Multivariable Calculus Quiz: Multivariable Chain Rule
15 questions · exam conditions
0:00
Multivariable Chain RuleQuestion 1 of 15

Let z=f(x,y)z = f(x,y) where x=g(u,v)x = g(u,v) and y=h(u,v)y = h(u,v). If fx=3f_x = 3, fy=−2f_y = -2, gu=4g_u = 4, gv=−1g_v = -1, hu=2h_u = 2, and hv=5h_v = 5, what is ∂z∂v\frac{\partial z}{\partial v}?

−13-13
−3-3
77
1313
← Back to quizzes

Multivariable Calculus Quiz

Multivariable Calculus Quiz: Multivariable Chain Rule

Practice Multivariable Chain Rule in Multivariable Calculus with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

What this quiz covers

This quiz focuses on Multivariable Chain Rule, giving you a quick way to practice the rules, question types, and explanations that matter most for Multivariable Calculus.

How to use this quiz

Try each quiz question before looking at the correct answer. Use the explanations to review missed ideas, then come back to similar questions until the pattern feels familiar.

All questions

Question 1

Let z=f(x,y)z = f(x,y) where x=g(u,v)x = g(u,v) and y=h(u,v)y = h(u,v). If fx=3f_x = 3, fy=−2f_y = -2, gu=4g_u = 4, gv=−1g_v = -1, hu=2h_u = 2, and hv=5h_v = 5, what is ∂z∂v\frac{\partial z}{\partial v}?

  1. −13-13 (correct answer)
  2. −3-3
  3. 77
  4. 1313
Explanation: Using the multivariable chain rule: ∂z∂v=∂f∂x∂x∂v+∂f∂y∂y∂v=fx⋅gv+fy⋅hv=3(−1)+(−2)(5)=−3+(−10)=−13\frac{\partial z}{\partial v} = \frac{\partial f}{\partial x}\frac{\partial x}{\partial v} + \frac{\partial f}{\partial y}\frac{\partial y}{\partial v} = f_x \cdot g_v + f_y \cdot h_v = 3(-1) + (-2)(5) = -3 + (-10) = -13. Choice B incorrectly omits the second term. Choice C uses incorrect signs. Choice D uses the absolute value.

Question 2

The temperature on a metal plate is given by T(x,y)=100−x2−3y2T(x, y) = 100 - x^2 - 3y^2. An ant walks along the elliptical path r⃗(t)=⟨2cos⁡(t),sin⁡(t)⟩\vec{r}(t) = \langle 2\cos(t), \sin(t) \rangle for t≥0t \ge 0. What is the rate of change of the temperature experienced by the ant at the first moment it crosses the line y=xy = x?

  1. 45\frac{4}{5} (correct answer)
  2. 11
  3. −45-\frac{4}{5}
  4. 285\frac{28}{5}
Explanation: The rate of change of temperature is dTdt=∂T∂xdxdt+∂T∂ydydt\frac{dT}{dt} = \frac{\partial T}{\partial x}\frac{dx}{dt} + \frac{\partial T}{\partial y}\frac{dy}{dt}. First, find the derivatives: ∂T∂x=−2x\frac{\partial T}{\partial x} = -2x, ∂T∂y=−6y\frac{\partial T}{\partial y} = -6y, dxdt=−2sin⁡(t)\frac{dx}{dt} = -2\sin(t), dydt=cos⁡(t)\frac{dy}{dt} = \cos(t). Substituting the path equations x=2cos⁡(t)x=2\cos(t) and y=sin⁡(t)y=\sin(t) into the chain rule gives: dTdt=(−2(2cos⁡t))(−2sin⁡t)+(−6(sin⁡t))(cos⁡t)=8sin⁡tcos⁡t−6sin⁡tcos⁡t=2sin⁡tcos⁡t=sin⁡(2t)\frac{dT}{dt} = (-2(2\cos t))(-2\sin t) + (-6(\sin t))(\cos t) = 8\sin t\cos t - 6\sin t\cos t = 2\sin t\cos t = \sin(2t). The ant crosses the line y=xy=x when sin⁡(t)=2cos⁡(t)\sin(t) = 2\cos(t), which means tan⁡(t)=2\tan(t)=2. The first time this occurs for t≥0t \ge 0 is in the first quadrant. Let this time be t0t_0. We can find the values of sin⁡(t0)\sin(t_0) and cos⁡(t0)\cos(t_0) from a right triangle with opposite side 2, adjacent side 1, and hypotenuse 5\sqrt{5}. So, sin⁡(t0)=25\sin(t_0) = \frac{2}{\sqrt{5}} and cos⁡(t0)=15\cos(t_0) = \frac{1}{\sqrt{5}}. The rate of change at t0t_0 is dTdt∣t=t0=2sin⁡(t0)cos⁡(t0)=2(25)(15)=45\frac{dT}{dt}|_{t=t_0} = 2\sin(t_0)\cos(t_0) = 2(\frac{2}{\sqrt{5}})(\frac{1}{\sqrt{5}}) = \frac{4}{5}.

Question 3

Let w=f(x2−4y2)w = f(x^2 - 4y^2), where ff is any differentiable function of a single variable. Which of the following partial differential equations must ww satisfy for any choice of ff?

  1. x∂w∂x+4y∂w∂y=0x \frac{\partial w}{\partial x} + 4y \frac{\partial w}{\partial y} = 0
  2. 4y∂w∂x−x∂w∂y=04y \frac{\partial w}{\partial x} - x \frac{\partial w}{\partial y} = 0
  3. 4y∂w∂x+x∂w∂y=04y \frac{\partial w}{\partial x} + x \frac{\partial w}{\partial y} = 0 (correct answer)
  4. 2x∂w∂x+8y∂w∂y=02x \frac{\partial w}{\partial x} + 8y \frac{\partial w}{\partial y} = 0
Explanation: Let u=x2−4y2u = x^2 - 4y^2, so w=f(u)w = f(u). We use the chain rule to find the partial derivatives of ww with respect to xx and yy. Note that ff is a function of a single variable uu, so its derivative is f′(u)f'(u). ∂w∂x=dfdu∂u∂x=f′(u)⋅(2x)\frac{\partial w}{\partial x} = \frac{df}{du} \frac{\partial u}{\partial x} = f'(u) \cdot (2x). ∂w∂y=dfdu∂u∂y=f′(u)⋅(−8y)\frac{\partial w}{\partial y} = \frac{df}{du} \frac{\partial u}{\partial y} = f'(u) \cdot (-8y). To find a relationship that holds for any ff, we must eliminate the f′(u)f'(u) term. We can do this by solving for f′(u)f'(u) in both equations: From the first equation, f′(u)=12x∂w∂xf'(u) = \frac{1}{2x} \frac{\partial w}{\partial x} (for x≠0x\neq 0). From the second equation, f′(u)=1−8y∂w∂yf'(u) = \frac{1}{-8y} \frac{\partial w}{\partial y} (for y≠0y\neq 0). Setting the expressions for f′(u)f'(u) equal gives: 12x∂w∂x=1−8y∂w∂y\frac{1}{2x} \frac{\partial w}{\partial x} = \frac{1}{-8y} \frac{\partial w}{\partial y}. Multiplying both sides by −16xy-16xy to clear denominators gives: −8y∂w∂x=2x∂w∂y-8y \frac{\partial w}{\partial x} = 2x \frac{\partial w}{\partial y}. Rearranging the terms to one side gives the partial differential equation: 8y∂w∂x+2x∂w∂y=08y \frac{\partial w}{\partial x} + 2x \frac{\partial w}{\partial y} = 0, which simplifies to 4y∂w∂x+x∂w∂y=04y \frac{\partial w}{\partial x} + x \frac{\partial w}{\partial y} = 0.

Question 4

Let z=f(x,y)z = f(x, y), where x=rcos⁡θx = r \cos\theta and y=rsin⁡θy = r \sin\theta. Given that ∂z∂r=1rx\frac{\partial z}{\partial r} = \frac{1}{r}x and ∂z∂θ=−y\frac{\partial z}{\partial \theta} = -y, find the expression for ∂z∂x\frac{\partial z}{\partial x} in terms of xx and yy.

  1. 2xx2+y2\frac{2x}{x^2+y^2}
  2. x2x^2
  3. xx2+y2\frac{x}{x^2+y^2}
  4. 11 (correct answer)
Explanation: When you encounter a problem involving coordinate transformations like polar to Cartesian, you need to use the chain rule to connect partial derivatives in different coordinate systems. To find ∂z∂x\frac{\partial z}{\partial x}, use the chain rule: ∂z∂x=∂z∂r∂r∂x+∂z∂θ∂θ∂x\frac{\partial z}{\partial x} = \frac{\partial z}{\partial r} \frac{\partial r}{\partial x} + \frac{\partial z}{\partial \theta} \frac{\partial \theta}{\partial x} First, find the needed partial derivatives. From r=x2+y2r = \sqrt{x^2 + y^2}, we get ∂r∂x=xr\frac{\partial r}{\partial x} = \frac{x}{r}. From θ=arctan⁡(y/x)\theta = \arctan(y/x), we get ∂θ∂x=−yx2+y2\frac{\partial \theta}{\partial x} = -\frac{y}{x^2 + y^2}. Substituting the given information: ∂z∂x=1rx⋅xr+(−y)⋅(−yx2+y2)=x2r2+y2x2+y2\frac{\partial z}{\partial x} = \frac{1}{r}x \cdot \frac{x}{r} + (-y) \cdot \left(-\frac{y}{x^2 + y^2}\right) = \frac{x^2}{r^2} + \frac{y^2}{x^2 + y^2} Since r2=x2+y2r^2 = x^2 + y^2, this becomes: ∂z∂x=x2x2+y2+y2x2+y2=x2+y2x2+y2=1\frac{\partial z}{\partial x} = \frac{x^2}{x^2 + y^2} + \frac{y^2}{x^2 + y^2} = \frac{x^2 + y^2}{x^2 + y^2} = 1 The answer is D. Option A gives 2xx2+y2\frac{2x}{x^2+y^2}, which would result from incorrectly doubling the first term. Option B suggests x2x^2, ignoring the coordinate transformation entirely. Option C gives xx2+y2\frac{x}{x^2+y^2}, which results from forgetting to include the second term from the chain rule. Remember: when transforming between coordinate systems, always apply the full chain rule and carefully track all terms—they often combine to give surprisingly simple results.

Question 5

Let z=f(x,y)z = f(x, y) be a differentiable function. A particle moves in the xyxy-plane along a path r⃗(t)=⟨x(t),y(t)⟩\vec{r}(t) = \langle x(t), y(t) \rangle. It is observed that the value of zz remains constant along the particle's path. Which of the following statements must be true?

  1. The particle's velocity vector is always parallel to the gradient of ff.
  2. The particle must be stationary.
  3. The particle's path follows a level curve of the function ff. (correct answer)
  4. The gradient of ff must be the zero vector at all points along the path.
Explanation: The rate of change of zz along the path is given by the chain rule: dzdt=∂f∂xdxdt+∂f∂ydydt\frac{dz}{dt} = \frac{\partial f}{\partial x}\frac{dx}{dt} + \frac{\partial f}{\partial y}\frac{dy}{dt}. This can be written as the dot product of the gradient of ff, ∇f=⟨∂f∂x,∂f∂y⟩\nabla f = \langle \frac{\partial f}{\partial x}, \frac{\partial f}{\partial y} \rangle, and the velocity vector of the particle, v⃗(t)=r⃗′(t)=⟨dxdt,dydt⟩\vec{v}(t) = \vec{r}'(t) = \langle \frac{dx}{dt}, \frac{dy}{dt} \rangle. So, dzdt=∇f⋅v⃗(t)\frac{dz}{dt} = \nabla f \cdot \vec{v}(t). We are given that zz remains constant along the path, which means dzdt=0\frac{dz}{dt} = 0. Therefore, ∇f⋅v⃗(t)=0\nabla f \cdot \vec{v}(t) = 0. This implies that the gradient vector ∇f\nabla f is orthogonal (perpendicular) to the velocity vector v⃗(t)\vec{v}(t) at every point on the path. The velocity vector is tangent to the path. Since the gradient vector is always normal to the level curves of a function, and the path's tangent vector is always orthogonal to the gradient, the path must be tangent to the level curves at every point. This means the particle's path follows a level curve of ff.

Question 6

Let w=g(u,v)w = g(u, v), where u=x+yu = x+y and v=yxv = \frac{y}{x}. It is known that at the point (x,y)=(1,1)(x,y)=(1,1), we have u=2,v=1u=2, v=1, and the partial derivatives are ∂g∂u=4\frac{\partial g}{\partial u} = 4 and ∂g∂v=−2\frac{\partial g}{\partial v} = -2. What is the value of ∂w∂x\frac{\partial w}{\partial x} at (x,y)=(1,1)(x,y)=(1,1)?

  1. 22
  2. 66 (correct answer)
  3. 44
  4. 88
Explanation: When you encounter a problem involving a composite function where the inner variables are functions of other variables, you need to use the chain rule for multivariable functions. Here, w=g(u,v)w = g(u,v) where both uu and vv depend on xx and yy. To find ∂w∂x\frac{\partial w}{\partial x}, apply the multivariable chain rule: ∂w∂x=∂g∂u⋅∂u∂x+∂g∂v⋅∂v∂x\frac{\partial w}{\partial x} = \frac{\partial g}{\partial u} \cdot \frac{\partial u}{\partial x} + \frac{\partial g}{\partial v} \cdot \frac{\partial v}{\partial x} First, calculate the partial derivatives of the inner functions:
  • u=x+yu = x + y, so ∂u∂x=1\frac{\partial u}{\partial x} = 1
  • v=yxv = \frac{y}{x}, so ∂v∂x=−yx2\frac{\partial v}{\partial x} = -\frac{y}{x^2}
At the point (x,y)=(1,1)(x,y) = (1,1), we have ∂v∂x=−112=−1\frac{\partial v}{\partial x} = -\frac{1}{1^2} = -1. Now substitute the given values: ∂g∂u=4\frac{\partial g}{\partial u} = 4 and ∂g∂v=−2\frac{\partial g}{\partial v} = -2: ∂w∂x=4⋅1+(−2)⋅(−1)=4+2=6\frac{\partial w}{\partial x} = 4 \cdot 1 + (-2) \cdot (-1) = 4 + 2 = 6 Choice A (22) would result from forgetting the second term of the chain rule. Choice C (44) comes from using only the first term ∂g∂u⋅∂u∂x\frac{\partial g}{\partial u} \cdot \frac{\partial u}{\partial x}. Choice D (88) might result from sign errors or incorrect application of the quotient rule. Study tip: For chain rule problems, always write out the full formula first, then systematically find each partial derivative. Double-check your derivative of v=yxv = \frac{y}{x} with respect to xx — treat yy as constant and use the power rule: v=yx−1v = yx^{-1}.

Question 7

Let w=f(u,v)w = f(u, v) be a differentiable function. The variables uu and vv are functions of xx and yy, which are in turn functions of rr and θ\theta. The relationships are given below, along with values of the partial derivatives at specific points:

  • x=rcos⁡θx = r\cos\theta, y=rsin⁡θy = r\sin\theta
  • At (r,θ)=(2,π/6)(r, \theta) = (2, \pi/6), the corresponding Cartesian coordinates are (x,y)=(3,1)(x, y) = (\sqrt{3}, 1).
  • At (x,y)=(3,1)(x, y) = (\sqrt{3}, 1), the values of uu and vv and their partials are: u=5u=5, v=0v=0, ∂u∂x=3\frac{\partial u}{\partial x}=3, ∂u∂y=−1\frac{\partial u}{\partial y}=-1, ∂v∂x=2\frac{\partial v}{\partial x}=2, ∂v∂y=4\frac{\partial v}{\partial y}=4.
  • At (u,v)=(5,0)(u,v)=(5,0), the partials of ff are: ∂f∂u=6\frac{\partial f}{\partial u}=6, ∂f∂v=−2\frac{\partial f}{\partial v}=-2.

Using the information provided, what is the value of ∂w∂r\frac{\partial w}{\partial r} at the point (r,θ)=(2,π/6)(r, \theta) = (2, \pi/6)?

  1. 7(3−1)7(\sqrt{3}-1) (correct answer)
  2. 73+17\sqrt{3}+1
  3. 53−75\sqrt{3}-7
  4. −14(1+3)-14(1+\sqrt{3})
Explanation: The chain rule for ∂w∂r\frac{\partial w}{\partial r} requires us to first find ∂w∂x\frac{\partial w}{\partial x} and ∂w∂y\frac{\partial w}{\partial y}. ∂w∂x=∂f∂u∂u∂x+∂f∂v∂v∂x=(6)(3)+(−2)(2)=18−4=14\frac{\partial w}{\partial x} = \frac{\partial f}{\partial u}\frac{\partial u}{\partial x} + \frac{\partial f}{\partial v}\frac{\partial v}{\partial x} = (6)(3) + (-2)(2) = 18 - 4 = 14. ∂w∂y=∂f∂u∂u∂y+∂f∂v∂v∂y=(6)(−1)+(−2)(4)=−6−8=−14\frac{\partial w}{\partial y} = \frac{\partial f}{\partial u}\frac{\partial u}{\partial y} + \frac{\partial f}{\partial v}\frac{\partial v}{\partial y} = (6)(-1) + (-2)(4) = -6 - 8 = -14. Next, we find the partial derivatives of xx and yy with respect to rr: x=rcos⁡θ  ⟹  ∂x∂r=cos⁡θx = r\cos\theta \implies \frac{\partial x}{\partial r} = \cos\theta. y=rsin⁡θ  ⟹  ∂y∂r=sin⁡θy = r\sin\theta \implies \frac{\partial y}{\partial r} = \sin\theta. At (r,θ)=(2,π/6)(r, \theta) = (2, \pi/6), ∂x∂r=cos⁡(π/6)=32\frac{\partial x}{\partial r} = \cos(\pi/6) = \frac{\sqrt{3}}{2} and ∂y∂r=sin⁡(π/6)=12\frac{\partial y}{\partial r} = \sin(\pi/6) = \frac{1}{2}. Now, we can apply the final chain rule: ∂w∂r=∂w∂x∂x∂r+∂w∂y∂y∂r\frac{\partial w}{\partial r} = \frac{\partial w}{\partial x}\frac{\partial x}{\partial r} + \frac{\partial w}{\partial y}\frac{\partial y}{\partial r}. Substituting the values we found: ∂w∂r=(14)(32)+(−14)(12)=73−7=7(3−1)\frac{\partial w}{\partial r} = (14)(\frac{\sqrt{3}}{2}) + (-14)(\frac{1}{2}) = 7\sqrt{3} - 7 = 7(\sqrt{3}-1). Distractor B comes from a sign error when computing ∂w∂y\frac{\partial w}{\partial y}. Distractor C comes from a cross-term error when computing ∂w∂x\frac{\partial w}{\partial x}. Distractor D is the value of ∂w∂θ\frac{\partial w}{\partial \theta}.

Question 8

Let P(V,T)P(V, T) be the pressure of a gas, depending on volume VV and temperature TT. The volume and temperature are changing with time tt according to V(t)=10+0.5t2V(t) = 10 + 0.5t^2 and T(t)=300+2tT(t) = 300 + 2t. At time t=10t=10, it is measured that V=60V=60, T=320T=320, ∂P∂V=−2\frac{\partial P}{\partial V} = -2, and ∂P∂T=5\frac{\partial P}{\partial T} = 5. However, the volume measurements are calibrated in liters (L) and the temperature in Kelvin (K), while the time is in seconds (s). The pressure is measured in kilopascals (kPa). What is the rate of change of pressure with respect to time, dPdt\frac{dP}{dt}, at t=10t=10 seconds?

  1. 33 kPa/s
  2. 88 kPa/s
  3. −10-10 kPa/s (correct answer)
  4. −12-12 kPa/s
Explanation: The rate of change of pressure with respect to time is given by the chain rule: dPdt=∂P∂VdVdt+∂P∂TdTdt\frac{dP}{dt} = \frac{\partial P}{\partial V}\frac{dV}{dt} + \frac{\partial P}{\partial T}\frac{dT}{dt}. We are given the values of the partial derivatives at the time of interest: ∂P∂V=−2\frac{\partial P}{\partial V} = -2 kPa/L and ∂P∂T=5\frac{\partial P}{\partial T} = 5 kPa/K. We need to find the rates of change of volume and temperature with respect to time by differentiating their respective functions. V(t)=10+0.5t2  ⟹  dVdt=tV(t) = 10 + 0.5t^2 \implies \frac{dV}{dt} = t. T(t)=300+2t  ⟹  dTdt=2T(t) = 300 + 2t \implies \frac{dT}{dt} = 2. Now, we evaluate these rates at t=10t=10 s. dVdt∣t=10=10\frac{dV}{dt}|_{t=10} = 10 L/s. dTdt∣t=10=2\frac{dT}{dt}|_{t=10} = 2 K/s. The given values of V=60V=60 and T=320T=320 at t=10t=10 confirm we are at the correct point, as V(10)=10+0.5(100)=60V(10) = 10+0.5(100)=60 and T(10)=300+2(10)=320T(10)=300+2(10)=320. We can now substitute all the values into the chain rule expression: dPdt=(−2 kPa/L)(10 L/s)+(5 kPa/K)(2 K/s)=−20 kPa/s+10 kPa/s=−10 kPa/s\frac{dP}{dt} = (-2 \text{ kPa/L})(10 \text{ L/s}) + (5 \text{ kPa/K})(2 \text{ K/s}) = -20 \text{ kPa/s} + 10 \text{ kPa/s} = -10 \text{ kPa/s}.

Question 9

Let w=f(x,y)w=f(x,y), where ff is a twice-differentiable function. Consider a change of variables given by u=x+yu=x+y and v=x−yv=x-y.

Which of the following expressions is equivalent to ∂2w∂x∂y\frac{\partial^2 w}{\partial x \partial y}?

  1. ∂2f∂u∂v−∂2f∂v∂u\frac{\partial^2 f}{\partial u \partial v} - \frac{\partial^2 f}{\partial v \partial u}
  2. ∂2f∂u2+∂2f∂v2\frac{\partial^2 f}{\partial u^2} + \frac{\partial^2 f}{\partial v^2}
  3. ∂2f∂u2−∂2f∂v∂u−∂2f∂v2\frac{\partial^2 f}{\partial u^2} - \frac{\partial^2 f}{\partial v \partial u} - \frac{\partial^2 f}{\partial v^2}
  4. ∂2f∂u2−∂2f∂v2\frac{\partial^2 f}{\partial u^2} - \frac{\partial^2 f}{\partial v^2} (correct answer)
Explanation: When you encounter a change of variables problem in multivariable calculus, you need to systematically apply the chain rule to transform partial derivatives from one coordinate system to another. To find ∂2w∂x∂y\frac{\partial^2 w}{\partial x \partial y}, start by finding the first-order partial derivatives. Using the chain rule with u=x+yu = x + y and v=x−yv = x - y: ∂w∂x=∂f∂u⋅∂u∂x+∂f∂v⋅∂v∂x=∂f∂u+∂f∂v\frac{\partial w}{\partial x} = \frac{\partial f}{\partial u} \cdot \frac{\partial u}{\partial x} + \frac{\partial f}{\partial v} \cdot \frac{\partial v}{\partial x} = \frac{\partial f}{\partial u} + \frac{\partial f}{\partial v} Now differentiate this with respect to yy: ∂2w∂x∂y=∂∂y(∂f∂u+∂f∂v)\frac{\partial^2 w}{\partial x \partial y} = \frac{\partial}{\partial y}\left(\frac{\partial f}{\partial u} + \frac{\partial f}{\partial v}\right) Applying the chain rule again: =∂2f∂u2⋅∂u∂y+∂2f∂u∂v⋅∂v∂y+∂2f∂v∂u⋅∂u∂y+∂2f∂v2⋅∂v∂y= \frac{\partial^2 f}{\partial u^2} \cdot \frac{\partial u}{\partial y} + \frac{\partial^2 f}{\partial u \partial v} \cdot \frac{\partial v}{\partial y} + \frac{\partial^2 f}{\partial v \partial u} \cdot \frac{\partial u}{\partial y} + \frac{\partial^2 f}{\partial v^2} \cdot \frac{\partial v}{\partial y} Since ∂u∂y=1\frac{\partial u}{\partial y} = 1 and ∂v∂y=−1\frac{\partial v}{\partial y} = -1, and mixed partials are equal (∂2f∂u∂v=∂2f∂v∂u\frac{\partial^2 f}{\partial u \partial v} = \frac{\partial^2 f}{\partial v \partial u}): =∂2f∂u2−∂2f∂u∂v+∂2f∂v∂u−∂2f∂v2=∂2f∂u2−∂2f∂v2= \frac{\partial^2 f}{\partial u^2} - \frac{\partial^2 f}{\partial u \partial v} + \frac{\partial^2 f}{\partial v \partial u} - \frac{\partial^2 f}{\partial v^2} = \frac{\partial^2 f}{\partial u^2} - \frac{\partial^2 f}{\partial v^2} This confirms answer D. A incorrectly assumes mixed partials aren't equal. B omits the negative signs from the chain rule. C includes an extra mixed partial term that should cancel out. Study tip: Always track the signs carefully when applying the chain rule, and remember that mixed partial derivatives are equal for smooth functions.

Question 10

Let w=f(x,y,z)w = f(x,y,z) where x=u+vx = u + v, y=u−vy = u - v, and z=uvz = uv. If ∂w∂u=3\frac{\partial w}{\partial u} = 3 and ∂w∂v=−2\frac{\partial w}{\partial v} = -2 at a certain point, what is ∂w∂x\frac{\partial w}{\partial x} at that point?

  1. 11
  2. 52\frac{5}{2}
  3. 12\frac{1}{2} (correct answer)
  4. 32\frac{3}{2}
Explanation: This is a classic chain rule problem involving implicit functions. When you have a function w=f(x,y,z)w = f(x,y,z) where xx, yy, and zz are themselves functions of other variables, you need to use the chain rule to find partial derivatives with respect to the new variables. To find ∂w∂x\frac{\partial w}{\partial x}, you need to express it in terms of the given information about ∂w∂u\frac{\partial w}{\partial u} and ∂w∂v\frac{\partial w}{\partial v}. Since x=u+vx = u + v, you can solve for uu and vv in terms of xx and yy: from x=u+vx = u + v and y=u−vy = u - v, you get u=x+y2u = \frac{x+y}{2} and v=x−y2v = \frac{x-y}{2}. Using the chain rule: ∂w∂x=∂w∂u∂u∂x+∂w∂v∂v∂x\frac{\partial w}{\partial x} = \frac{\partial w}{\partial u}\frac{\partial u}{\partial x} + \frac{\partial w}{\partial v}\frac{\partial v}{\partial x} From the expressions above, ∂u∂x=12\frac{\partial u}{\partial x} = \frac{1}{2} and ∂v∂x=12\frac{\partial v}{\partial x} = \frac{1}{2}. Substituting: ∂w∂x=3⋅12+(−2)⋅12=32−1=12\frac{\partial w}{\partial x} = 3 \cdot \frac{1}{2} + (-2) \cdot \frac{1}{2} = \frac{3}{2} - 1 = \frac{1}{2} Option A (11) likely comes from incorrectly assuming ∂u∂x=∂v∂x=1\frac{\partial u}{\partial x} = \frac{\partial v}{\partial x} = 1. Option B (52\frac{5}{2}) results from adding the given partial derivatives directly. Option D (32\frac{3}{2}) comes from using only the first term of the chain rule. Remember: when variables are related through transformations, always write out the full chain rule expansion and carefully compute each partial derivative in the transformation.

Question 11

If z=ln⁡(x2+y2)z = \ln(x^2 + y^2) where x=etcos⁡sx = e^t \cos s and y=etsin⁡sy = e^t \sin s, what is ∂z∂s\frac{\partial z}{\partial s}?

  1. 2et(cos⁡s−sin⁡s)e2t\frac{2e^t(\cos s - \sin s)}{e^{2t}}
  2. 00 (correct answer)
  3. 2(−sin⁡s+cos⁡s)cos⁡2s+sin⁡2s\frac{2(-\sin s + \cos s)}{\cos^2 s + \sin^2 s}
  4. 22
Explanation: First, note that x2+y2=e2tcos⁡2s+e2tsin⁡2s=e2t(cos⁡2s+sin⁡2s)=e2tx^2 + y^2 = e^{2t}\cos^2 s + e^{2t}\sin^2 s = e^{2t}(\cos^2 s + \sin^2 s) = e^{2t}. Therefore z=ln⁡(e2t)=2tz = \ln(e^{2t}) = 2t. Since zz depends only on tt and not on ss, we have ∂z∂s=0\frac{\partial z}{\partial s} = 0. The other choices result from incorrectly applying the chain rule without first simplifying the expression.

Question 12

Let zz be a differentiable function of xx and yy that satisfies the equation z3+zx+y2=12z^3 + zx + y^2 = 12. If x(t)=2t2x(t) = 2t^2 and y(t)=3ty(t) = 3t, find the value of dzdt\frac{dz}{dt} at the moment when t=1t=1.

  1. 225\frac{22}{5}
  2. −225-\frac{22}{5} (correct answer)
  3. −275-\frac{27}{5}
  4. −345-\frac{34}{5}
Explanation: First, find the values of xx, yy, and zz at t=1t=1. At t=1t=1, we have x(1)=2(1)2=2x(1)=2(1)^2=2 and y(1)=3(1)=3y(1)=3(1)=3. Substituting these into the governing equation gives z3+z(2)+(3)2=12z^3 + z(2) + (3)^2 = 12, which simplifies to z3+2z−3=0z^3 + 2z - 3 = 0. By inspection, z=1z=1 is a solution. To find dzdt\frac{dz}{dt}, we use the chain rule: dzdt=∂z∂xdxdt+∂z∂ydydt\frac{dz}{dt} = \frac{\partial z}{\partial x}\frac{dx}{dt} + \frac{\partial z}{\partial y}\frac{dy}{dt}. We need the partial derivatives of zz. Differentiating the equation z3+zx+y2=12z^3 + zx + y^2 = 12 implicitly: With respect to xx: 3z2∂z∂x+(z+x∂z∂x)+0=0  ⟹  (3z2+x)∂z∂x=−z  ⟹  ∂z∂x=−z3z2+x3z^2\frac{\partial z}{\partial x} + (z + x\frac{\partial z}{\partial x}) + 0 = 0 \implies (3z^2+x)\frac{\partial z}{\partial x} = -z \implies \frac{\partial z}{\partial x} = \frac{-z}{3z^2+x}. With respect to yy: 3z2∂z∂y+x∂z∂y+2y=0  ⟹  (3z2+x)∂z∂y=−2y  ⟹  ∂z∂y=−2y3z2+x3z^2\frac{\partial z}{\partial y} + x\frac{\partial z}{\partial y} + 2y = 0 \implies (3z^2+x)\frac{\partial z}{\partial y} = -2y \implies \frac{\partial z}{\partial y} = \frac{-2y}{3z^2+x}. At the point (x,y,z)=(2,3,1)(x,y,z)=(2,3,1), we have ∂z∂x=−13(1)2+2=−15\frac{\partial z}{\partial x} = \frac{-1}{3(1)^2+2} = -\frac{1}{5} and ∂z∂y=−2(3)3(1)2+2=−65\frac{\partial z}{\partial y} = \frac{-2(3)}{3(1)^2+2} = -\frac{6}{5}. Next, we find the derivatives of the path functions: dxdt=4t\frac{dx}{dt} = 4t and dydt=3\frac{dy}{dt} = 3. At t=1t=1, dxdt=4\frac{dx}{dt}=4 and dydt=3\frac{dy}{dt}=3. Finally, substitute all values into the chain rule: dzdt=(−15)(4)+(−65)(3)=−45−185=−225\frac{dz}{dt} = (-\frac{1}{5})(4) + (-\frac{6}{5})(3) = -\frac{4}{5} - \frac{18}{5} = -\frac{22}{5}.

Question 13

The equation xln⁡y+yln⁡z+zln⁡x=0x \ln y + y \ln z + z \ln x = 0 implicitly defines zz as a function of xx and yy near the point (1,1,1)(1, 1, 1). Find the value of ∂z∂x\frac{\partial z}{\partial x} at this point.

  1. −1-1 (correct answer)
  2. 11
  3. 00
  4. −12-\frac{1}{2}
Explanation: Let F(x,y,z)=xln⁡y+yln⁡z+zln⁡x=0F(x, y, z) = x \ln y + y \ln z + z \ln x = 0. The formula for implicit differentiation is ∂z∂x=−∂F/∂x∂F/∂z\frac{\partial z}{\partial x} = -\frac{\partial F / \partial x}{\partial F / \partial z}. First, we compute the partial derivatives of FF. ∂F∂x=∂∂x(xln⁡y+yln⁡z+zln⁡x)=ln⁡y+0+zx\frac{\partial F}{\partial x} = \frac{\partial}{\partial x}(x \ln y + y \ln z + z \ln x) = \ln y + 0 + \frac{z}{x}. ∂F∂z=∂∂z(xln⁡y+yln⁡z+zln⁡x)=0+yz+ln⁡x\frac{\partial F}{\partial z} = \frac{\partial}{\partial z}(x \ln y + y \ln z + z \ln x) = 0 + \frac{y}{z} + \ln x. Now, we evaluate these partial derivatives at the point (1,1,1)(1, 1, 1). ∂F∂x∣(1,1,1)=ln⁡(1)+11=0+1=1\frac{\partial F}{\partial x}|_{(1,1,1)} = \ln(1) + \frac{1}{1} = 0 + 1 = 1. ∂F∂z∣(1,1,1)=11+ln⁡(1)=1+0=1\frac{\partial F}{\partial z}|_{(1,1,1)} = \frac{1}{1} + \ln(1) = 1 + 0 = 1. Finally, we use the formula: ∂z∂x=−11=−1\frac{\partial z}{\partial x} = -\frac{1}{1} = -1. A common error is to forget the negative sign in the formula, leading to the answer 1.

Question 14

Let F(x,y,z)=0F(x,y,z) = 0 define zz implicitly as a function of xx and yy. If Fx=6F_x = 6, Fy=−4F_y = -4, and Fz=8F_z = 8, what is ∂z∂x\frac{\partial z}{\partial x}?

  1. 43\frac{4}{3}
  2. 34\frac{3}{4}
  3. −43-\frac{4}{3}
  4. −34-\frac{3}{4} (correct answer)
Explanation: When you see an equation like F(x,y,z)=0F(x,y,z) = 0 that defines zz implicitly as a function of xx and yy, you need to use implicit differentiation to find partial derivatives like ∂z∂x\frac{\partial z}{\partial x}. The key insight is applying the chain rule. When you differentiate F(x,y,z)=0F(x,y,z) = 0 with respect to xx while treating yy as constant, you get: ∂F∂x+∂F∂z⋅∂z∂x=0\frac{\partial F}{\partial x} + \frac{\partial F}{\partial z} \cdot \frac{\partial z}{\partial x} = 0 This comes from recognizing that zz depends on xx, so differentiating FF with respect to zz requires multiplying by ∂z∂x\frac{\partial z}{\partial x}. Solving for ∂z∂x\frac{\partial z}{\partial x}: ∂z∂x=−∂F∂x∂F∂z=−FxFz\frac{\partial z}{\partial x} = -\frac{\frac{\partial F}{\partial x}}{\frac{\partial F}{\partial z}} = -\frac{F_x}{F_z} Substituting the given values: ∂z∂x=−68=−34\frac{\partial z}{\partial x} = -\frac{6}{8} = -\frac{3}{4} Answer D is correct. Answer A (43\frac{4}{3}) uses the wrong ratio and misses the negative sign. Answer B (34\frac{3}{4}) has the correct magnitude but forgets the crucial negative sign that comes from moving FxF_x to the other side of the equation. Answer C (−43-\frac{4}{3}) incorrectly uses FzFx\frac{F_z}{F_x} instead of FxFz\frac{F_x}{F_z} but does include the negative sign. Remember the formula: ∂z∂x=−FxFz\frac{\partial z}{\partial x} = -\frac{F_x}{F_z} and ∂z∂y=−FyFz\frac{\partial z}{\partial y} = -\frac{F_y}{F_z}. The negative sign is essential and comes directly from implicit differentiation.

Question 15

If u=f(x−y,y−z,z−x)u = f(x-y, y-z, z-x) where ff is differentiable, which expression represents ∂u∂x+∂u∂y+∂u∂z\frac{\partial u}{\partial x} + \frac{\partial u}{\partial y} + \frac{\partial u}{\partial z}?

  1. f1+f2+f3f_1 + f_2 + f_3
  2. 00 (correct answer)
  3. f1−f2−f3f_1 - f_2 - f_3
  4. −f1+f2−f3-f_1 + f_2 - f_3
Explanation: Let w1=x−yw_1 = x-y, w2=y−zw_2 = y-z, w3=z−xw_3 = z-x. Then ∂u∂x=f1⋅1+f2⋅0+f3⋅(−1)=f1−f3\frac{\partial u}{\partial x} = f_1 \cdot 1 + f_2 \cdot 0 + f_3 \cdot (-1) = f_1 - f_3, ∂u∂y=f1⋅(−1)+f2⋅1+f3⋅0=−f1+f2\frac{\partial u}{\partial y} = f_1 \cdot (-1) + f_2 \cdot 1 + f_3 \cdot 0 = -f_1 + f_2, ∂u∂z=f1⋅0+f2⋅(−1)+f3⋅1=−f2+f3\frac{\partial u}{\partial z} = f_1 \cdot 0 + f_2 \cdot (-1) + f_3 \cdot 1 = -f_2 + f_3. Adding: (f1−f3)+(−f1+f2)+(−f2+f3)=0(f_1 - f_3) + (-f_1 + f_2) + (-f_2 + f_3) = 0. The other choices result from incorrectly applying the chain rule.