← 4. Classical Demand Theory

Exercises

Problems to check your understanding of this chapter. The solutions are folded away — try them yourself first.

Easy

1Easy

With u(x1,x2)=x11/3x22/3u(x_1, x_2) = x_1^{1/3} x_2^{2/3}, p1=2p_1 = 2, p2=3p_2 = 3, w=120w = 120, find Walrasian demand x(p,w)x(p, w) and indirect utility v(p,w)v(p, w).

xl(p,w)=alwplx_l(p, w) = \frac{a_l w}{p_l}
The tangency at a=1/3a = 1/3, p=(2,3)p = (2, 3), w=120w = 120.
Show solution
  1. Plug a=1/3a = 1/3 into the Cobb-Douglas demand formula: x1=(1/3)⋅1202=20x_1 = \frac{(1/3) \cdot 120}{2} = 20, x2=(2/3)⋅1203=803x_2 = \frac{(2/3) \cdot 120}{3} = \frac{80}{3}.

  2. Indirect utility is v=201/3(80/3)2/3v = 20^{1/3} (80/3)^{2/3}. Checking the budget: 2⋅20+3⋅80/3=1202 \cdot 20 + 3 \cdot 80/3 = 120 — Walras' law holds.

2Easy

Starting from the budget line with p1=1p_1 = 1, p2=2p_2 = 2, w=100w = 100, how does the budget line move when ww rises to 150150?

Find the new optimum of a Cobb-Douglas consumer with a=1/2a = 1/2.

Show solution
  1. A pure income rise shifts the budget line outward in parallel: intercepts move from (100,50)(100, 50) to (150,75)(150, 75).

  2. Demand is proportional to wealth, so x1=0.5⋅150/1=75x_1 = 0.5 \cdot 150/1 = 75, x2=0.5⋅150/2=37.5x_2 = 0.5 \cdot 150/2 = 37.5 — exactly 1.51.5 times the original (50,25)(50, 25).

Medium

3Medium

Let u=x11/4x23/4u = x_1^{1/4} x_2^{3/4}, p2=1p_2 = 1, w=80w = 80.

When p1p_1 rises from 11 to 44, compute the substitution, income, and total effects of the Slutsky decomposition.

A=x(p,w),w′=p′⋅A,B=x(p′,w′),C=x(p′,w)A = x(p, w), \quad w' = p' \cdot A, \quad B = x(p', w'), \quad C = x(p', w)
a=1/4a = 1/4, p1:1→4p_1: 1 \to 4, w=80w = 80 — substitution −11.25-11.25, income −3.75-3.75.
Show solution
  1. With a=1/4a = 1/4, A=(0.25⋅80/1, 0.75⋅80/1)=(20,60)A = (0.25 \cdot 80/1,\ 0.75 \cdot 80/1) = (20, 60). Slutsky compensated income is w′=4⋅20+60=140w' = 4 \cdot 20 + 60 = 140.

  2. B=(0.25⋅140/4, 0.75⋅140)=(8.75,105)B = (0.25 \cdot 140/4,\ 0.75 \cdot 140) = (8.75, 105), C=(0.25⋅80/4, 0.75⋅80)=(5,60)C = (0.25 \cdot 80/4,\ 0.75 \cdot 80) = (5, 60).

  3. Substitution effect =8.75−20=−11.25= 8.75 - 20 = -11.25, income effect =5−8.75=−3.75= 5 - 8.75 = -3.75, total =5−20=−15= 5 - 20 = -15. The substitution effect is negative, and since the good is normal the income effect is negative too.

    −15=−11.25⏟substitution+(−3.75)⏟income-15 = \underbrace{-11.25}_{\text{substitution}} + \underbrace{(-3.75)}_{\text{income}}
4Medium

Prove directly from the definition of the EMP that the expenditure function e(p,u)e(p, u) is homogeneous of degree one in prices.

e(p,u)=min⁡u(x)≥up⋅xe(p, u) = \min_{u(x) \ge u} p \cdot x
Show solution
  1. For α>0\alpha > 0, e(αp,u)=min⁡u(x)≥u(αp)⋅x=αmin⁡u(x)≥up⋅x=αe(p,u)e(\alpha p, u) = \min_{u(x)\ge u} (\alpha p) \cdot x = \alpha \min_{u(x)\ge u} p \cdot x = \alpha e(p, u). The scalar α\alpha factors out because the constraint set does not involve prices.

  2. The economics: doubling every price exactly doubles the cheapest cost of a given utility — only the unit of money changed.

Hard

5Hard

Prove with the Slutsky equation that a Giffen good cannot arise under Cobb-Douglas utility.

∂x1∂p1=∂h1∂p1−∂x1∂wx1\frac{\partial x_1}{\partial p_1} = \frac{\partial h_1}{\partial p_1} - \frac{\partial x_1}{\partial w} x_1
Show solution
  1. In Cobb-Douglas, ∂x1/∂w=a/p1>0\partial x_1/\partial w = a/p_1 > 0 — good 1 is always normal. So the income effect −(∂x1/∂w)x1-(\partial x_1/\partial w) x_1 is always negative.

  2. The substitution effect ∂h1/∂p1≤0\partial h_1/\partial p_1 \le 0 is also never positive (compensated law of demand), so the total effect is a sum of two negatives — always negative. A Giffen good (∂x1/∂p1>0\partial x_1/\partial p_1 > 0) is impossible.

6Hard

Prove the duality identity e(p,v(p,w))=we(p, v(p, w)) = w from the definitions of the UMP and EMP (assume interior solutions and local nonsatiation).

v(p,w)=max⁡p⋅x≤wu(x),e(p,u)=min⁡u(x)≥up⋅xv(p, w) = \max_{p \cdot x \le w} u(x), \qquad e(p, u) = \min_{u(x) \ge u} p \cdot x
Show solution
  1. Let x∗=x(p,w)x^* = x(p, w) solve the UMP.

    By local nonsatiation p⋅x∗=wp \cdot x^* = w and u(x∗)=v(p,w)u(x^*) = v(p, w).

    Since x∗x^* is feasible for the EMP at target utility v(p,w)v(p,w), e(p,v(p,w))≤p⋅x∗=we(p, v(p, w)) \le p \cdot x^* = w.

  2. Conversely, if e(p,v(p,w))<we(p, v(p,w)) < w, the EMP solution yy satisfies p⋅y<wp \cdot y < w and u(y)≥v(p,w)u(y) \ge v(p, w).

    Local nonsatiation gives a nearby feasible bundle with even higher uu, contradicting the maximality of v(p,w)v(p, w).

    Hence equality holds.