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Determine the dimensions of each variable.

Computer Science

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a) To show that the equation is homogeneous, we need to verify that the dimensions on both sides of the equation are the same. We will use the base dimensions of Mass $[M]$, Length $[L]$, Time $[T]$, and Current $[I]$.

  1. Determine the dimensions of each variable.

    • Specific charge δ\delta: charge per unit mass. [δ]=chargemass=[IT][M]=[M−1IT][\delta] = \frac{\text{charge}}{\text{mass}} = \frac{[IT]}{[M]} = [M^{-1}IT]
    • Potential difference UU: energy per unit charge. Energy has dimensions of work, which is force ×\times distance ([MLT−2]×[L]=[ML2T−2][MLT^{-2}] \times [L] = [ML^2T^{-2}]). [U]=energycharge=[ML2T−2][IT]=[ML2T−3I−1][U] = \frac{\text{energy}}{\text{charge}} = \frac{[ML^2T^{-2}]}{[IT]} = [ML^2T^{-3}I^{-1}]
    • Magnetic field BB: From the Lorentz force F=qvBF = qvB, we have B=FqvB = \frac{F}{qv}. [B]=forcecharge×velocity=[MLT−2][IT][LT−1]=[MLT−2][IL]=[MT−2I−1][B] = \frac{\text{force}}{\text{charge} \times \text{velocity}} = \frac{[MLT^{-2}]}{[IT][LT^{-1}]} = \frac{[MLT^{-2}]}{[IL]} = [MT^{-2}I^{-1}]
    • Radius rr: length. [r]=[L][r] = [L]
  2. Calculate the dimension of the Left Hand Side (LHS) of the equation.

    The LHS is δ\delta.

    [LHS]=[δ]=[M−1IT][\text{LHS}] = [\delta] = [M^{-1}IT]
  3. Calculate the dimension of the Right Hand Side (RHS) of the equation.

    The RHS is 2UB2r2\frac{2U}{B^2r^2}. The numerical constant '2' is dimensionless.

    [RHS]=[U][B]2[r]2=[ML2T−3I−1]([MT−2I−1])2([L])2[\text{RHS}] = \frac{[U]}{[B]^2[r]^2} = \frac{[ML^2T^{-3}I^{-1}]}{([MT^{-2}I^{-1}])^2([L])^2} [RHS]=[ML2T−3I−1][M2T−4I−2][L2][\text{RHS}] = \frac{[ML^2T^{-3}I^{-1}]}{[M^2T^{-4}I^{-2}][L^2]} [RHS]=[M1−2L2−2T−3−(−4)I−1−(−2)][\text{RHS}] = [M^{1-2}L^{2-2}T^{-3-(-4)}I^{-1-(-2)}] [RHS]=[M−1L0T1I1]=[M−1IT][\text{RHS}] = [M^{-1}L^0T^1I^1] = [M^{-1}IT]
  4. Compare the dimensions of the LHS and RHS.

    Since [LHS]=[M−1IT][\text{LHS}] = [M^{-1}IT] and [RHS]=[M−1IT][\text{RHS}] = [M^{-1}IT], the dimensions on both sides are identical.
    Therefore, the equation δ=2UB2r2\delta = \frac{2U}{B^2r^2} is homogeneous.

    b)

    • All correct equations must be homogeneous: This means that for any physically correct equation, the dimensions of the physical quantities on both sides of the equation must be identical. If the dimensions do not match, the equation is fundamentally incorrect and cannot describe a real physical phenomenon. Dimensional homogeneity is a necessary condition for an equation to be valid.

    • Not all homogeneous equations are physically correct: An equation can be dimensionally homogeneous but still be physically incorrect. This is because dimensional analysis does not account for dimensionless numerical constants (like 12\frac{1}{2}, 2π2\pi, etc.) or the precise functional relationship between variables. It only checks the consistency of units, not the accuracy of the physical law.

    Example:
    Consider the kinetic energy (KEKE) of an object with mass mm and velocity vv.
    The physically correct equation for kinetic energy is:

    KE=12mv2KE = \frac{1}{2}mv^2

    The dimension of kinetic energy is [ML2T−2][ML^2T^{-2}].
    The dimensions of the RHS are [M][LT−1]2=[ML2T−2][M][LT^{-1}]^2 = [ML^2T^{-2}].
    This equation is dimensionally homogeneous.

    Now, consider a proposed equation for kinetic energy that is dimensionally homogeneous but physically incorrect:

    KE=mv2KE = mv^2

    The dimensions of the RHS are [M][LT−1]2=[ML2T−2][M][LT^{-1}]^2 = [ML^2T^{-2}].
    This equation is also dimensionally homogeneous, as both sides have dimensions of [ML2T−2][ML^2T^{-2}].
    However, it is physically incorrect because the numerical constant 12\frac{1}{2} is missing. This example demonstrates that while dimensional homogeneity is a necessary condition for a correct equation, it is not a sufficient condition.

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