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Exponentials and Logarithms -- Diagnostic Tests

flowchart TD
A[Diag Exponentials And Logarithms] --> B[Key Concepts]
A --> C[Core Principles]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
C --> F[Design patterns]
D --> G[Real-world usage]

Mathematics is the language of patterns and logic, a tool for describing relationships and solving problems.

Exponentials and Logarithms, Diagnostic Tests

Section titled “Exponentials and Logarithms, Diagnostic Tests”

Tests edge cases, boundary conditions, and common misconceptions for exponentials and logarithms.

UT-1: ln⁡(ab)=bln⁡a\ln(a^b) = b\ln a vs (ln⁡a)b(\ln a)^b Conflation

Section titled “UT-1: ln⁡(ab)=bln⁡a\ln(a^b) = b\ln aln(ab)=blna vs (ln⁡a)b(\ln a)^b(lna)b Conflation”

Question:

(a) Without using a calculator, determine which is larger: πe\pi^e or eπe^\pi.

(b) A student writes ln⁡(x2)=(ln⁡x)2\ln(x^2) = (\ln x)^2 and uses this to solve ln⁡(x2)=4\ln(x^2) = 4. Find the correct solution set and the (incorrect) solution set the student would obtain.

(c) Solve the equation 2x=x22^x = x^2 for real xx Giving exact answers where possible.

[Difficulty: hard. Tests the fundamental distinction between ln⁡(ab)=bln⁡a\ln(a^b) = b\ln a and (ln⁡a)b(\ln a)^b And requires analytical comparison of transcendental expressions.]

Solution:

(a) Consider f(x)=ln⁡xxf(x) = \frac{\ln x}{x}. Its derivative is:

f"(x)=1⋅x−ln⁡x⋅1x2=1−ln⁡xx2f"(x) = \frac{1 \cdot x - \ln x \cdot 1}{x^2} = \frac{1 - \ln x}{x^2}

f′(x)=0f'(x) = 0 when ln⁡x=1\ln x = 1 I.e. x=ex = e. For x<ex \lt e: f′(x)>0f'(x) \gt 0; for x>ex \gt e: f′(x)<0f'(x) \lt 0.

So f(x)f(x) has a global maximum at x=ex = e Meaning f(e)≥f(π)f(e) \geq f(\pi):

ln⁡ee≥ln⁡ππ  ⟹  1e≥ln⁡ππ  ⟹  π≥eln⁡π\frac{\ln e}{e} \geq \frac{\ln \pi}{\pi} \implies \frac{1}{e} \geq \frac{\ln \pi}{\pi} \implies \pi \geq e \ln \pi   ⟹  π≥ln⁡(πe)  ⟹  eπ≥πe\implies \pi \geq \ln(\pi^e) \implies e^\pi \geq \pi^e

Therefore eπe^\pi is larger.

(b) The correct identity is ln⁡(x2)=2ln⁡∣x∣\ln(x^2) = 2\ln\lvert x \rvert.

ln⁡(x2)=4  ⟹  2ln⁡∣x∣=4  ⟹  ln⁡∣x∣=2  ⟹  ∣x∣=e2  ⟹  x=±e2\ln(x^2) = 4 \implies 2\ln\lvert x \rvert = 4 \implies \ln\lvert x \rvert = 2 \implies \lvert x \rvert = e^2 \implies x = \pm e^2.

Correct solution set: {e2,−e2}\{e^2, -e^2\}.

The student’s incorrect equation (ln⁡x)2=4(\ln x)^2 = 4 gives ln⁡x=±2\ln x = \pm 2 So x=e2x = e^2 or x=e−2x = e^{-2}.

Student’s (incorrect) solution set: {e2,e−2}\{e^2, e^{-2}\}.

The student loses x=−e2x = -e^2 (because ln⁡x\ln x is undefined for x<0x \lt 0) and gains x=e−2x = e^{-2} (which is not a solution of the original equation since ln⁡(e−2)2=ln⁡(e−4)=−4≠4\ln(e^{-2})^2 = \ln(e^{-4}) = -4 \neq 4).

(c) By inspection, x=2x = 2 and x=4x = 4 are solutions: 22=4=222^2 = 4 = 2^2 and 24=16=422^4 = 16 = 4^2.

For x<0x \lt 0: 2x>02^x \gt 0 and x2>0x^2 \gt 0 So solutions may exist. At x=−0.7666...x = -0.7666...: 2−0.7666≈0.5872^{-0.7666} \approx 0.587 and (−0.7666)2≈0.588(-0.7666)^2 \approx 0.588. This is a solution, which we denote x=−W(−2ln⁡2)2ln⁡2x = -\frac{W(-2\ln 2)}{2\ln 2} where WW is the Lambert WW-function. For A-Level purposes, we note there are exactly three solutions: x≈−0.767x \approx -0.767, x=2x = 2 And x=4x = 4.

To show there are no other solutions for x≥0x \geq 0: consider g(x)=2x−x2g(x) = 2^x - x^2. We have g(0) = 1$$g(1) = 1$$g(2) = 0$$g(3) = -1$$g(4) = 0$$g(5) = 7. Since g′′(x)=2x(ln⁡2)2−2g''(x) = 2^x(\ln 2)^2 - 2 And 2x(ln⁡2)2>22^x(\ln 2)^2 \gt 2 for x>5x \gt 5 (because 25⋅(ln⁡2)2≈2.142^5 \cdot (\ln 2)^2 \approx 2.14), gg is convex for x≥5x \geq 5 and grows without bound. By Rolle’s theorem, there can be at most one root in (3,4)(3, 4) and at most one in (4,∞)(4, \infty). Since g(4)=0g(4) = 0 and gg is increasing at x=4x = 4 There are no further roots beyond x=4x = 4.


Question:

(a) Solve e2x−5ex+6=0e^{2x} - 5e^x + 6 = 0 Giving exact answers.

(b) Solve e2x−5ex+6=1e^{2x} - 5e^x + 6 = 1 for x∈Rx \in \mathbb{R} Giving exact answers.

(c) A student solving part (b) writes e2x−5ex+5=0e^{2x} - 5e^x + 5 = 0 Substitutes u=exu = e^x And gets u2−5u+5=0u^2 - 5u + 5 = 0. Find the values of uu And explain why the student must check that u>0u \gt 0 before taking natural logarithms.

[Difficulty: hard. Tests recognition of the hidden quadratic substitution and the positivity constraint on exe^x that eliminates spurious solutions.]

Solution:

(a) Let u=exu = e^x. Since ex>0e^x \gt 0 for all x∈Rx \in \mathbb{R} We require u>0u \gt 0.

u2−5u+6=0  ⟹  (u−2)(u−3)=0  ⟹  u=2 or u=3u^2 - 5u + 6 = 0 \implies (u-2)(u-3) = 0 \implies u = 2 \text{ or } u = 3

Both satisfy u>0u \gt 0.

ex=2  ⟹  x=ln⁡2e^x = 2 \implies x = \ln 2

ex=3  ⟹  x=ln⁡3e^x = 3 \implies x = \ln 3

Solutions: x=ln⁡2x = \ln 2 and x=ln⁡3x = \ln 3.

(b) e2x−5ex+6=1  ⟹  e2x−5ex+5=0e^{2x} - 5e^x + 6 = 1 \implies e^{2x} - 5e^x + 5 = 0.

Let u=exu = e^x (u>0u \gt 0):

u2−5u+5=0  ⟹  u=5±25−202=5±52u^2 - 5u + 5 = 0 \implies u = \frac{5 \pm \sqrt{25 - 20}}{2} = \frac{5 \pm \sqrt{5}}{2}

Both roots are positive: 5−52≈1.382>0\frac{5 - \sqrt{5}}{2} \approx 1.382 \gt 0 and 5+52≈3.618>0\frac{5 + \sqrt{5}}{2} \approx 3.618 \gt 0.

x=ln⁡ ⁣(5+52)orx=ln⁡ ⁣(5−52)x = \ln\!\left(\frac{5 + \sqrt{5}}{2}\right) \quad \text{or} \quad x = \ln\!\left(\frac{5 - \sqrt{5}}{2}\right)

(c) The student obtains u=5±52u = \frac{5 \pm \sqrt{5}}{2} Both positive. The check is necessary because if a root were negative or zero, taking ln⁡u\ln u would be undefined. For example, if the equation were e2x−3ex−4=0e^{2x} - 3e^x - 4 = 0 Then u=−1u = -1 or u=4u = 4 And u=−1u = -1 would give ex=−1e^x = -1 Which has no real solution. This is a common trap: the substitution u=exu = e^x implicitly constrains u>0u \gt 0 And students who forget this constraint accept spurious solutions.


UT-3: Domain Difference Between ln⁡(x2)\ln(x^2) and 2ln⁡x2\ln x

Section titled “UT-3: Domain Difference Between ln⁡(x2)\ln(x^2)ln(x2) and 2ln⁡x2\ln x2lnx”

Question:

(a) State the domain of f(x)=ln⁡(x2)f(x) = \ln(x^2) and the domain of g(x)=2ln⁡xg(x) = 2\ln x.

(b) On the intersection of their domains, show that f(x)=g(x)f(x) = g(x).

(c) A student claims ff is an even function and gg is not. Verify this claim by finding f(−x)f(-x) and g(−x)g(-x).

(d) The function h(x)=ln⁡(x2+2x+1)h(x) = \ln(x^2 + 2x + 1) is defined for all x≠−1x \neq -1. Express h(x)h(x) in the form 2ln⁡(… )2\ln(\dots) and state the domain restriction that applies to this equivalent form.

[Difficulty: hard. Tests the critical domain difference between ln⁡(x2)\ln(x^2) and 2ln⁡x2\ln x And the consequences for function properties like evenness.]

Solution:

(a) f(x)=ln⁡(x2)f(x) = \ln(x^2): we need x2>0x^2 \gt 0 I.e. x≠0x \neq 0. Domain: R∖{0}\mathbb{R} \setminus \{0\}.

g(x)=2ln⁡xg(x) = 2\ln x: we need x>0x \gt 0. Domain: (0,∞)(0, \infty).

(b) On the intersection (0,∞)(0, \infty):

f(x)=ln⁡(x2)=2ln⁡x=g(x)f(x) = \ln(x^2) = 2\ln x = g(x)

By the logarithm power law ln⁡(ab)=bln⁡a\ln(a^b) = b\ln a Valid for a>0a \gt 0.

(c) f(−x)=ln⁡((−x)2)=ln⁡(x2)=f(x)f(-x) = \ln((-x)^2) = \ln(x^2) = f(x) for all x≠0x \neq 0. So ff is even.

g(−x)=2ln⁡(−x)g(-x) = 2\ln(-x): this is undefined for all −x≤0-x \leq 0 I.e. For all x≥0x \geq 0. Since g(−x)g(-x) is not even defined on the same domain as g(x)$$g is not an even function.

(d) h(x)=ln⁡(x2+2x+1)=ln⁡((x+1)2)h(x) = \ln(x^2 + 2x + 1) = \ln((x+1)^2).

Using the power law: h(x)=2ln⁡∣x+1∣h(x) = 2\ln\lvert x+1 \rvert.

The domain restriction: ∣x+1∣>0  ⟹  x+1≠0  ⟹  x≠−1\lvert x + 1 \rvert \gt 0 \implies x + 1 \neq 0 \implies x \neq -1 Which matches the original domain.

A student who writes h(x)=2ln⁡(x+1)h(x) = 2\ln(x+1) has restricted the domain to x>−1x \gt -1 Losing all values x<−1x \lt -1. The correct equivalent form uses the absolute value: h(x)=2ln⁡∣x+1∣h(x) = 2\ln\lvert x+1 \rvert.


Tests synthesis of exponentials and logarithms with other topics. Requires combining concepts from multiple units.

IT-1: Integrating eaxsin⁡(bx)e^{ax}\sin(bx) by Parts Twice (with Integration)

Section titled “IT-1: Integrating eaxsin⁡(bx)e^{ax}\sin(bx)eaxsin(bx) by Parts Twice (with Integration)”

Question:

(a) Find ∫e3xsin⁡(2x) dx\int e^{3x}\sin(2x)\, dx.

(b) Verify your answer by differentiation.

(c) Hence evaluate ∫0π2e3xsin⁡(2x) dx\int_0^{\frac{\pi}{2}} e^{3x}\sin(2x)\, dx Giving an exact answer.

[Difficulty: hard. Requires integration by parts applied twice, producing an equation that is solved for the original integral.]

Solution:

(a) Let I=∫e3xsin⁡(2x) dxI = \int e^{3x}\sin(2x)\, dx.

Use integration by parts twice. Set u = e^{3x}$$\frac{dv}{dx} = \sin(2x).

First application: du = 3e^{3x}\, dx$$v = -\frac{1}{2}\cos(2x).

I=−12e3xcos⁡(2x)+32∫e3xcos⁡(2x) dxI = -\frac{1}{2}e^{3x}\cos(2x) + \frac{3}{2}\int e^{3x}\cos(2x)\, dx

Second application on the remaining integral: u=e3xu = e^{3x}, dvdx=cos⁡(2x)\frac{dv}{dx} = \cos(2x).

du=3e3x dxdu = 3e^{3x}\, dx, v=12sin⁡(2x)v = \frac{1}{2}\sin(2x).

∫e3xcos⁡(2x) dx=12e3xsin⁡(2x)−32∫e3xsin⁡(2x) dx=12e3xsin⁡(2x)−32I\int e^{3x}\cos(2x)\, dx = \frac{1}{2}e^{3x}\sin(2x) - \frac{3}{2}\int e^{3x}\sin(2x)\, dx = \frac{1}{2}e^{3x}\sin(2x) - \frac{3}{2}I

Substituting back:

I=−12e3xcos⁡(2x)+32(12e3xsin⁡(2x)−32I)I = -\frac{1}{2}e^{3x}\cos(2x) + \frac{3}{2}\left(\frac{1}{2}e^{3x}\sin(2x) - \frac{3}{2}I\right) I=−12e3xcos⁡(2x)+34e3xsin⁡(2x)−94II = -\frac{1}{2}e^{3x}\cos(2x) + \frac{3}{4}e^{3x}\sin(2x) - \frac{9}{4}I I+94I=e3x(−12cos⁡(2x)+34sin⁡(2x))I + \frac{9}{4}I = e^{3x}\left(-\frac{1}{2}\cos(2x) + \frac{3}{4}\sin(2x)\right) 134I=e3x4(−2cos⁡(2x)+3sin⁡(2x))\frac{13}{4}I = \frac{e^{3x}}{4}\left(-2\cos(2x) + 3\sin(2x)\right) I=e3x13(3sin⁡(2x)−2cos⁡(2x))+CI = \frac{e^{3x}}{13}\left(3\sin(2x) - 2\cos(2x)\right) + C

(b) Let F(x)=e3x13(3sin⁡(2x)−2cos⁡(2x))F(x) = \frac{e^{3x}}{13}(3\sin(2x) - 2\cos(2x)).

F′(x)=113[3e3x(3sin⁡(2x)−2cos⁡(2x))+e3x(6cos⁡(2x)+4sin⁡(2x))]F'(x) = \frac{1}{13}\left[3e^{3x}(3\sin(2x) - 2\cos(2x)) + e^{3x}(6\cos(2x) + 4\sin(2x))\right] =e3x13[9sin⁡(2x)−6cos⁡(2x)+6cos⁡(2x)+4sin⁡(2x)]= \frac{e^{3x}}{13}\left[9\sin(2x) - 6\cos(2x) + 6\cos(2x) + 4\sin(2x)\right] =e3x13⋅13sin⁡(2x)=e3xsin⁡(2x)= \frac{e^{3x}}{13} \cdot 13\sin(2x) = e^{3x}\sin(2x)

Confirmed.

(c) ∫0π2e3xsin⁡(2x) dx=[e3x13(3sin⁡(2x)−2cos⁡(2x))]0π2\int_0^{\frac{\pi}{2}} e^{3x}\sin(2x)\, dx = \left[\frac{e^{3x}}{13}(3\sin(2x) - 2\cos(2x))\right]_0^{\frac{\pi}{2}}

At x=π2x = \frac{\pi}{2}: e3π/2(3sin⁡π−2cos⁡π)=e3π/2(0+2)=2e3π/2e^{3\pi/2}(3\sin\pi - 2\cos\pi) = e^{3\pi/2}(0 + 2) = 2e^{3\pi/2}

At x=0x = 0: e0(3sin⁡0−2cos⁡0)=1(0−2)=−2e^0(3\sin 0 - 2\cos 0) = 1(0 - 2) = -2

=113(2e3π/2−(−2))=2(e3π/2+1)13= \frac{1}{13}(2e^{3\pi/2} - (-2)) = \frac{2(e^{3\pi/2} + 1)}{13}

IT-2: Gradient of a Logarithmic Function (with Differentiation)

Section titled “IT-2: Gradient of a Logarithmic Function (with Differentiation)”

Question:

(a) Find dydx\frac{dy}{dx} when y=ln⁡ ⁣(x2+1)y = \ln\!\left(\sqrt{x^2 + 1}\right) Simplifying your answer.

(b) Find the equation of the tangent to the curve y=ln⁡ ⁣(x2+1)y = \ln\!\left(\sqrt{x^2 + 1}\right) at the point where x=3x = \sqrt{3}.

(c) Show that the curve has no stationary points.

(d) A second curve is defined by y=e−xln⁡(x2+1)y = e^{-x}\ln(x^2 + 1). Find the value of xx at which this curve has a stationary point, giving your answer to 3 significant figures.

[Difficulty: hard. Combines the chain rule with logarithmic differentiation, and introduces a product rule with exponential decay.]

Solution:

(a) Using ln⁡ ⁣(x2+1)=12ln⁡(x2+1)\ln\!\left(\sqrt{x^2+1}\right) = \frac{1}{2}\ln(x^2+1) by the power law:

dydx=12⋅2xx2+1=xx2+1\frac{dy}{dx} = \frac{1}{2} \cdot \frac{2x}{x^2+1} = \frac{x}{x^2+1}

(b) At x=3x = \sqrt{3}: dydx=33+1=34\frac{dy}{dx} = \frac{\sqrt{3}}{3+1} = \frac{\sqrt{3}}{4}.

y=12ln⁡(3+1)=12ln⁡4=ln⁡2y = \frac{1}{2}\ln(3+1) = \frac{1}{2}\ln 4 = \ln 2.

Equation of tangent: y−ln⁡2=34(x−3)y - \ln 2 = \frac{\sqrt{3}}{4}(x - \sqrt{3}).

y=34x−34+ln⁡2y = \frac{\sqrt{3}}{4}x - \frac{3}{4} + \ln 2

(c) dydx=xx2+1=0  ⟹  x=0\frac{dy}{dx} = \frac{x}{x^2+1} = 0 \implies x = 0.

Wait: xx2+1=0\frac{x}{x^2+1} = 0 when x=0x = 0. Let me check: at x=0x = 0, dydx=0\frac{dy}{dx} = 0. So x=0x = 0 IS a stationary point.

The question says “show that the curve has no stationary points.” This is incorrect, the curve does have a stationary point at x=0x = 0. Let me re-examine.

At x=0x = 0: y=12ln⁡1=0y = \frac{1}{2}\ln 1 = 0. The gradient is 01=0\frac{0}{1} = 0. So x=0x = 0 is a stationary point. This is a minimum since d2ydx2=(x2+1)−x⋅2x(x2+1)2=1−x2(x2+1)2\frac{d^2y}{dx^2} = \frac{(x^2+1) - x \cdot 2x}{(x^2+1)^2} = \frac{1-x^2}{(x^2+1)^2} Which is positive at x=0x = 0.

The correct statement is that the curve has exactly one stationary point, a minimum at (0,0)(0, 0). The question as stated is incorrect.

(d) y=e−xln⁡(x2+1)y = e^{-x}\ln(x^2+1).

By the product rule:

dydx=−e−xln⁡(x2+1)+e−x⋅2xx2+1\frac{dy}{dx} = -e^{-x}\ln(x^2+1) + e^{-x} \cdot \frac{2x}{x^2+1} =e−x(2xx2+1−ln⁡(x2+1))= e^{-x}\left(\frac{2x}{x^2+1} - \ln(x^2+1)\right)

Since e−x>0e^{-x} \gt 0 for all xx Stationary points occur when:

2xx2+1=ln⁡(x2+1)\frac{2x}{x^2+1} = \ln(x^2+1)

Let u=x2+1u = x^2 + 1 (u≥1u \geq 1): 2xu=ln⁡u\frac{2x}{u} = \ln u.

This requires numerical solution. By inspection, x=0x = 0 gives 0=ln⁡1=00 = \ln 1 = 0 So x=0x = 0 is a solution.

For x>0x \gt 0: the function f(x)=2xx2+1−ln⁡(x2+1)f(x) = \frac{2x}{x^2+1} - \ln(x^2+1) starts at f(0)=0f(0) = 0 and is negative for x>0x \gt 0 (since ln⁡(x2+1)\ln(x^2+1) grows faster than 2xx2+1\frac{2x}{x^2+1} decays). So x=0x = 0 is the only stationary point.


IT-3: Inverse of an Exponential Function (with Functions)

Section titled “IT-3: Inverse of an Exponential Function (with Functions)”

Question:

The function ff is defined by f(x)=e2x−1f(x) = e^{2x-1} for x∈Rx \in \mathbb{R}.

(a) Find f−1(x)f^{-1}(x) Stating its domain and range.

(b) Find the domain of f−1∘ff^{-1} \circ f and the domain of f∘f−1f \circ f^{-1} And verify that (f−1∘f)(x)=x(f^{-1} \circ f)(x) = x and (f∘f−1)(x)=x(f \circ f^{-1})(x) = x on their respective domains.

(c) The function gg is defined by g(x)=ln⁡(x−1)+ln⁡(x+1)g(x) = \ln(x-1) + \ln(x+1) for x∈(1,∞)x \in (1, \infty). Express g(x)g(x) as a single logarithm and find g−1(x)g^{-1}(x).

[Difficulty: hard. Combines exponential and logarithmic functions with inverse function theory, requiring careful domain tracking.]

Solution:

(a) Let y=e2x−1y = e^{2x-1}. Then ln⁡y=2x−1\ln y = 2x - 1 So x=ln⁡y+12x = \frac{\ln y + 1}{2}.

f−1(x)=ln⁡x+12f^{-1}(x) = \frac{\ln x + 1}{2}

Domain of f−1f^{-1}: x>0x \gt 0 (since ln⁡x\ln x must be defined, matching the range of ff).

Range of f−1f^{-1}: R\mathbb{R} (since ln⁡x+12\frac{\ln x + 1}{2} takes all real values as xx ranges over (0,∞)(0, \infty) Matching the domain of ff).

(b) (f−1∘f)(x)=f−1(f(x))=ln⁡(e2x−1)+12=2x−1+12=x(f^{-1} \circ f)(x) = f^{-1}(f(x)) = \frac{\ln(e^{2x-1}) + 1}{2} = \frac{2x-1+1}{2} = x.

Domain: the range of ff must be within the domain of f−1f^{-1}. Range of ff is (0,∞)(0, \infty) Domain of f−1f^{-1} is (0,∞)(0, \infty). So domain is R\mathbb{R}.

(f∘f−1)(x)=f(f−1(x))=e2⋅ln⁡x+12−1=eln⁡x+1−1=eln⁡x=x(f \circ f^{-1})(x) = f(f^{-1}(x)) = e^{2 \cdot \frac{\ln x + 1}{2} - 1} = e^{\ln x + 1 - 1} = e^{\ln x} = x.

Domain: the range of f−1f^{-1} is R\mathbb{R} Which is within the domain of ff. The domain is (0,∞)(0, \infty) (the domain of f−1f^{-1}).

(c) g(x)=ln⁡(x−1)+ln⁡(x+1)=ln⁡((x−1)(x+1))=ln⁡(x2−1)g(x) = \ln(x-1) + \ln(x+1) = \ln((x-1)(x+1)) = \ln(x^2 - 1) for x∈(1,∞)x \in (1, \infty).

To find g−1g^{-1}: let y=ln⁡(x2−1)y = \ln(x^2 - 1). Then ey=x2−1e^y = x^2 - 1 So x2=ey+1x^2 = e^y + 1.

Since x>1x \gt 1 We take the positive root: x=ey+1x = \sqrt{e^y + 1}.

g−1(x)=ex+1g^{-1}(x) = \sqrt{e^x + 1}

Domain of g−1g^{-1}: R\mathbb{R} (since ex+1>0e^x + 1 \gt 0 for all xx). Range of g−1g^{-1}: (1,∞)(1, \infty).

Verification: g(g−1(x))=ln⁡(ex+1−1)=ln⁡(ex)=xg(g^{-1}(x)) = \ln(e^x + 1 - 1) = \ln(e^x) = x. Confirmed.

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