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Answer the following question. Show that the centripetal force on a particle undergoing uniform circular motion is -mrω2. - Physics

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Question

Answer the following question.

Show that the centripetal force on a particle undergoing uniform circular motion is -mrω2.

Answer in Brief
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Solution

  1. Suppose a particle is performing U.C.M in anticlockwise direction. The co-ordinate axes are chosen as shown in the figure.
    Let, A = initial position of the particle which lies on positive X-axis
    P = instantaneous position after time t
    θ = angle made by radius vector
    ω = constant angular speed
    `vec"r"` = instantaneous position vector at time t
  2. From the figure,
    `vec"r" = hat"i""x" + hat"j""y"`
    where, `hat"i" and hat"j"` are unit vectors along X-axis and Y-axis respectively.
  3. Also, x = r cos θ and y = r sin θ
    ∴ `vec"r" = ["r"hat"i"cos theta + "r"hat"j"sin theta]`
    But θ = ωt
    ∴ `vec"r" = ["r"hat"i" cos omega"t" + "r"hat"j" sin omega"t"]`      ....(1)
  4. Velocity of the particle is given as rate of change of position vector.
    ∴ `vec"v" = (vec"dr")/"dt" = "d"/"dt" ["r"hat"i" cos omega"t" + "r" hat"j" sin omega"t"]`
    `= "r"["d"/"dt" cos omega"t"]hat"i" + "r"["d"/"dt" sin omega"t"]hat"j"`
    ∴ `vec"v" = - "r"omega hat"i" sin omega"t" + "r"omega hat"j" cos omega"t"`
    ∴ `vec"v" = "r"omega (-hat"i" sin omega"t" + hat"j" cos omega"t")`
  5. Further, instantaneous linear acceleration of the particle at instant t is given by,
    `vec"a" = (vec"dv")/"dt" = "d"/"dt"["r"omega(- hat"i" sin omega "t" + hat"j" cos omega"t")]`
    `= "r"omega ["d"/"dt" (- hat"i" sin omega"t" + hat"j" cos omega "t")]`
    `= "r"omega ["d"/"dt" (- sin omega"t")hat"i" + "d"/"dt"(cos omega "t")hat"j"]`
    `= "r"omega(-omega hat"i" cos omega"t" - omega hat"j" sin omega "t")`
    `= - "r"omega^2(hat"i" cos omega "t" + hat"j" sin omega"t")`
    ∴ `vec"a" = - omega^2("r"hat"i" cos omega"t" + "r" hat"j" sin omega "t")`        ....(2)
  6. From equation (1) and (2),
    `vec"a" = - omega^2vec"r"`      ....(3)
    The negative sign shows that the direction of acceleration is opposite to the direction of the position vector. Equation (3) is the centripetal acceleration.
  7. The magnitude of centripetal acceleration is given by,
    a = `omega^2"r"`
  8. The force providing this acceleration should also be in the same direction, hence centripetal.
    ∴ `vec"F" = "m"vec"a" = - "m"omega^2vec"r"`
    This is the expression for the centripetal force on a particle undergoing uniform circular motion.
  9. Magnitude of F = `"m"omega^2"r" = "mv"^2/"r"` = mωv
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Chapter 3: Motion in a Plane - Exercises [Page 45]

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Balbharati Physics [English] Standard 11 Maharashtra State Board
Chapter 3 Motion in a Plane
Exercises | Q 2. (x) | Page 45

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