Mathematics - IB Physics

  1. An electron is initially at rest in a uniform electric field of strength E=1.5×103 N C−1E = 1.5 \times 10^3 \text{ N C}^{-1}. What is the speed of the electron after it has travelled a distance of 5.0 cm5.0 \text{ cm} in the field?
    Answer: 5.1×106 m s−15.1 \times 10^6 \text{ m s}^{-1} The work done by the electric field on the electron provides it with kinetic energy. Work done W=Fd=(qE)dW = Fd = (qE)d. The kinetic energy gained is Ek=12mv2E_k = \frac{1}{2}mv^2. Setting W=EkW = E_k gives qEd=12mv2qEd = \frac{1}{2}mv^2. Rearranging for vv: v=2qEdmv = \sqrt{\frac{2qEd}{m}}. Using values for an electron (q=eq=e, m=mem=m_e) from the data booklet: v=2(1.60×10−19)(1.5×103)(0.050)9.11×10−31=2.4×10−179.11×10−31≈5.1×106 m s−1v = \sqrt{\frac{2(1.60 \times 10^{-19})(1.5 \times 10^3)(0.050)}{9.11 \times 10^{-31}}} = \sqrt{\frac{2.4 \times 10^{-17}}{9.11 \times 10^{-31}}} \approx 5.1 \times 10^6 \text{ m s}^{-1}.
  2. Car A starts from rest and accelerates uniformly at 3.0 m s−23.0 \text{ m s}^{-2}. At the same instant, Car B, which is 100 m ahead of Car A, is moving in the same direction at a constant velocity of 5.0 m s−15.0 \text{ m s}^{-1}. At what time does Car A overtake Car B?
    Answer: 10 s Let the starting position of Car A be s=0s=0. The position of Car A at time tt is sA=ut+12at2=0+12(3.0)t2=1.5t2s_A = ut + \frac{1}{2}at^2 = 0 + \frac{1}{2}(3.0)t^2 = 1.5t^2. The initial position of Car B is s=100s=100 m. Its position at time tt is sB=s0+vt=100+5.0ts_B = s_0 + vt = 100 + 5.0t. Car A overtakes Car B when sA=sBs_A = s_B. So, 1.5t2=100+5.0t1.5t^2 = 100 + 5.0t. This gives the quadratic equation 1.5t2−5.0t−100=01.5t^2 - 5.0t - 100 = 0. Using the quadratic formula, t=−(−5.0)±(−5.0)2−4(1.5)(−100)2(1.5)=5±25+6003=5±6253=5±253t = \frac{-(-5.0) \pm \sqrt{(-5.0)^2 - 4(1.5)(-100)}}{2(1.5)} = \frac{5 \pm \sqrt{25 + 600}}{3} = \frac{5 \pm \sqrt{625}}{3} = \frac{5 \pm 25}{3}. Since time must be positive, t=303=10 st = \frac{30}{3} = 10 \text{ s}.
  3. A 60 W incandescent light bulb is about 5% efficient at producing visible light. Estimate the order of magnitude for the number of visible-light photons it emits per second. (Assume the average wavelength of visible light is 500 nm).
    Answer: 101910^{19} First, calculate the power of the visible light emitted: Pvis=60 W×0.05=3.0 WP_{vis} = 60 \text{ W} \times 0.05 = 3.0 \text{ W}. Next, calculate the energy of a single photon: Ephoton=hf=hc/λE_{photon} = hf = hc/\lambda. Using approximations: E≈(6.6×10−34)(3×108)500×10−9≈20×10−265×10−7=4×10−19 JE \approx \frac{(6.6 \times 10^{-34})(3 \times 10^8)}{500 \times 10^{-9}} \approx \frac{20 \times 10^{-26}}{5 \times 10^{-7}} = 4 \times 10^{-19} \text{ J}. The number of photons per second is N=Pvis/Ephoton=3.0/(4×10−19)=0.75×1019N = P_{vis} / E_{photon} = 3.0 / (4 \times 10^{-19}) = 0.75 \times 10^{19}. The order of magnitude is 101910^{19}.
  4. A student plots a graph to determine the acceleration due to gravity, gg, using the simple pendulum equation T=2πlgT = 2\pi\sqrt{\frac{l}{g}}. The graph produces a straight line that passes through the origin. Which of the following correctly identifies the quantities on the axes and the expression for the gradient of the graph?
    Answer: y-axis: T2T^2, x-axis: ll, gradient: 4π2g\frac{4\pi^2}{g} To obtain a linear relationship, the equation T=2πlgT = 2\pi\sqrt{\frac{l}{g}} should be rearranged into the form y=mx+cy = mx + c. Squaring both sides gives T2=4π2lgT^2 = 4\pi^2 \frac{l}{g}, which can be written as T2=(4π2g)lT^2 = \left(\frac{4\pi^2}{g}\right)l. If T2T^2 is plotted on the y-axis and ll is plotted on the x-axis, the graph will be a straight line through the origin with a gradient m=4π2gm = \frac{4\pi^2}{g}.
  5. What is the order of magnitude of the ratio of the electrostatic force to the gravitational force between two protons?
    Answer: 103610^{36} The ratio is FEFG=ke2/r2Gmp2/r2=ke2Gmp2\frac{F_E}{F_G} = \frac{k e^2 / r^2}{G m_p^2 / r^2} = \frac{k e^2}{G m_p^2}. Using approximate values from the data booklet: k≈9×109k \approx 9 \times 10^9, e≈1.6×10−19e \approx 1.6 \times 10^{-19}, G≈6.7×10−11G \approx 6.7 \times 10^{-11}, mp≈1.7×10−27m_p \approx 1.7 \times 10^{-27}. The ratio is approximately (9×109)(1.6×10−19)2(6.7×10−11)(1.7×10−27)2≈1010⋅(10−19)210−10⋅(10−27)2=10−2810−64=1036\frac{(9 \times 10^9)(1.6 \times 10^{-19})^2}{(6.7 \times 10^{-11})(1.7 \times 10^{-27})^2} \approx \frac{10^{10} \cdot (10^{-19})^2}{10^{-10} \cdot (10^{-27})^2} = \frac{10^{-28}}{10^{-64}} = 10^{36}. This shows the immense relative strength of the electrostatic force.
  6. The unit of pressure, the pascal (Pa), can be expressed in terms of the fundamental SI units for mass (kg), length (m), and time (s). Which of the following is the correct expression for the pascal?
    Answer: kg m−1s−2\text{kg m}^{-1} \text{s}^{-2} Pressure is defined as force per unit area (P=F/AP = F/A). The SI unit of force is the newton (N) and the unit of area is square meters (m2\text{m}^2), so 1 Pa=1 N m−21 \text{ Pa} = 1 \text{ N m}^{-2}. Force is defined by Newton's second law (F=maF=ma), so 1 N=1 kg⋅m s−21 \text{ N} = 1 \text{ kg} \cdot \text{m s}^{-2}. Substituting this into the expression for the pascal gives 1 Pa=(1 kg m s−2)m−2=1 kg m−1s−21 \text{ Pa} = (1 \text{ kg m s}^{-2}) \text{m}^{-2} = 1 \text{ kg m}^{-1} \text{s}^{-2}.
  7. A beam of light enters a block of glass with a refractive index of 1.50 from air (refractive index ≈ 1.00). The angle of incidence is 60∘60^\circ. What is the angle of refraction inside the glass?
    Answer: 35∘35^\circ According to Snell's Law, n1sin⁡θ1=n2sin⁡θ2n_1 \sin{\theta_1} = n_2 \sin{\theta_2}. Here, n1=1.00n_1 = 1.00 (air), θ1=60∘\theta_1 = 60^\circ, and n2=1.50n_2 = 1.50 (glass). We need to find θ2\theta_2. 1.00×sin⁡(60∘)=1.50×sin⁡θ21.00 \times \sin(60^\circ) = 1.50 \times \sin{\theta_2}. sin⁡θ2=sin⁡(60∘)1.50=0.8661.50≈0.577\sin{\theta_2} = \frac{\sin(60^\circ)}{1.50} = \frac{0.866}{1.50} \approx 0.577. The angle of refraction is θ2=arcsin⁡(0.577)≈35.3∘\theta_2 = \arcsin(0.577) \approx 35.3^\circ. The closest answer is 35∘35^\circ.
  8. In an experiment to determine the resistivity ρ\rho of a wire, the resistance RR of different lengths LL of the wire is measured. The wire has a uniform cross-sectional area AA. If a graph of RR is plotted on the y-axis against LL on the x-axis, what does the gradient of the resulting straight-line graph represent?
    Answer: ρ/A\rho/A The formula for resistance in terms of resistivity is R=ρLAR = \frac{\rho L}{A}. To analyse this relationship with a linear graph, we can write it as R=(ρA)LR = \left(\frac{\rho}{A}\right)L. This equation is in the form y=mx+cy = mx + c, where y=Ry=R, x=Lx=L, the y-intercept c=0c=0, and the gradient m=ρAm = \frac{\rho}{A}.
  9. Two long, parallel wires carry currents I1I_1 and I2I_2 and are separated by a distance rr. They experience a magnetic force per unit length ff. If the current in both wires is doubled and their separation distance is halved, what is the new force per unit length?
    Answer: 8f8f The force per unit length ff between two parallel wires is given by f=μ0I1I22πrf = \frac{\mu_0 I_1 I_2}{2\pi r}. This shows that ff is directly proportional to the product of the currents (I1I2I_1 I_2) and inversely proportional to the distance (rr). If both currents are doubled (I1→2I1,I2→2I2I_1 \rightarrow 2I_1, I_2 \rightarrow 2I_2) and the distance is halved (r→r/2r \rightarrow r/2), the new force fnewf_{new} will be proportional to (2I1)(2I2)(r/2)=4I1I2r/2=8I1I2r\frac{(2I_1)(2I_2)}{(r/2)} = \frac{4 I_1 I_2}{r/2} = 8 \frac{I_1 I_2}{r}. Thus, the new force per unit length is 8f8f.
  10. A black body has a thermodynamic temperature TT and radiates power PP. If the thermodynamic temperature of the black body is doubled to 2T2T, what is the new power radiated?
    Answer: 16P16P According to the Stefan-Boltzmann law, the power PP radiated by a black body is proportional to the fourth power of its thermodynamic temperature TT (P∝T4P \propto T^4). If the temperature is doubled (T→2TT \rightarrow 2T), the new power PnewP_{new} will be proportional to (2T)4=24T4=16T4(2T)^4 = 2^4 T^4 = 16T^4. Therefore, the new power is 16 times the original power, so Pnew=16PP_{new} = 16P.
  11. Two point charges experience an electrostatic force FF. The distance between the charges is then tripled, and the magnitude of one of the charges is doubled. What is the new electrostatic force in terms of FF?
    Answer: 29F\frac{2}{9}F According to Coulomb's Law, the electrostatic force FF is proportional to the product of the charges (q1q2q_1q_2) and inversely proportional to the square of the distance (r2r^2) between them: F∝q1q2r2F \propto \frac{q_1q_2}{r^2}. If one charge is doubled (q1→2q1q_1 \rightarrow 2q_1) and the distance is tripled (r→3rr \rightarrow 3r), the new force FnewF_{new} will be proportional to (2q1)q2(3r)2=2q1q29r2=29q1q2r2\frac{(2q_1)q_2}{(3r)^2} = \frac{2q_1q_2}{9r^2} = \frac{2}{9} \frac{q_1q_2}{r^2}. Therefore, Fnew=29FF_{new} = \frac{2}{9}F.
  12. An experimenter plots data points with error bars on a graph to find a physical constant from the gradient. To determine the uncertainty in the gradient, two additional lines are drawn. Which statement best describes these two lines?
    Answer: A line of maximum possible slope and a line of minimum possible slope that pass through the error bars of all data points. The uncertainty in the gradient is found by considering the range of possible straight lines that can be reasonably drawn through the data, given the uncertainties represented by the error bars. This range is defined by the line of maximum possible slope (the 'steepest' line) and the line of minimum possible slope (the 'shallowest' line) that still pass through or touch the error bars of all data points. The uncertainty in the gradient is typically taken as half the difference between these maximum and minimum gradients.
  13. A block of weight W=mgW = mg is placed on a frictionless plane inclined at an angle θ\theta to the horizontal. What is the magnitude of the component of the block's weight that acts parallel to the surface of the plane?
    Answer: mgsin⁡θmg \sin{\theta} The weight mgmg acts vertically downwards. This vector can be resolved into two components: one perpendicular to the inclined plane and one parallel to it. Using trigonometry, the component of weight parallel to the plane is mgsin⁡θmg \sin{\theta}, and the component perpendicular to the plane is mgcos⁡θmg \cos{\theta}. The parallel component is the one that would cause the block to accelerate down the plane.
  14. A radioactive sample has a half-life of T1/2T_{1/2}. What is the time required for the activity of the sample to decrease to 110\frac{1}{10} of its initial value?
    Answer: T1/2ln⁡(10)ln⁡(2)T_{1/2} \frac{\ln(10)}{\ln(2)} The activity AA follows the decay law A=A0e−λtA = A_0 e^{-\lambda t}, where λ\lambda is the decay constant. We are given A/A0=1/10A/A_0 = 1/10. So, 1/10=e−λt1/10 = e^{-\lambda t}. Taking the natural logarithm of both sides gives ln⁡(1/10)=−λt\ln(1/10) = -\lambda t, which simplifies to t=ln⁡(10)λt = \frac{\ln(10)}{\lambda}. The decay constant is related to the half-life by λ=ln⁡(2)T1/2\lambda = \frac{\ln(2)}{T_{1/2}}. Substituting for λ\lambda gives t=ln⁡(10)ln⁡(2)/T1/2=T1/2ln⁡(10)ln⁡(2)t = \frac{\ln(10)}{\ln(2)/T_{1/2}} = T_{1/2} \frac{\ln(10)}{\ln(2)}.
  15. A graph shows the variation of the resultant force FF acting on an object as a function of time tt. What physical quantity is represented by the area under the force-time graph?
    Answer: The change in momentum of the object. By definition, impulse is the product of the average force and the time interval over which it acts (J=FΔtJ = F \Delta t). For a variable force, the impulse is the integral of the force with respect to time, which corresponds to the area under the force-time graph. The impulse-momentum theorem states that the impulse on an object is equal to the change in its momentum (J=ΔpJ = \Delta p).
  16. A swimmer can swim at a speed of 1.5 m s−11.5 \text{ m s}^{-1} in still water. She swims across a river that has a current of 2.0 m s−12.0 \text{ m s}^{-1} flowing at a right angle to her intended direction of travel. What is the magnitude of her resultant velocity relative to the river bank?
    Answer: 2.5 m s−12.5 \text{ m s}^{-1} The swimmer's velocity relative to the water and the velocity of the water current are perpendicular vectors. The resultant velocity is the vector sum of these two velocities. The magnitude of the resultant velocity can be found using the Pythagorean theorem: vresultant=vswimmer2+vcurrent2=(1.5)2+(2.0)2=2.25+4.00=6.25=2.5 m s−1v_{resultant} = \sqrt{v_{swimmer}^2 + v_{current}^2} = \sqrt{(1.5)^2 + (2.0)^2} = \sqrt{2.25 + 4.00} = \sqrt{6.25} = 2.5 \text{ m s}^{-1}.
  17. A satellite of mass mm orbits a planet of mass MM in a stable circular orbit of radius rr with an orbital period TT. Which expression correctly gives the mass of the planet MM? (GG is the gravitational constant.)
    Answer: M=4π2r3GT2M = \frac{4\pi^2 r^3}{GT^2} For a circular orbit, the gravitational force provides the centripetal force. So, Fg=Fc⇒GMmr2=mv2rF_g = F_c \Rightarrow \frac{GMm}{r^2} = \frac{mv^2}{r}. The orbital speed is v=2πrTv = \frac{2\pi r}{T}. Substituting for vv: GMmr2=mr(2πrT)2=mr4π2r2T2\frac{GMm}{r^2} = \frac{m}{r} \left(\frac{2\pi r}{T}\right)^2 = \frac{m}{r} \frac{4\pi^2 r^2}{T^2}. Simplifying gives GMr2=4π2rT2\frac{GM}{r^2} = \frac{4\pi^2 r}{T^2}. Rearranging for MM gives Kepler's third law in this form: M=4π2r3GT2M = \frac{4\pi^2 r^3}{GT^2}.

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