Exponential DE Models - Calculus 1

  1. Carbon-14 decays according to the equation dydt=−0.00012y\frac{dy}{dt} = -0.00012 y, where tt is in years. A sample of a fossil is found to contain 25% of its original carbon-14. Which expression represents the age of the fossil in years?
    Answer: ln⁡(4)0.00012\frac{\ln(4)}{0.00012} When you encounter exponential decay problems, you're dealing with differential equations where the rate of change is proportional to the current amount. The equation dydt=−0.00012y\frac{dy}{dt} = -0.00012y tells us that carbon-14 decreases at a rate proportional to how much is present. To solve this separable differential equation, separate variables: dyy=−0.00012 dt\frac{dy}{y} = -0.00012 \, dt. Integrating both sides gives ln⁡∣y∣=−0.00012t+C\ln|y| = -0.00012t + C. Using the initial condition that at t=0t = 0, y=y0y = y_0 (the original amount), we find C=ln⁡(y0)C = \ln(y_0). Therefore: y=y0e−0.00012ty = y_0 e^{-0.00012t}. Since the fossil contains 25% of its original carbon-14, we have 0.25y0=y0e−0.00012t0.25y_0 = y_0 e^{-0.00012t}. Dividing by y0y_0 gives 0.25=e−0.00012t0.25 = e^{-0.00012t}. Taking the natural logarithm: ln⁡(0.25)=−0.00012t\ln(0.25) = -0.00012t, so t=ln⁡(0.25)−0.00012t = \frac{\ln(0.25)}{-0.00012}. Since ln⁡(0.25)=ln⁡(14)=−ln⁡(4)\ln(0.25) = \ln(\frac{1}{4}) = -\ln(4), we get t=−ln⁡(4)−0.00012=ln⁡(4)0.00012t = \frac{-\ln(4)}{-0.00012} = \frac{\ln(4)}{0.00012}. This matches choice B. Choice A has the wrong sign—it would give a negative age. Choice C omits the logarithm entirely, treating this like a linear rather than exponential relationship. Choice D uses the half-life formula incorrectly, multiplying 4 by carbon-14's half-life without proper logarithmic adjustment. Study tip: In exponential decay problems, always set up the ratio equation first, then use natural logarithms to solve for time. Watch for sign errors when rearranging.
  2. Let y1(t)y_1(t) be the solution to dydt=−0.5y\frac{dy}{dt} = -0.5y with y(0)=100y(0)=100, and let y2(t)y_2(t) be the solution to dydt=−0.2y\frac{dy}{dt} = -0.2y with y(0)=100y(0)=100. For t>0t>0, let D(t)=y2(t)−y1(t)D(t) = y_2(t) - y_1(t). At what time tt does D(t)D(t) reach its maximum value?
    Answer: 103ln⁡(52)\frac{10}{3} \ln(\frac{5}{2}) When you encounter differential equations of the form dydt=−ky\frac{dy}{dt} = -ky, you're dealing with exponential decay. These have solutions of the form y(t)=y0e−kty(t) = y_0 e^{-kt} where y0y_0 is the initial value. For this problem, you need to find the solutions first. Since both equations have y(0)=100y(0) = 100: - y1(t)=100e−0.5ty_1(t) = 100e^{-0.5t} - y2(t)=100e−0.2ty_2(t) = 100e^{-0.2t} Therefore: D(t)=y2(t)−y1(t)=100e−0.2t−100e−0.5t=100(e−0.2t−e−0.5t)D(t) = y_2(t) - y_1(t) = 100e^{-0.2t} - 100e^{-0.5t} = 100(e^{-0.2t} - e^{-0.5t}) To find the maximum, set D′(t)=0D'(t) = 0: D′(t)=100(−0.2e−0.2t+0.5e−0.5t)=0D'(t) = 100(-0.2e^{-0.2t} + 0.5e^{-0.5t}) = 0 This gives us: 0.5e−0.5t=0.2e−0.2t0.5e^{-0.5t} = 0.2e^{-0.2t} Dividing both sides by 0.2e−0.5t0.2e^{-0.5t}: 0.50.2=e−0.2t+0.5t=e0.3t\frac{0.5}{0.2} = e^{-0.2t + 0.5t} = e^{0.3t} So 2.5=e0.3t2.5 = e^{0.3t}, which means ln⁡(2.5)=0.3t\ln(2.5) = 0.3t Therefore: t=ln⁡(2.5)0.3=ln⁡(5/2)3/10=103ln⁡(52)t = \frac{\ln(2.5)}{0.3} = \frac{\ln(5/2)}{3/10} = \frac{10}{3}\ln\left(\frac{5}{2}\right) Answer choice A uses 107\frac{10}{7} instead of 103\frac{10}{3} in the denominator—a calculation error. Choice B suggests the maximum occurs at t=0t = 0, but D(0)=0D(0) = 0, which is clearly not the maximum since D(t)>0D(t) > 0 for small positive tt. Choice D incorrectly assumes no maximum exists, but since both exponentials decay to zero, D(t)D(t) must have a maximum. Study tip: For difference functions involving exponential decay, always check the derivative and remember that different decay rates will create a maximum at some finite time.
  3. The rate of change of a quantity yy is directly proportional to yy. If yy decreases by 20% in 4 years, what is the constant of proportionality kk?
    Answer: ln⁡(0.8)4\frac{\ln(0.8)}{4} The model is y(t)=y0ekty(t) = y_0 e^{kt}. A decrease of 20% means that the value at t=4t=4 is 80% of the initial value. So, y(4)=0.8y0y(4) = 0.8 y_0. Substituting this into the model equation gives 0.8y0=y0ek⋅40.8 y_0 = y_0 e^{k \cdot 4}. Dividing by y0y_0 gives 0.8=e4k0.8 = e^{4k}. To solve for kk, we take the natural logarithm of both sides: ln⁡(0.8)=4k\ln(0.8) = 4k. Therefore, k=ln⁡(0.8)4k = \frac{\ln(0.8)}{4}.
  4. The value of an investment, V(t)V(t), grows according to dVdt=kV\frac{dV}{dt} = kV. The investment triples in 15 years. What is the instantaneous rate of growth of the investment, in dollars per year, at the exact moment its value is $9000?
    Answer: 600ln⁡(3)600 \ln(3) First, find the constant kk. We are given that the investment triples in 15 years. So, 3V0=V0ek⋅153V_0 = V_0 e^{k \cdot 15}, which implies 3=e15k3 = e^{15k}. Taking the natural logarithm gives ln⁡(3)=15k\ln(3) = 15k, so k=ln⁡(3)15k = \frac{\ln(3)}{15}. The instantaneous rate of growth is given by dVdt=kV\frac{dV}{dt} = kV. We want to find this rate when V=9000V = 9000. Substituting the values of kk and VV gives dVdt=(ln⁡(3)15)(9000)=600ln⁡(3)\frac{dV}{dt} = \left(\frac{\ln(3)}{15}\right) (9000) = 600 \ln(3). The initial value of the investment is not needed to solve the problem.
  5. The rate of growth of a cell culture is proportional to its size. Initially, the culture contains 200 cells, and after 3 hours, it contains 500 cells. How many cells are in the culture after 6 hours?
    Answer: 1250 Let P(t)P(t) be the number of cells. The model is P(t)=P0ektP(t) = P_0 e^{kt}. We have P0=200P_0 = 200. So, P(t)=200ektP(t) = 200 e^{kt}. We are given P(3)=500P(3) = 500, so 500=200e3k500 = 200 e^{3k}, which means e3k=500/200=2.5e^{3k} = 500/200 = 2.5. We want to find P(6)P(6). P(6)=200e6k=200(e3k)2P(6) = 200 e^{6k} = 200 (e^{3k})^2. Substituting the value of e3ke^{3k}, we get P(6)=200(2.5)2=200(6.25)=1250P(6) = 200 (2.5)^2 = 200 (6.25) = 1250.
  6. The population of a bacterial colony, PP, grows according to the differential equation dPdt=kP\frac{dP}{dt} = kP. The initial population doubles in 3 hours. At what time, in hours, will the population be 10 times its initial size?
    Answer: 3ln⁡(10)ln⁡(2)\frac{3 \ln(10)}{\ln(2)} The solution is P(t)=P0ektP(t) = P_0 e^{kt}. The doubling time is 3 hours, so 2P0=P0ek⋅32P_0 = P_0 e^{k \cdot 3}, which simplifies to 2=e3k2 = e^{3k}. Taking the natural logarithm gives ln⁡(2)=3k\ln(2) = 3k, so k=ln⁡(2)3k = \frac{\ln(2)}{3}. We want to find the time tt when P(t)=10P0P(t) = 10P_0. So, 10P0=P0ekt10P_0 = P_0 e^{kt}, which means 10=ekt10 = e^{kt}. Taking the natural logarithm gives ln⁡(10)=kt\ln(10) = kt. Substituting the value of kk, we get ln⁡(10)=(ln⁡(2)3)t\ln(10) = \left(\frac{\ln(2)}{3}\right)t. Solving for tt gives t=3ln⁡(10)ln⁡(2)t = \frac{3 \ln(10)}{\ln(2)}.
  7. The population of a species is governed by dP/dt=kPdP/dt = kP. The time it takes for the population to grow from 100 to 200 is TT. How long does it take for the population to grow from 200 to 800?
    Answer: 2T2T When you encounter a differential equation like dPdt=kP\frac{dP}{dt} = kP, you're dealing with exponential growth. This equation tells you that the rate of population change is proportional to the current population, which produces the classic exponential pattern where populations double, triple, etc. in consistent time intervals. To solve this, start with the general solution: P(t)=P0ektP(t) = P_0 e^{kt}, where P0P_0 is the initial population. Since the population grows from 100 to 200 in time TT, you can write: 200=100ekT200 = 100e^{kT}, which simplifies to 2=ekT2 = e^{kT}. Now for the key insight: you want to find how long it takes to go from 200 to 800. Notice that 800=200×4=200×22800 = 200 \times 4 = 200 \times 2^2. Since the population doubles every TT time units (from 2=ekT2 = e^{kT}), going from 200 to 800 requires exactly 2 doublings: 200 → 400 → 800. Therefore, this takes 2T2T. Choice A (6T6T) would represent 6 doublings, reaching 200×26=12,800200 \times 2^6 = 12,800. Choice B (3T3T) represents 3 doublings, reaching 200×23=1,600200 \times 2^3 = 1,600. Choice C (4T4T) represents 4 doublings, reaching 200×24=3,200200 \times 2^4 = 3,200. All of these overshoot the target of 800. Study tip: In exponential growth problems, always identify the "doubling time" first. Then count how many doublings you need to reach your target. This approach is much faster than working with the exponential formula directly.
  8. A population P(t)P(t) grows according to dPdt=kP\frac{dP}{dt} = kP. At time t=Tt=T, the population has doubled from its initial value. What was the average population over the time interval [0,T][0, T]?
    Answer: P0ln⁡(2)\frac{P_0}{\ln(2)} This question combines exponential growth with the concept of average value of a function. When you see the differential equation dPdt=kP\frac{dP}{dt} = kP, you're dealing with exponential growth where the solution is P(t)=P0ektP(t) = P_0 e^{kt}. Since the population doubles at time t=Tt = T, we have P(T)=2P0=P0ekTP(T) = 2P_0 = P_0 e^{kT}. This means ekT=2e^{kT} = 2, so kT=ln⁡(2)kT = \ln(2). To find the average population over [0,T][0, T], you need the average value formula: Average=1T−0∫0TP(t) dt=1T∫0TP0ekt dt\text{Average} = \frac{1}{T-0}\int_0^T P(t)\,dt = \frac{1}{T}\int_0^T P_0 e^{kt}\,dt. Evaluating this integral: P0T∫0Tekt dt=P0T⋅1k[ekt]0T=P0kT(ekT−1)\frac{P_0}{T}\int_0^T e^{kt}\,dt = \frac{P_0}{T} \cdot \frac{1}{k}[e^{kt}]_0^T = \frac{P_0}{kT}(e^{kT} - 1). Since kT=ln⁡(2)kT = \ln(2) and ekT=2e^{kT} = 2, we get: P0ln⁡(2)(2−1)=P0ln⁡(2)\frac{P_0}{\ln(2)}(2 - 1) = \frac{P_0}{\ln(2)}. Choice A) P0ln⁡(2)P_0 \ln(2) incorrectly multiplies by ln⁡(2)\ln(2) instead of dividing by it. Choice B) 3P02\frac{3P_0}{2} might come from incorrectly averaging the initial and final populations: P0+2P02\frac{P_0 + 2P_0}{2}, but this only works for linear functions. Choice D) P0P_0 ignores the growth entirely. Remember: for exponential functions, the average value isn't simply the arithmetic mean of endpoints. Always use the integral formula for average value, and be careful with your algebra when substituting known relationships.
  9. Let f(t)f(t) be a solution to y′=kyy' = ky with k>0k>0. The line tangent to the graph of y=f(t)y=f(t) at t=at=a passes through the origin. Which of the following must be true?
    Answer: ka=1ka = 1 This problem combines differential equations with tangent line geometry. When you see a differential equation like y′=kyy' = ky paired with geometric conditions, you need to find the general solution first, then apply the constraint. The differential equation y′=kyy' = ky has the general solution f(t)=Cektf(t) = Ce^{kt} for some constant CC. At point (a,f(a))(a, f(a)), the slope of the tangent line is f′(a)=kf(a)=kCekaf'(a) = kf(a) = kCe^{ka}. Since this tangent line passes through both the point (a,f(a))(a, f(a)) and the origin (0,0)(0,0), you can find its slope using the slope formula: slope=f(a)−0a−0=Cekaa\text{slope} = \frac{f(a) - 0}{a - 0} = \frac{Ce^{ka}}{a}. Setting the two expressions for slope equal: kCeka=CekaakCe^{ka} = \frac{Ce^{ka}}{a}. Assuming Ceka≠0Ce^{ka} \neq 0 (which must be true since the tangent line has a well-defined slope), you can divide both sides by CekaCe^{ka} to get k=1ak = \frac{1}{a}, which means ka=1ka = 1. Looking at the wrong answers: (A) a=ka = k would only be true if k=1k = 1, but kk can be any positive value. (C) f(a)=kf(a) = k has no necessary relationship to our geometric constraint. (D) a=0a = 0 would make the tangent line undefined since we'd have a vertical line through the origin. Study tip: When tangent lines pass through special points like the origin, always set up two expressions for the slope—one using the derivative and one using the point-slope relationship—then solve the resulting equation.
  10. The relationship between the atmospheric pressure PP and the altitude hh is modeled by the differential equation dPdh=−kP\frac{dP}{dh} = -kP, where kk is a positive constant. If the pressure at sea level (h=0h=0) is P0P_0 and the pressure at altitude HH is 0.5P00.5 P_0, what is the pressure at altitude 3H3H?
    Answer: 0.125P00.125 P_0 When you encounter a differential equation like dPdh=−kP\frac{dP}{dh} = -kP, you're dealing with exponential decay. This separable equation tells us that pressure decreases at a rate proportional to the current pressure as altitude increases. To solve this, separate variables: dPP=−k dh\frac{dP}{P} = -k \, dh. Integrating both sides gives ln⁡P=−kh+C\ln P = -kh + C, so P=Ae−khP = Ae^{-kh} where AA is a constant. Using the initial condition P(0)=P0P(0) = P_0, we find A=P0A = P_0, giving us P(h)=P0e−khP(h) = P_0 e^{-kh}. Now here's the key insight: at altitude HH, we know P(H)=0.5P0P(H) = 0.5P_0. This means P0e−kH=0.5P0P_0 e^{-kH} = 0.5P_0, so e−kH=0.5e^{-kH} = 0.5. At altitude 3H3H: P(3H)=P0e−k(3H)=P0(e−kH)3=P0(0.5)3=0.125P0P(3H) = P_0 e^{-k(3H)} = P_0 (e^{-kH})^3 = P_0 (0.5)^3 = 0.125P_0. Answer A (0.25P00.25P_0) represents what you'd get if you mistakenly thought the relationship was linear rather than exponential. Answer C (P0e−3kHP_0 e^{-3kH}) is technically correct but unnecessarily complicated since we can determine the numerical value. Answer D is wrong because we can find the pressure without explicitly knowing kk - the given condition at altitude HH provides all the information we need. Study tip: In exponential decay problems, look for ways to use given conditions to eliminate unknown constants. The key is recognizing that (e−kH)3=(0.5)3(e^{-kH})^3 = (0.5)^3 when you know e−kH=0.5e^{-kH} = 0.5.
  11. The pressure PP of a gas in a container is decreasing at a rate proportional to the pressure itself. The initial pressure is P0P_0. The pressure is measured at t=1t=1 to be P1P_1 and at t=3t=3 to be P3P_3. Which of the following is an expression for P0P_0?
    Answer: P1P1/P3P_1 \sqrt{P_1/P_3} When you encounter a problem stating that a quantity decreases "at a rate proportional to itself," you're dealing with exponential decay. This translates to the differential equation dPdt=−kP\frac{dP}{dt} = -kP, where k is a positive constant. The solution to this equation is P(t)=P0e−ktP(t) = P_0 e^{-kt}, where P0P_0 is the initial pressure at t = 0. Using the given data points, we have: - At t = 1: P1=P0e−kP_1 = P_0 e^{-k} - At t = 3: P3=P0e−3kP_3 = P_0 e^{-3k} To find P0P_0, first solve for k using the ratio P3P1=P0e−3kP0e−k=e−2k\frac{P_3}{P_1} = \frac{P_0 e^{-3k}}{P_0 e^{-k}} = e^{-2k}. This gives us e−k=P3P1e^{-k} = \sqrt{\frac{P_3}{P_1}}. Substituting back into P1=P0e−kP_1 = P_0 e^{-k}: P0=P1e−k=P1P3/P1=P1P1P3P_0 = \frac{P_1}{e^{-k}} = \frac{P_1}{\sqrt{P_3/P_1}} = P_1 \sqrt{\frac{P_1}{P_3}} This confirms answer C is correct. Answer A, P1P3\sqrt{P_1 P_3}, would be the geometric mean but doesn't account for the time intervals properly. Answer B, 3P1−P32\frac{3P_1 - P_3}{2}, suggests linear decay rather than exponential. Answer D, P3+P1−P32P_3 + \frac{P_1 - P_3}{2}, is simply the arithmetic mean of the two measured values. Study tip: Whenever you see "rate proportional to the quantity itself," immediately think exponential growth or decay. Set up dydt=±ky\frac{dy}{dt} = \pm ky and use the given data points to work backwards to find unknown parameters.
  12. The concentration C(t)C(t) of a drug in the bloodstream decays exponentially according to dC/dt=kCdC/dt = kC. The initial concentration is C0C_0. After 2 hours, the concentration is C0e\frac{C_0}{e}. At what time tt is the instantaneous rate of decay, −dC/dt-dC/dt, equal to half of the initial rate of decay?
    Answer: 2ln⁡(2)2\ln(2) hours When you encounter exponential decay problems, you're dealing with differential equations where the rate of change is proportional to the current amount. Here, dCdt=kC\frac{dC}{dt} = kC tells us the concentration follows exponential decay. First, solve for the general solution: C(t)=C0ektC(t) = C_0 e^{kt}. Using the given condition that C(2)=C0eC(2) = \frac{C_0}{e}, we get C0e=C0e2k\frac{C_0}{e} = C_0 e^{2k}, which gives us e2k=1ee^{2k} = \frac{1}{e}, so k=−12k = -\frac{1}{2}. Therefore, C(t)=C0e−t/2C(t) = C_0 e^{-t/2}. The instantaneous rate of decay is −dCdt=−kC=12C0e−t/2-\frac{dC}{dt} = -kC = \frac{1}{2}C_0 e^{-t/2}. The initial rate of decay (at t=0t = 0) is 12C0\frac{1}{2}C_0. We need to find when the rate equals half of this initial rate: 12C0e−t/2=12⋅12C0=14C0\frac{1}{2}C_0 e^{-t/2} = \frac{1}{2} \cdot \frac{1}{2}C_0 = \frac{1}{4}C_0. Solving: e−t/2=12e^{-t/2} = \frac{1}{2}, so −t2=ln⁡(12)=−ln⁡(2)-\frac{t}{2} = \ln(\frac{1}{2}) = -\ln(2), giving us t=2ln⁡(2)t = 2\ln(2). Choice A (2e2e hours) confuses the exponential base with the natural logarithm. Choice B (4 hours) likely comes from doubling the given 2-hour timeframe without proper calculation. Choice C (ln⁡(2)\ln(2) hours) misses the factor of 2 that comes from our decay constant k=−12k = -\frac{1}{2}. Remember: in exponential decay problems, always establish your decay constant first using given conditions, then carefully set up equations for rates rather than concentrations when the question asks about rates of change.
  13. A quantity P(t)P(t) grows according to the differential equation dPdt=kP\frac{dP}{dt} = kP. If P(t)P(t) increases from AA to BB over a time interval of length T1T_1, and from BB to CC over a time interval of length T2T_2, where A,B,CA, B, C are positive constants, which of the following is equal to T1T2\frac{T_1}{T_2}?
    Answer: ln⁡(B)−ln⁡(A)ln⁡(C)−ln⁡(B)\frac{\ln(B) - \ln(A)}{\ln(C) - \ln(B)} When you encounter a differential equation of the form dPdt=kP\frac{dP}{dt} = kP, you're dealing with exponential growth. This equation has the solution P(t)=P0ektP(t) = P_0 e^{kt}, where P0P_0 is the initial value. To find the time intervals, you need to use the relationship between consecutive values. If PP grows from AA to BB in time T1T_1, then B=AekT1B = Ae^{kT_1}. Taking the natural logarithm: ln⁡(B)=ln⁡(A)+kT1\ln(B) = \ln(A) + kT_1, so T1=ln⁡(B)−ln⁡(A)kT_1 = \frac{\ln(B) - \ln(A)}{k}. Similarly, if PP grows from BB to CC in time T2T_2, then T2=ln⁡(C)−ln⁡(B)kT_2 = \frac{\ln(C) - \ln(B)}{k}. Therefore, T1T2=ln⁡(B)−ln⁡(A)ln⁡(C)−ln⁡(B)\frac{T_1}{T_2} = \frac{\ln(B) - \ln(A)}{\ln(C) - \ln(B)}, which is answer choice D. Let's examine why the other options are wrong: A) ln⁡(B−A)ln⁡(C−B)\frac{\ln(B-A)}{\ln(C-B)} incorrectly uses differences inside the logarithm rather than differences of logarithms. This would apply to additive growth, not exponential growth. B) B−AC−B\frac{B-A}{C-B} is the ratio of absolute changes, which would be correct for linear growth (dPdt=k\frac{dP}{dt} = k), but not exponential growth. C) ln⁡(B/A)C/B\frac{\ln(B/A)}{C/B} mixes logarithmic and linear ratios inappropriately, combining the correct numerator form with an incorrect denominator. Remember: for exponential growth problems, time intervals are proportional to differences of natural logarithms, not differences of the original values. Always solve the differential equation first to establish the exponential relationship.
  14. A quantity Q(t)Q(t) changes at a rate proportional to its current value. If Q(2)=20Q(2) = 20 and Q(5)=160Q(5) = 160, what is the instantaneous rate of change of QQ at t=2t=2?
    Answer: 20ln⁡(2)20 \ln(2) The model is dQdt=kQ\frac{dQ}{dt} = kQ, with solution Q(t)=Q0ektQ(t) = Q_0 e^{kt}. We have 20=Q0e2k20 = Q_0 e^{2k} and 160=Q0e5k160 = Q_0 e^{5k}. Dividing the second equation by the first gives 16020=e5ke2k\frac{160}{20} = \frac{e^{5k}}{e^{2k}}, which simplifies to 8=e3k8 = e^{3k}. Taking the natural logarithm, ln⁡(8)=3k\ln(8) = 3k, so 3ln⁡(2)=3k3\ln(2) = 3k, which means k=ln⁡(2)k = \ln(2). The question asks for the rate of change at t=2t=2, which is dQdt∣t=2\frac{dQ}{dt}|_{t=2}. Using the differential equation, dQdt∣t=2=k⋅Q(2)=ln⁡(2)⋅20=20ln⁡(2)\frac{dQ}{dt}|_{t=2} = k \cdot Q(2) = \ln(2) \cdot 20 = 20 \ln(2).
  15. A cup of coffee at 180∘180^{\circ}F is placed in a room with a constant temperature of 70∘70^{\circ}F. The coffee's temperature, T(t)T(t), is modeled by the differential equation dTdt=k(T−70)\frac{dT}{dt} = k(T - 70). If the coffee cools to 130∘130^{\circ}F in 10 minutes, which expression represents the temperature T(t)T(t) after tt minutes?
    Answer: T(t)=70+110(611)t/10T(t) = 70 + 110 (\frac{6}{11})^{t/10} The differential equation dTdt=k(T−70)\frac{dT}{dt} = k(T - 70) has the solution T(t)−70=(T0−70)ektT(t) - 70 = (T_0 - 70)e^{kt}, where T0T_0 is the initial temperature. With T(0)=180T(0)=180, this becomes T(t)=70+(180−70)ekt=70+110ektT(t) = 70 + (180 - 70)e^{kt} = 70 + 110e^{kt}. We use the point (10,130)(10, 130) to find kk: 130=70+110e10k130 = 70 + 110e^{10k}, which simplifies to 60=110e10k60 = 110e^{10k}, so 611=e10k\frac{6}{11} = e^{10k}. We can write ek=(611)1/10e^k = (\frac{6}{11})^{1/10}. Substituting this back into the solution gives T(t)=70+110(ek)t=70+110((611)1/10)t=70+110(611)t/10T(t) = 70 + 110(e^k)^t = 70 + 110 ((\frac{6}{11})^{1/10})^t = 70 + 110 (\frac{6}{11})^{t/10}.
  16. The rate of decay of a radioactive isotope is proportional to the amount present. If the half-life of the isotope is 100 years, what fraction of the original amount remains after 50 years?
    Answer: 12\frac{1}{\sqrt{2}} When you encounter radioactive decay problems, you're dealing with exponential decay where the rate of change is proportional to the current amount. This creates the differential equation dNdt=−kN\frac{dN}{dt} = -kN, which has the solution N(t)=N0e−ktN(t) = N_0 e^{-kt}, where N0N_0 is the initial amount. The key insight is using the half-life to find the decay constant. Since half the material remains after 100 years: 12=e−100k\frac{1}{2} = e^{-100k}. Taking the natural logarithm: k=ln⁡(2)100k = \frac{\ln(2)}{100}. Now you can find the amount remaining after 50 years: N(50)=N0e−k⋅50=N0e−ln⁡(2)100⋅50=N0e−ln⁡(2)2N(50) = N_0 e^{-k \cdot 50} = N_0 e^{-\frac{\ln(2)}{100} \cdot 50} = N_0 e^{-\frac{\ln(2)}{2}} Since e−ln⁡(2)2=(eln⁡(2))−1/2=2−1/2=12e^{-\frac{\ln(2)}{2}} = (e^{\ln(2)})^{-1/2} = 2^{-1/2} = \frac{1}{\sqrt{2}}, the fraction remaining is 12\frac{1}{\sqrt{2}}, making C correct. Looking at the wrong answers: A) 34\frac{3}{4} might tempt you if you incorrectly assume linear decay rather than exponential. B) 12\frac{1}{2} is the amount remaining at the half-life (100 years), not at 50 years. D) 14\frac{1}{4} would be correct at 200 years (two half-lives), not 50 years. Study tip: Remember that exponential decay means equal time periods correspond to equal fractional changes, not equal absolute changes. After one half-life you have 12\frac{1}{2}, after half a half-life you have 12\frac{1}{\sqrt{2}}, and the pattern continues exponentially.
  17. A bank account balance, BB, grows according to the differential equation dBdt=0.04B\frac{dB}{dt} = 0.04B, where tt is in years. An initial deposit of $100 is made at t=0t=0, and a second deposit of $100 is made at t=5t=5. What is the balance in the account at t=10t=10?
    Answer: 100e0.4+100e0.2100e^{0.4} + 100e^{0.2} We can model the growth of each deposit separately. The first $100 is invested for the full 10 years. Its value at t=10t=10 is 100e0.04⋅10=100e0.4100e^{0.04 \cdot 10} = 100e^{0.4}. The second $100 is deposited at t=5t=5 and is invested for 10−5=510-5=5 years. Its value at t=10t=10 is 100e0.04⋅5=100e0.2100e^{0.04 \cdot 5} = 100e^{0.2}. The total balance at t=10t=10 is the sum of the values of these two deposits, which is 100e0.4+100e0.2100e^{0.4} + 100e^{0.2}.
  18. A solution y=f(t)y=f(t) to y′=kyy'=ky satisfies f(1)=3f(1)=3 and f(2)=12f(2)=12. What is the value of f(0)f(0)?
    Answer: 3/43/4 When you encounter a differential equation of the form y′=kyy' = ky, you're dealing with exponential growth or decay. The general solution is always y=Cekty = Ce^{kt}, where CC and kk are constants determined by the given conditions. To find these constants, use your two data points: f(1)=3f(1) = 3 and f(2)=12f(2) = 12. Substituting into y=Cekty = Ce^{kt}: 3=Cek⋅1=Cek3 = Ce^{k \cdot 1} = Ce^k 12=Cek⋅2=Ce2k12 = Ce^{k \cdot 2} = Ce^{2k} Divide the second equation by the first to eliminate CC: 123=Ce2kCek=ek\frac{12}{3} = \frac{Ce^{2k}}{Ce^k} = e^k So ek=4e^k = 4, which means k=ln⁡(4)k = \ln(4). Now find CC using the first equation: 3=Cek=C⋅43 = Ce^k = C \cdot 4, so C=34C = \frac{3}{4}. Therefore, f(t)=34etln⁡(4)=34⋅4tf(t) = \frac{3}{4}e^{t\ln(4)} = \frac{3}{4} \cdot 4^t. At t=0t = 0: f(0)=34⋅40=34⋅1=34f(0) = \frac{3}{4} \cdot 4^0 = \frac{3}{4} \cdot 1 = \frac{3}{4}. The answer is B. Choice A (32\frac{3}{2}) likely comes from incorrectly assuming C=32C = \frac{3}{2} without properly using both conditions. Choice C (12\frac{1}{2}) might result from computational errors in finding CC. Choice D (−6-6) could stem from sign errors or completely misapplying the exponential formula. Study tip: For exponential differential equations, always use the ratio method to find kk first—it eliminates CC and simplifies your work. Then substitute back to find CC.
  19. A radioactive substance decays according to the differential equation dMdt=kM\frac{dM}{dt} = kM, where MM is the mass in grams and tt is the time in years. The mass of the substance is measured to be M1M_1 at time t1t_1 and M2M_2 at time t2=t1+Δtt_2 = t_1 + \Delta t. What is the half-life of the substance?
    Answer: Δtln⁡(2)ln⁡(M1)−ln⁡(M2)\frac{\Delta t \ln(2)}{\ln(M_1) - \ln(M_2)} The solution to the differential equation is M(t)=M0ektM(t) = M_0 e^{kt}. We have M1=M(t1)M_1 = M(t_1) and M2=M(t1+Δt)M_2 = M(t_1 + \Delta t). Dividing the two equations gives M2M1=M0ek(t1+Δt)M0ekt1=ekΔt\frac{M_2}{M_1} = \frac{M_0 e^{k(t_1 + \Delta t)}}{M_0 e^{kt_1}} = e^{k \Delta t}. Solving for kk yields k=1Δtln⁡(M2M1)k = \frac{1}{\Delta t}\ln(\frac{M_2}{M_1}). The half-life T1/2T_{1/2} is the time it takes for the substance to decay to half its amount, which is given by the formula T1/2=ln⁡(1/2)k=−ln⁡(2)kT_{1/2} = \frac{\ln(1/2)}{k} = \frac{-\ln(2)}{k}. Substituting our expression for kk, we get T1/2=−ln⁡(2)1Δtln⁡(M2/M1)=−Δtln⁡(2)ln⁡(M2)−ln⁡(M1)=Δtln⁡(2)ln⁡(M1)−ln⁡(M2)T_{1/2} = \frac{-\ln(2)}{\frac{1}{\Delta t}\ln(M_2/M_1)} = \frac{-\Delta t \ln(2)}{\ln(M_2) - \ln(M_1)} = \frac{\Delta t \ln(2)}{\ln(M_1) - \ln(M_2)}.
  20. Let y(t)y(t) be a solution to dydt=ky\frac{dy}{dt} = ky with k<0k<0 and y(0)>0y(0)>0. Let tht_h be the half-life. Which of the following statements is true about the time tqt_q it takes for the quantity to reduce to one-quarter of its original size?
    Answer: tq=2tht_q = 2t_h When you encounter differential equations of the form dydt=ky\frac{dy}{dt} = ky with k<0k < 0, you're dealing with exponential decay. The solution is y(t)=y(0)ekty(t) = y(0)e^{kt}, where y(0)y(0) is the initial value. The key insight is understanding the relationship between half-life and quarter-life. The half-life tht_h is when y(th)=12y(0)y(t_h) = \frac{1}{2}y(0). Setting up the equation: 12y(0)=y(0)ekth\frac{1}{2}y(0) = y(0)e^{kt_h}, which simplifies to 12=ekth\frac{1}{2} = e^{kt_h}. Taking the natural log: kth=ln⁡(1/2)=−ln⁡(2)kt_h = \ln(1/2) = -\ln(2), so th=−ln⁡(2)k=ln⁡(2)∣k∣t_h = \frac{-\ln(2)}{k} = \frac{\ln(2)}{|k|}. For the quarter-life tqt_q, we need y(tq)=14y(0)y(t_q) = \frac{1}{4}y(0). Notice that 14=12×12\frac{1}{4} = \frac{1}{2} \times \frac{1}{2}, meaning the quantity halves twice. Since each halving takes time tht_h, the total time is tq=2tht_q = 2t_h. This makes D correct. Let's examine why the other answers fail: A suggests tq=4tht_q = 4t_h, which would correspond to reducing to (12)4=116(\frac{1}{2})^4 = \frac{1}{16} of the original size. B proposes tq=(th)2t_q = (t_h)^2, which has no physical basis in exponential decay. C gives tq=th+ln⁡(2)/∣k∣t_q = t_h + \ln(2)/|k|, but since th=ln⁡(2)/∣k∣t_h = \ln(2)/|k|, this would equal 2th2t_h anyway—though the form suggests a misunderstanding of the additive nature of half-lives. Remember: in exponential decay, each additional half-life period halves the remaining quantity, so multiple reductions are additive in time.

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