβ‹…L2β‹…Tβˆ’2M \cdot L^{2} \cdot T^{-2}, yet they are fundamentally different physical quantities. Dimensional identity is a clue about structure β€” it does not mean two things are the same.

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