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E.m.f has the same unit as electric potential, hence they are dimensionally equivalent. From Electrostatics, potential difference = kq/r where k=constant (Nm2C-2), q=charge (C), r=distance (m). Find the dimensions of P.d.

Physics

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Answer

[Pd]=ML2T−3I−1\mathrm{[Pd]} = \mathrm{M L^{2} T^{-3} I^{-1}}

Step-by-step solution

5 steps
  1. Potential difference from electrostatics

    Pd=kqr\mathrm{Pd} = \frac{k q}{r}

    where [k]=N⋅m2⋅C−2[k] = \mathrm{N \cdot m^2 \cdot C^{-2}}, [q]=C[q] = \mathrm{C}, [r]=m[r] = \mathrm{m}.

    Substitute dimensions:

    [Pd]=[N⋅m2⋅C−2]⋅[C][m]=N⋅m⋅C−1.[\mathrm{Pd}] = \frac{[\mathrm{N \cdot m^2 \cdot C^{-2}}] \cdot [\mathrm{C}]}{[\mathrm{m}]} = \mathrm{N \cdot m \cdot C^{-1}}.
  2. Dimensions of force

    [N]=[F]=MLT−2.[\mathrm{N}] = [\mathrm{F}] = \mathrm{M L T^{-2}}.

    Thus,

    [Pd]=(MLT−2)⋅L⋅C−1=ML2T−2C−1.[\mathrm{Pd}] = (\mathrm{M L T^{-2}}) \cdot \mathrm{L} \cdot \mathrm{C^{-1}} = \mathrm{M L^2 T^{-2} C^{-1}}.
  3. Dimensions of charge

    [C]=[A⋅s]=IT.[\mathrm{C}] = [\mathrm{A \cdot s}] = \mathrm{I T}.

    Substitute:

    [Pd]=ML2T−2⋅(IT)−1=ML2T−2⋅I−1T−1=ML2T−3I−1.[\mathrm{Pd}] = \mathrm{M L^2 T^{-2}} \cdot (\mathrm{I T})^{-1} = \mathrm{M L^2 T^{-2} \cdot I^{-1} T^{-1}} = \mathrm{M L^2 T^{-3} I^{-1}}.
  4. Confirm from work per unit charge

    Work done =F⋅r= \mathrm{F \cdot r}, so

    [work]=(MLT−2)⋅L=ML2T−2.[\text{work}] = (\mathrm{M L T^{-2}}) \cdot \mathrm{L} = \mathrm{M L^2 T^{-2}}. [Pd]=[work][q]=ML2T−2IT=ML2T−3I−1.[\mathrm{Pd}] = \frac{[\text{work}]}{[q]} = \frac{\mathrm{M L^2 T^{-2}}}{\mathrm{I T}} = \mathrm{M L^2 T^{-3} I^{-1}}.
  5. E.M.F.

    has same dimensions as electric potential difference.

    [Pd]=ML2T−3I−1\mathrm{[Pd]} = \mathrm{M L^{2} T^{-3} I^{-1}}
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