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Calculate the gravitational force and initial accelerations of two particles with given masses and separation.

Physics

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Question 12. b. (i): Gravitational force and initial accelerations

  1. Identify the given values and convert units.

    Mass of particle 1: m1=1 kgm_1 = 1 \text{ kg}.
    Mass of particle 2: m2=2 kgm_2 = 2 \text{ kg}.
    Separation distance: r=50 cm=0.50 mr = 50 \text{ cm} = 0.50 \text{ m}.
    Gravitational constant: G=6.674×10−11 N m2/kg2G = 6.674 \times 10^{-11} \text{ N m}^2/\text{kg}^2.

  2. Calculate the gravitational force (FF) between the particles.

    Using Newton's Law of Universal Gravitation:

    F=Gm1m2r2F = G \frac{m_1 m_2}{r^2} F=(6.674×10−11 N m2/kg2)(1 kg)(2 kg)(0.50 m)2F = (6.674 \times 10^{-11} \text{ N m}^2/\text{kg}^2) \frac{(1 \text{ kg})(2 \text{ kg})}{(0.50 \text{ m})^2} F=(6.674×10−11)20.25 NF = (6.674 \times 10^{-11}) \frac{2}{0.25} \text{ N} F=(6.674×10−11)×8 NF = (6.674 \times 10^{-11}) \times 8 \text{ N} F=5.3392×10−10 NF = 5.3392 \times 10^{-10} \text{ N}
  3. Calculate the initial acceleration of each particle.

    Using Newton's Second Law (F=maF = ma):
    For particle 1 (m1m_1):

    a1=Fm1=5.3392×10−10 N1 kga_1 = \frac{F}{m_1} = \frac{5.3392 \times 10^{-10} \text{ N}}{1 \text{ kg}} a1=5.3392×10−10 m/s2a_1 = 5.3392 \times 10^{-10} \text{ m/s}^2

    For particle 2 (m2m_2):

    a2=Fm2=5.3392×10−10 N2 kga_2 = \frac{F}{m_2} = \frac{5.3392 \times 10^{-10} \text{ N}}{2 \text{ kg}} a2=2.6696×10−10 m/s2a_2 = 2.6696 \times 10^{-10} \text{ m/s}^2

    The gravitational force is 5.34×10−10 N\boxed{5.34 \times 10^{-10} \text{ N}}.
    The initial acceleration of the 1 kg particle is 5.34×10−10 m/s2\boxed{5.34 \times 10^{-10} \text{ m/s}^2}.
    The initial acceleration of the 2 kg particle is 2.67×10−10 m/s2\boxed{2.67 \times 10^{-10} \text{ m/s}^2}.

    Question 12. b. (ii): Escape velocity from the moon

  4. Identify the given values and convert units.

    Mass of the moon: M=7.4×1022 kgM = 7.4 \times 10^{22} \text{ kg}.
    Radius of the moon: R=1740 km=1740×103 m=1.74×106 mR = 1740 \text{ km} = 1740 \times 10^3 \text{ m} = 1.74 \times 10^6 \text{ m}.
    Gravitational constant: G=6.674×10−11 N m2/kg2G = 6.674 \times 10^{-11} \text{ N m}^2/\text{kg}^2.

  5. Calculate the escape velocity (vev_e).

    The formula for escape velocity is:

    ve=2GMRv_e = \sqrt{\frac{2GM}{R}} ve=2×(6.674×10−11 N m2/kg2)×(7.4×1022 kg)1.74×106 mv_e = \sqrt{\frac{2 \times (6.674 \times 10^{-11} \text{ N m}^2/\text{kg}^2) \times (7.4 \times 10^{22} \text{ kg})}{1.74 \times 10^6 \text{ m}}} ve=9.87752×10121.74×106 m/sv_e = \sqrt{\frac{9.87752 \times 10^{12}}{1.74 \times 10^6}} \text{ m/s} ve=5.67673×106 m/sv_e = \sqrt{5.67673 \times 10^6} \text{ m/s} ve≈2382.59 m/sv_e \approx 2382.59 \text{ m/s}

    Rounding to two significant figures:

    ve≈2.4×103 m/sv_e \approx 2.4 \times 10^3 \text{ m/s}

    The escape velocity from the moon is:

    2.4×103 m/s\boxed{2.4 \times 10^3 \text{ m/s}}

    Question 13. a. (i): Viscosity and coefficient of viscosity

    • Viscosity: A measure of a fluid's resistance to flow. It describes the internal friction within a fluid when it is in motion. A highly viscous fluid flows slowly, while a low-viscosity fluid flows easily.

    • Coefficient of viscosity (η\eta): A quantitative measure of a fluid's viscosity. It is defined as the ratio of the shear stress to the rate of shear strain in a fluid.

      • SI unit: Pascal-second (Pa⋅s\text{Pa} \cdot \text{s}) or Newton-second per square meter (N s/m2\text{N s/m}^2).
      • Dimensions: [ML−1T−1][ML^{-1}T^{-1}].

    Question 13. a. (ii): Stokes's Law and Terminal Velocity derivation

  6. State the mathematical expression for Stokes's Law and define symbols.

    Stokes's Law describes the viscous drag force (FdF_d) on a small spherical object moving through a viscous fluid at low Reynolds numbers:

    Fd=6πηavF_d = 6\pi \eta a v

    Where:

    • η\eta (eta) is the coefficient of viscosity of the fluid.
    • aa is the radius of the spherical object.
    • vv is the velocity of the spherical object relative to the fluid.
  7. Sketch the forces acting on the sphere.

    When a metallic sphere falls under gravity in a liquid, three forces act on it:

    1. Gravitational force (FgF_g) acting downwards.
    2. Buoyant force (FbF_b) acting upwards (due to Archimedes' principle).
    3. Viscous drag force (FdF_d) acting upwards (due to Stokes's Law).
  8. Show the derivation of terminal velocity.

    At terminal velocity, the net force on the sphere is zero, meaning the upward forces balance the downward force:

    Fg=Fb+FdF_g = F_b + F_d

    Substitute the expressions for each force:

    • Gravitational force: Fg=mg=ρVgF_g = mg = \rho V g, where VV is the volume of the sphere. For a sphere, V=43πa3V = \frac{4}{3}\pi a^3. Fg=ρ(43πa3)gF_g = \rho \left(\frac{4}{3}\pi a^3\right) g
    • Buoyant force: Fb=σVgF_b = \sigma V g, where σ\sigma is the density of the liquid. Fb=σ(43πa3)gF_b = \sigma \left(\frac{4}{3}\pi a^3\right) g
    • Viscous drag force (at terminal velocity vv): Fd=6πηavF_d = 6\pi \eta a v

    Substitute these into the force balance equation:

    ρ(43πa3)g=σ(43πa3)g+6πηav\rho \left(\frac{4}{3}\pi a^3\right) g = \sigma \left(\frac{4}{3}\pi a^3\right) g + 6\pi \eta a v

    Rearrange to solve for vv:

    6πηav=ρ(43πa3)g−σ(43πa3)g6\pi \eta a v = \rho \left(\frac{4}{3}\pi a^3\right) g - \sigma \left(\frac{4}{3}\pi a^3\right) g 6πηav=(43πa3)g(ρ−σ)6\pi \eta a v = \left(\frac{4}{3}\pi a^3\right) g (\rho - \sigma)

    Divide both sides by 6πηa6\pi \eta a:

    v=(43πa3)g(ρ−σ)6πηav = \frac{\left(\frac{4}{3}\pi a^3\right) g (\rho - \sigma)}{6\pi \eta a}

    Simplify the expression:

    v=4πa3g(ρ−σ)3×6πηav = \frac{4\pi a^3 g (\rho - \sigma)}{3 \times 6\pi \eta a} v=4πa3g(ρ−σ)18πηav = \frac{4\pi a^3 g (\rho - \sigma)}{18\pi \eta a}

    Cancel π\pi and one aa:

    v=4a2g(ρ−σ)18ηv = \frac{4 a^2 g (\rho - \sigma)}{18 \eta}

    Reduce the fraction 418\frac{4}{18} to 29\frac{2}{9}:

    v=2a2(ρ−σ)g9η\boxed{v = \frac{2a^2(\rho - \sigma)g}{9\eta}}

    Question 13. b. (i): Conditions for liquid to be ideal

    Two conditions for a liquid to be considered ideal are:

    1. It is incompressible: Its density remains constant regardless of pressure changes.
    2. It is non-viscous: It has no internal friction, meaning its coefficient of viscosity is zero.

    Question 13. b. (ii): Kinetic and potential energies per unit volume

  9. Define density.

    The density of the liquid is ρ=mV\rho = \frac{m}{V}.

  10. Derive the expression for kinetic energy per unit volume.

    The kinetic energy (KEKE) of a liquid of mass mm and velocity vv is:

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

    To find the kinetic energy per unit volume, divide by the volume VV:

    KEV=12mv2V\frac{KE}{V} = \frac{\frac{1}{2}mv^2}{V}

    Substitute m=ρVm = \rho V:

    KEV=12(ρV)v2V\frac{KE}{V} = \frac{\frac{1}{2}(\rho V)v^2}{V} KEV=12ρv2\boxed{\frac{KE}{V} = \frac{1}{2}\rho v^2}
  11. Derive the expression for potential energy per unit volume.

    The potential energy (PEPE) of a liquid of mass mm at a height hh is:

    PE=mghPE = mgh

    To find the potential energy per unit volume, divide by the volume VV:

    PEV=mghV\frac{PE}{V} = \frac{mgh}{V}

    Substitute m=ρVm = \rho V:

    PEV=(ρV)ghV\frac{PE}{V} = \frac{(\rho V)gh}{V} PEV=ρgh\boxed{\frac{PE}{V} = \rho gh}

    Question 14. a. (i): State the zeroth and first laws of thermodynamics

    • Zeroth Law of Thermodynamics: If two thermodynamic systems are each in thermal equilibrium with a third system, then they are in thermal equilibrium with each other. This law establishes the concept of temperature.

    • First Law of Thermodynamics: The change in the internal energy (ΔU\Delta U) of a system is equal to the heat added to the system (QQ) minus the work done by the system (WW). It is a statement of the conservation of energy.

      ΔU=Q−W\Delta U = Q - W
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