Source: https://www150.statcan.gc.ca/n1/pub/11-633-x/11-633-x2019004-eng.htm
Timestamp: 2019-10-22 11:16:54
Document Index: 197348191

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﻿ Estimating the Effect of Changing Canada-US Border Costs on North American Trade Patterns and Expenditures: Detailed Methodology
Estimating the Effect of Changing Canada-US Border Costs on North American Trade Patterns and Expenditures: Detailed Methodology
by W. Mark Brown, Afshan Dar-Brodeur and Jay Dixon
Analytical Studies Branch No. 023
2 The gravity model
3.3 Network distance
4 Estimating the structural gravity model
4.1 Estimation method
5 Gravity model estimates
6 General equilibrium PPML
6.1	Fixed effects and multilateral resistances
6.2	Trade costs, output and expenditure
6.3	Counterfactual scenarios: an illustration
World trade has expanded since the Second World War, facilitated by the ratification of multilateral and regional trade agreements. One of the earliest such agreements was the 1988 Canada — MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfKttLearuGrYvMBJHgitnMCPbhDG0evam XvP5wqSXMqHnxAJn0BKvguHDwzZbqegqvATv2CG4uz3bIuV1wyUbqe dmvETj2BSbqegm0B1jxALjhiov2DaebbnrfifHhDYfgasaacH8rrpk 0dbbf9q8WrFfeuY=Hhbbf9v8vrpy0dd9qqpae9q8qqvqFr0dXdHiVc =bYP0xH8peuj0lXxfrpe0=vqpeeaY=brpwe9Fve9Fve8meaacaGacm GadaWaaiqacaabaiaafaaakeaaryqqYLwySbacgaqcLbwaqaaaaaaa aaWdbiaa=rbiaaa@40D2@ United States Free Trade Agreement, to which Mexico acceded in 1994 to create the North American Free Trade Agreement (NAFTA). It was renegotiated in 2018. These agreements originally focused on disciplining tariffs and quotas applied to goods crossing the border. The most recent negotiations, while addressing market access in certain industries, also focused more on other burdens associated with administrative borders.Note
At the same time, Canadian provinces have been negotiating to further reduce trade barriers between them by updating the 1995 Agreement on Internal Trade (AIT) with the signing of the Canadian Free Trade Agreement (CFTA) in 2017. There are no tariffs or quotas levied at the borders separating provinces. The main impediments are thought instead to be caused by differences in regulatory frameworks and government procurement practices, and amount to about a 7% tariff equivalent (Bemrose, Brown and Tweedle 2017).
Frictions caused by red-tape and delays at borders, regulatory differences, or uncertainty over future policies, are commonly referred to as non-tariff barriers (NTBs). Unlike traditional trade policies like tariffs and quotas that are easy to identify and measure directly, frictions that range from red tape and border-related delivery delays, to divergent regulations and firms’ uncertainty about how policies will evolve, are not. The average bilateral costs of both tariff and non-tariff barriers can, however, be estimated indirectly by applying the gravity model framework to suitable data.
Trade frictions generated by the Canada-United States border have already been the subject of extensive research using the gravity model. The seminal work by McCallum (1995) on Canada and United States trade pointed to an extraordinarily large border effect. But the literature’s subsequent estimates of border frictions have declined as researchers have taken advantage of refinements to theory, measurement and estimation methods. These refinements include Anderson and van Wincoop’s (2003) incorporation of “multilateral resistance” terms to accommodate regional differences in access to and competition from global markets. The “structural” gravity model imbues the estimation with a general equilibrium structure that summarizes the ability of a region to generate and absorb trade from all other potential trading partners.
More recent work has suggested that further refinements are needed to accurately estimate border costs. Much of the emphasis has been on how to deal with the paucity of detail in available data. Trade flows are often measured at an aggregated level, between nations or large sub-national units, like provinces or states. But the level of geographic aggregation used in estimation matters, with higher levels of aggregation often biasing border estimates upwards. Hillberry and Hummels (2008) uses geographically detailed (i.e., zip code level) United States data to show that when the size of regions is reduced to the sub-state level the state borders’ effects on inter-state trade found with more aggregate data vanish entirely. Similarly, Bemrose, Brown and Tweedle 2017 found that smaller and more geographically uniform regions are associated with smaller estimated provincial border effects in Canada, although they are not eliminated.
This methodological note describes how to estimate the costs that administrative borders impose on Canada-United States trade using recently constructed data at Statistics Canada. A structural gravity model is applied to data from the Surface Transportation File (STF). The STF was built from shipping records to measure domestic trade between detailed locations within Canada and between the United States and Canada. It is augmented for this paper with the 2012 United States Commodity Flow Survey (CFS) to produce a data set that measures trade among 201 comparable Canadian and United States regions in year 2012. The combined data can measure the average costs of Canada-United States and provincial borders simultaneously. We are unaware of any work estimating the Canada-United States border effect at such a fine-grained geography.
The average tariff equivalents are useful to illustrate the effect of trade frictions on Canada-United States bilateral trade. But changing international border costs also affect domestic trade patterns as firms shift between domestic and international markets. Together these first- and second-order impacts give a fuller picture of the economic significance of changing international trade costs.Note Anderson, Larch and Yotov (2018) show how, using counterfactual scenarios, the structural gravity model allows for the direct and indirect impacts of a change in bilateral trade costs to be quantified. We present the application of the structural gravity model in this paper and use it to illustrate the aggregate outcomes of counterfactual changes to Canada-United States border costs.
The following section discusses the gravity model. Section 3 covers the construction of the data and highlights the advantages and limitations of using detailed shipment data from different sources. Section 4 discusses the model’s empirical implementation, including the need to adjust the estimating equation to allow for features of the data. Results for Canada-United States and provincial border effects are presented in Section 5. A methodology for elaborating on the general equilibrium effects with an example of results are discussed in Section 6. For a more detailed description of these results, see Brown, Dar-Brodeur and Dixon (2019).
In the gravity model framework, bilateral trade is analysed by analogy with Newtonian gravity: trade flows between two regions are assumed to be an increasing function of their economic sizes and inversely related to the distance between them. Trade flows not explained by these variables are attributed to other trade “frictions”. When applied to measuring administrative borders, the model estimates the degree to which interregional trade frictions must exceed domestic ones.
Anderson and van Wincoop’s (2003, 2004) showed that in addition to size and proximity, gravity models should also incorporate regions’ relationships with third parties. These models are often referred to as “structural” gravity, of which there are many varieties in the literature.Note Each imposes different conditions on consumers or producers, leading to different interpretations of the parameters, they all result in common expressions for the equilibrium value of bilateral exports, X i j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaamiwamaaBa aaleaacaWGPbGaamOAaaqabaaaaa@38DB@ , from geographical location i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGPbaaaa@3704@ to location j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGQbaaaa@3705@ :
X ij = ( t ij Π i P j ) −ϵ Y i E j , (1) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGybWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaak8qacqGH 9aqpdaqadaWdaeaapeWaaSaaa8aabaWdbiaadshapaWaaSbaaSqaa8 qacaWGPbGaamOAaaWdaeqaaaGcbaWdbiabfc6aq9aadaWgaaWcbaWd biaadMgaa8aabeaak8qacaWGqbWdamaaBaaaleaapeGaamOAaaWdae qaaaaaaOWdbiaawIcacaGLPaaapaWaaWbaaSqabeaapeGaeyOeI0Ye fv3ySLgznfgDOfdaryqr1ngBPrginfgDObYtUvgaiuaacqWF1pG8aa GccaWGzbWdamaaBaaaleaapeGaamyAaaWdaeqaaOWdbiaadweapaWa aSbaaSqaa8qacaWGQbaapaqabaGcpeGaaiilauaabeqabyaaaaqaaa qaaaqaaaqaaaqaaaqaaiaacIcacaaIXaGaaiykaaaaaaa@5905@
P j −ϵ = ∑ i ( t ij Π i ) −ϵ Y i , (2) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGqbWdamaaDaaaleaapeGaamOAaaWdaeaapeGaeyOeI0Yefv3y SLgznfgDOfdaryqr1ngBPrginfgDObYtUvgaiuaacqWF1pG8aaGccq GH9aqpdaaeqbWdaeaapeWaaeWaa8aabaWdbmaalaaapaqaa8qacaWG 0bWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaaaOqaa8qacqqHGo aupaWaaSbaaSqaa8qacaWGPbaapaqabaaaaaGcpeGaayjkaiaawMca a8aadaahaaWcbeqaa8qacqGHsislcqWF1pG8aaaapaqaa8qacaWGPb aabeqdcqGHris5aOGaamywa8aadaWgaaWcbaWdbiaadMgaa8aabeaa k8qacaGGSaGaaCzcaiaaxMaacaWLjaGaaiikaiaaikdacaGGPaaaaa@5C1D@
Π i −ϵ = ∑ j ( t ij P j ) −ϵ E j . (3) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqqHGoaupaWaa0baaSqaa8qacaWGPbaapaqaa8qacqGHsisltuuD JXwAK1uy0HwmaeHbfv3ySLgzG0uy0Hgip5wzaGqbaiab=v=aYdaaki abg2da9maaqafapaqaa8qadaqadaWdaeaapeWaaSaaa8aabaWdbiaa dshapaWaaSbaaSqaa8qacaWGPbGaamOAaaWdaeqaaaGcbaWdbiaadc fapaWaaSbaaSqaa8qacaWGQbaapaqabaaaaaGcpeGaayjkaiaawMca a8aadaahaaWcbeqaa8qacqGHsislcqWF1pG8aaaapaqaa8qacaWGQb aabeqdcqGHris5aOGaamyra8aadaWgaaWcbaWdbiaadQgaa8aabeaa k8qacaGGUaGaaCzcaiaaxMaacaWLjaGaaiikaiaaiodacaGGPaaaaa@5C0E@
The variables Y i ( = ∑ j X i j ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGzbWdamaaBaaaleaapeGaamyAaaWdaeqaaOWdbiaacIcacqGH 9aqpdaaeqbWdaeaapeGaamiwa8aadaWgaaWcbaWdbiaadMgacaWGQb aapaqabaaabaWdbiaadQgaaeqaniabggHiLdGccaGGPaaaaa@4109@ and E j ( = ∑ i X i j ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGfbWdamaaBaaaleaapeGaamOAaaWdaeqaaOWdbiaacIcacqGH 9aqpdaaeqbWdaeaapeGaamiwa8aadaWgaaWcbaWdbiaadMgacaWGQb aapaqabaaabaWdbiaadMgaaeqaniabggHiLdGccaGGPaaaaa@40F5@ are the values of location i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGPbaaaa@3704@ ’s total output and location j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGQbaaaa@3705@ ’s total expenditure (on goods and services to/from all locations, including themselves), respectively. The variable tij is the bilateral trade costs between i and j. The parameter − ϵ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqGHsisltuuDJXwAK1uy0HwmaeHbfv3ySLgzG0uy0Hgip5wzaGqb aiab=v=aYdaa@42FC@ is the elasticity of trade with respect to trade costs (or more commonly, the trade cost elasticity).Note
Depending on the underlying model, the trade cost elasticity reflects one or more of the heterogeneity of consumer preferences, scale economies, or the fixed costs of exporting. In the case of supply-side models, it reflects the (Frechet or Pareto) dispersion of firms’ productive efficiency.
The key feature distinguishing the structural gravity model from its earlier forms is the introduction of “multilateral resistance” (MR) terms, variables Π i MathType@MTEF@5@5@+= feaagKart1ev2aqaMTbvLHfij5gC1rhimfMBNvxyNvgaCbvAFTxA9b WexLMBbXgBcf2CPn2qVrwzqf2zLnharuavP1wzZbItLDhis9wBH5ga rmWu51MyVXgaruWqVvNCPvMCG4uz3bqee0evGueE0jxyaibaieYlNi =xH8yiVC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbbG8FasP YRqj0=yi0dXdbba9pGe9xq=JbbG8A8frFve9Fve9Ff0dmeaabaqaci GacaGaaeqabaWaaeaaeaaakeaaqaaaaaaaaaWdbiabfc6aq9aadaWg aaWcbaWdbiaadMgaa8aabeaaaaa@42AD@ and P j MathType@MTEF@5@5@+= feaagKart1ev2aqaMLbvLHfij5gC1rhimfMBNvxyNvgaq91EQ1hatC vAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhiov2DGi1BTfMBaeXa tLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4rNCHbGeaGqiVCI8Ff YJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfeaY=biLkVc Lq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr0=vqpWqaaeaabiGaci aacaqabeaadaqaaqaaaOqaaabaaaaaaaaapeGaamiua8aadaWgaaWc baWdbiaadQgaa8aabeaaaaa@413F@ , which are the solutions to the non-linear system of 2N Equations (2) and (3), subject to a normalization.Note
The first term is referred to as region i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaamyAaaaa@36E3@ ’s outward multilateral resistance (OMR) and the second term as region j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaamOAaaaa@36E4@ ’s inward multilateral resistance (IMR). These terms account for the fact that bilateral trade flows are not only affected by trade frictions between the two regions, but also by their relative positions with respect to all other potential trading partners. As described by Anderson and Yotov (2010), the OMRs can be interpreted as measure of the trade cost incidence on sellers as they bring goods to a hypothetical world market. Similarly, the IMRs summarize the incidence of trade costs on consumers receiving goods from the world market. In models derived from the constant elasticity of substitution (CES) utility function, the IMRs are also the regional consumer price indexes. Economic geographers often refer to OMRs as an index of exporting regions’ market access and the IMRs as indexes of competition in the destination region. Together, the multilateral resistance terms account for the indirect effect that multilateral trading relationships have on bilateral trade flows.
The literature has identified two data-related issues that may influence border effect estimates. Due to data limitations, many papers are confined to analysing trade between highly aggregated/heterogeneous regions like countries or provinces/states. The distance goods travel are approximated by the great circle distance between administrative or commercial capitals, or the regions’ economic or demographic centroids. Gravity researchers have observed that estimated border frictions can be influenced by heterogeneity in internal regional trade costs associated with trading regions of differing sizes (Coughlin and Novy, 2016). In addition, standard distance measures may bias the estimation of border frictions, because trade flows tend to be short distance and so are likely overestimated (Head and Mayer 2009).
The two different data sources used in this paper address these concerns by using a relatively homogeneous set of sub-provincial/state regions and a more accurate measure of the distance that goods travel between them. The following subsections discuss the construction of the data, their advantages and potential limitations.
The data are derived from two different sources. Canadian domestic and cross-border trade flows are derived from Statistics Canada’s Surface Transportation File (STF). United States internal trade comes from the United States 2012 Commodity Flow Survey (CFS). They include shipments measured in terms of commodity, tonnage, value, network distance shipped, and by detailed origin and destination. The precision of the origins and destinations allows for the measurement of trade flows between 201 sub-provincial/state areas.
While the STF covers the major modes of transportation used by most commodities, it does not cover air, marine and goods moved by pipeline, or own-account trucking. To account for these limitations, shipment values are weighted to ensure they add to inter-/intra-provincial trade totals by commodity for domestic trade reported by the provincial supply-use (input-output) tables. Similarly, cross-border shipments are weighted to add to provincial-United States exports/imports by commodity, again using the provincial supply-use tables.Note Hence, domestic and cross-border flows add to known totals. This approach assumes that the patterns of trade followed by modes not covered follow those generated by the for-hire trucking and rail.Note
The exception is commodities produced by the energy industry. Although energy products are also shipped by rail and truck, they are primarily moved by pipeline. Since pipelines are not included in the STF, there is not enough information in the file to accurately attribute energy flows down to the sub-provincial level. The energy sector is therefore excluded from this analysis.
The STF by itself is insufficient to measure the Canada-United States border effect. The appropriate comparison group to cross-border trade is domestic trade in both countries. The United States domestic trade flows are not included in the STF, and so comparable shipment-level data from the 2012 CFS are used to fill the gap.Note CFS trade flows are scaled to United States gross output as in Anderson and van Wincoop (2003), and the oil and gas industry is excluded.Note
The CFS is a quinquennial survey, and only has publicly available microdata for 2012, while the STF is based on annual data from 2004-2012. The combined data is restricted to the year 2012 to generate a shipment-level file for North America. The shipments are aggregated to generate intra- and inter-regional trade on a North America-wide basis, taking advantage of the (relatively) detailed origins and destinations reported on each file.
While the STF and CFS are broadly comparable, there are some important differences to be kept in mind when using the combined information for analytical purposes. First, domestic STF flows are benchmarked to the provincial supply-use tables estimating origin and final use of commodities across provinces. As a result, the domestic portion of the STF is converted from a ‘logistics file’ that measures where goods are picked up and dropped off to a quasi-‘trade file’, tracking where they are made and used. The CFS and cross-border trade from the STF remain logistics-based. Bemrose, Brown and Tweedle (2017) show that benchmarking stretches trade flows across space, relative to un-benchmarked logistics flows.
Second, both the STF and CFS derive trade flows from shipping records, but the STF obtains them from trucking firms (‘carrier-based’ survey), while the CFS obtains them from establishments that generate the shipments (‘shipper-based’ survey), leading to potential differences in coverage. The truck-based shipments in STF are derived from the Trucking Commodity Origin Destination (TCOD) Survey, which does not include private trucking. The CFS, on the other hand, does. If private trucking is a significant proportion of short distance flows, these flows will be better represented in the CFS than the STF. Finally, the CFS measures distances between zip codes, while the STF uses much more spatially detailed postal codes.
One additional factor complicates the calculation of a full set of regional flows and their respective distances below the provincial/state level. While truck shipments to and from the United States are reported by zip code on the STF file, only the state of destination/origin are reported for rail shipments. Interregional rail shipments between Canada and the United States were allocated to sub-state areas using the value-weighted share of corresponding truck exports/imports. While the pattern of rail and truck shipments at the sub-state level are likely not perfectly correlated, there should be a strong correspondence.Note Hence, any error introduced is expected to have a relatively small effect on the aggregate flows.
The gravity model, by construction, measures inter-regional relative to average intra-regional trade costs. This construction presents no issues when regions are homogeneous (i.e., they have roughly the same size and geography). However, in most data, the units of analysis have different sizes and thus different, usually unobservable, internal trade costs. Larger regions naturally have higher internal costs than smaller ones, and yet estimation often treats them both as dimensionless points in space. Coughlin and Novy (2016) show that the size-related heterogeneity can bias border effect estimates.Note
The data allow for two sub-national geographies to define trading units. The first is the province/state geography that the literature has relied upon. However, in the light of Coughlin and Novy (2016)’s findings, a second more fine-grained geography is also used. It is based on the CFS’s division of states into metropolitan and non-metropolitan (MA/non-MA) areas. While there is no perfect analogue in Canada, STF-based flows can be aggregated by Economic Regions (ERs) that are comparable in size to the United States MA/non-MA geography (see Map 1).Note Furthermore, ERs and MA/non-MA boundaries respect provincial and state borders in the same way.
There are some differences between ERs and MA/non-MAs. ERs are not purely metropolitan-based. Hence, while there is a tendency for them to roughly follow metropolitan boundaries (e.g., Edmonton and Calgary), other metropolitan areas (e.g., the Toronto metropolitan region) are composed of several ERs. Furthermore, the United States geography treats the rest of each state as a non-metropolitan residual, while the “non-metropolitan” portions of provinces may be split into multiple ERs (see Map 1). Still, there is enough commonality to treat them as compatible. To simplify the discussion both geographies will hereafter be referred to as ERs.
Long description for Map 1 ﻿
The title of Map 1 is “Economic regions of Canada and the United States.”
Map 1 shows the North American continent, except for the western part of Alaska, Greenland, and the southern part of Mexico. There are no labels indicating countries, regions or other geographical features on the map. The northern part of Mexico is shaded in grey. The water features are shaded in blue. The northern part of Canada (Nunavut, Northwest Territories and the Yukon) are shaded in light grey. The continental United States and the 10 Canadian provinces are white.
The map legend is located on the lower right corner of the map. It is a white square with a border in black colour. In this white square, there is a smaller square delineated with a thin black line, with “Provincial and state borders” written beside it in black. Below it is a square of same dimensions delineated with a thin light purple line, with “Economic Regions” written beside it in black. Below this second square is a square of the same dimensions, shaded in light grey colour, with “Regions not in the analysis” written beside it in black. This last square has no borders.
Below the legend is the scale for the map. The scale is a horizontal thick bar with alternating black and light blue colour. The scale extends from 0 to 1,000 kilometres, with graduations shown at 0, 250, 500 and 1,000 kilometres. It is about the same width as the map legend.
The provincial and state borders are shown on the map for all of Canada and the United States. The economic region borders are shown on the map for the continental United States and for the ten Canadian provinces, which are in white, because only these regions are part of the study.
The note and source for the map are as follows:
Note: Economic regions refer to their namesake in Canada and to the metropolitan/non-metropolitan geography used in the U.S. Commodity Flow Survey.
Sources: Statistics Canada,
Another factor potentially biasing border effect estimates is the mis-measurement of shipping distances (Head and Mayer, 2009). Most research is limited to using great circle distances between arbitrary points within trading areas. These measures often mischaracterize the distance goods traded between regions actually travel. The STF and CFS allow the derivation of the network distances that more accurately reflect the origins, destinations and journeys goods can be expected to take.Note However, the network distances used here are constructed using two sources that differ in their methodologies, and the differences between them may bias border effect estimates. It is thus important to understand how much they differ when comparing cross-border to domestic trade.
Table 1 shows the distribution of distances between ERs for domestic Canadian and cross-border trade derived from the STF and domestic United States trade derived from the CFS. For domestic trade, the percentile distribution of distances are reported for intra-ER, distances between ERs within the same province/state, and between different provinces/states. Regardless of whether distances are intra- or inter-ER, the two files generate the same distribution of shorter distance flows. It is only at the 90th and especially the 99th percentile of ER pairs that we observe much longer distances shipped in Canada, reflecting its larger size and more dispersed population. Otherwise, the STF and CFS generate broadly comparable distributions of within and between ER distances.
Cross-border distances tend to be longer than domestic flows. There are no cross-border pair distances below 150 kilometres. Since cross-border flows are much more heavily weighted towards longer distance shipments (greater than 400 km), any difference in the effect of distance on trade flows stemming from the construction of the data may bias the estimated border effect derived from the model. This potential bias can be compensated for in the specification of the econometric model. One possible remedy is discussed in Section 4.
Network distances between Economic Regions by trade type and geography
This table displays the results of Network distances between Economic Regions by trade type and geography. The information is grouped by Trade Type (appearing as row headers), Percentile, Median, p1, p10, p25, p75, p90 and p99, calculated using kilometers units of measure (appearing as column headers).
Intra-ER
60 10 20 40 90 150 710
390 50 130 220 670 940 1,610
2,550 310 760 1,280 3,960 4,980 6,240
30 20 20 20 60 70 120
230 60 130 160 350 500 880
1,780 200 640 1,100 2,780 3,840 4,860
2,690 430 1,060 1,750 3,720 4,660 5,860
Notes: Reported are the percentiles of the mean shipment-based network distance within and between Economic Regions (ERs) by trade type (i.e., Canada-U.S, Canadian domestic, and United States domestic) and, for domestic distances, geography. The latter includes intra-ER and ER to ER distances within provinces/states and between provinces and states. Distances are rounded to the nearest 10 kilometers.
The estimation equation corresponding to the model for bilateral trade described in Section 2 is often expressed as:
X ij =exp( T ij B+ π i + χ j ) ξ ij . (4) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGybWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaak8qacqGH 9aqpciGGLbGaaiiEaiaacchacaGGOaGaaCiva8aadaWgaaWcbaWdbi aahMgacaWHQbaapaqabaGcpeGaaCOqaiabgUcaRiabec8aW9aadaWg aaWcbaWdbiaadMgaa8aabeaak8qacqGHRaWkcqaHhpWypaWaaSbaaS qaa8qacaWGQbaapaqabaGcpeGaaiykaiabe67a49aadaWgaaWcbaWd biaadMgacaWGQbaapaqabaGcpeGaaiOlaiaaxMaacaWLjaGaaCzcai aacIcacaaI0aGaaiykaaaa@533F@
The link between the estimating equation to Equation (1) can be seen by defining the natural log of bilateral trade costs, ln ( t i j − ϵ ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qaciGGSbGaaiOBaiaacIcacaWG0bWdamaaDaaaleaapeGaamyAaiaa dQgaa8aabaWdbiabgkHiTmrr1ngBPrwtHrhAXaqeguuDJXwAKbstHr hAG8KBLbacfaGae8x9dipaaOGaaiykaaaa@4984@ , as the multiplication of the logarithmically transformed determinants of trade costs by their trade elasticities, T i j B MathType@MTEF@5@5@+= feaagKart1ev2aqaMvcvLHfij5gC1rhimfMBNvxyNvgaC1wy0HMyMT hvFTxAQ1hic1hatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLnhi ov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr4r NCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9 q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr0= vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaapeGa aCiva8aadaWgaaWcbaWdbiaahMgacaWHQbaapaqabaGcpeGaaCOqaa aa@47C3@ (boldface denotes vectors), π i = − ln ( Π i − ϵ Y i ) MathType@MTEF@5@5@+= feaagKart1ev2aqaMjfvLHfij5gC1rhimfMBNvxyNvgaCbxAFTxA9b spG0ciCXMBGWfBLzgDOWLzYf2y7XfuP91EP1Nx71cxLb3CPX2BU1xF 7L1x7LwF9XLCPDgA0LcatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuL wBLnhiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqt ubsr4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk 0xbba9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr 0=vr0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaa aapeGaeqiWda3damaaBaaaleaapeGaamyAaaWdaeqaaOWdbiabg2da 9iabgkHiTiGacYgacaGGUbWaaeWaa8aabaWdbmaalaaapaqaa8qacq qHGoaupaWaa0baaSqaa8qacaWGPbaapaqaa8qacqGHsisltuuDJXwA K1uy0HwmaeHbfv3ySLgzG0uy0Hgip5wzaGqbaiab=v=aYdaaaOWdae aapeGaamywa8aadaWgaaWcbaWdbiaadMgaa8aabeaaaaaak8qacaGL OaGaayzkaaaaaa@6FD2@ and χ j = − ln ( P j − ϵ E j ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqaHhpWypaWaaSbaaSqaa8qacaWGQbaapaqabaGcpeGaeyypa0Ja eyOeI0IaciiBaiaac6gadaqadaWdaeaapeWaaSaaa8aabaWdbiaadc fapaWaa0baaSqaa8qacaWGQbaapaqaa8qacqGHsisltuuDJXwAK1uy 0HwmaeHbfv3ySLgzG0uy0Hgip5wzaGqbaiab=v=aYdaaaOWdaeaape Gaamyra8aadaWgaaWcbaWdbiaadQgaa8aabeaaaaaak8qacaGLOaGa ayzkaaaaaa@5049@ . In cross-sectional data, the last two terms can be incorporated in the estimation as directional exporter and importer fixed effects accounting for the multilateral resistance terms and the relative economic size of regions i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaamyAaaaa@36E3@ and j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaamOAaaaa@36E4@ .Note The ξ ij MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaeqOVdG3aaS baaSqaaiaadMgacaWGQbaabeaaaaa@39C1@ is a random error term that captures un-modelled trade costs and allows for errors in data construction. When implemented, the estimation must exclude both the intercept and a fixed effect (importer or exporter) or two fixed effects (an importer and an exporter) to avoid perfect collinearity. To make interpretation of the fixed effects in the Section 5 simpler, we forgo an intercept and exclude the importer dummy for Ontario in the province/state regressions, and for the Greater Toronto area when the ER geography is used. We define bilateral trade costs as:
T ij B=ln d ij B d + β BR CUB R ij + β PBR PB R ij + β SBR SB R ij . (5) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWHubWdamaaBaaaleaapeGaaCyAaiaahQgaa8aabeaak8qacaWH cbGaeyypa0JaaCiBaiaah6gacaWHKbWdamaaBaaaleaapeGaaCyAai aahQgaa8aabeaak8qacaWHcbWdamaaBaaaleaapeGaaCizaaWdaeqa aOWdbiabgUcaRiabek7aI9aadaWgaaWcbaWdbiaadkeacaWGsbaapa qabaGcpeGaam4qaiaadwfacaWGcbGaamOua8aadaWgaaWcbaWdbiaa dMgacaWGQbaapaqabaGcpeGaey4kaSIaeqOSdi2damaaBaaaleaape GaamiuaiaadkeacaWGsbaapaqabaGcpeGaamiuaiaadkeacaWGsbWd amaaBaaaleaapeGaamyAaiaadQgaa8aabeaak8qacqGHRaWkcqaHYo GypaWaaSbaaSqaa8qacaWGtbGaamOqaiaadkfaa8aabeaak8qacaWG tbGaamOqaiaadkfapaWaaSbaaSqaa8qacaWGPbGaamOAaaWdaeqaaO Wdbiaac6cacaWLjaGaaCzcaiaaxMaacaGGOaGaaGynaiaacMcaaaa@65B3@
The first term on the right-hand side captures the non-linear effect of distance, discussed in more detail at the end of this sub-section. The main focus of this paper is the trade frictions induced by the intercession of administrative borders. In Equation (5) the binary variables take a value of one if regions lie on either side of the Canada-United States ( C U B R MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaam4qaiaadw facaWGcbGaamOuaaaa@3935@ ), a provincial ( P B R MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaamiuaiaadk eacaWGsbaaaa@3868@ ) or a state border ( S B R MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaam4uaiaadk eacaWGsbaaaa@386B@ ), respectively, and zero otherwise. The exponentiated coefficient for the Canada-United States border dummy exp ( β C U B R ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaciyzaiaacI hacaGGWbGaaiikaiabek7aInaaBaaaleaacaWGdbGaamyvaiaadkea caWGsbaabeaakiaacMcaaaa@3F40@ and the trade elasticity can be used to calculate a tariff equivalent for the border’s impact on bilateral trade. The tariff equivalent summarizes the impact of tariffs and “tariffies” any border-related non-tariff barriers.Note
In much of the literature, trade costs of exporting from region i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGPbaaaa@3670@ to region j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGQbaaaa@3671@ are assumed to be a log-linear function of distance between them. While this assumption is likely innocuous when modelling trade over long distances, it may be problematic when using a fine geographic breakdown, as trade involves fixed logistical and search costs that must be covered to move goods any significant distance. These outlays inflate per km costs at short distances, but their impact declines rapidly as they are spread over longer distances (see Behrens and Brown (2018)). This non-linearity in trade costs may be more pronounced in estimations that include a large number of short distance flows within regions and between near neighbours (i.e., between ERs within provinces/states).Note
In order to accommodate potential non-linearities, as well as compensating for differences in the underlying data sources that make up our sample, the estimating Equation (4) includes a spline over distance, ( d i j MathType@MTEF@5@5@+= feaagKart1ev2aqaMncvLHfij5gC1rhimfMBNvxyNvgaC1wy0HMyMT hzFTxAQ1xFamXvP5wqSXMqHnxAJn0BKvguHDwzZbqefqvATv2CG4uz 3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhiov2DaebbnrfifHhDYf gasaacH8YjY=vipgYlh9vqqj=hEeeu0xXdbba9frFj0=OqFfea0dXd d9vqai=hGuQ8kuc9pgc9q8qqaq=dir=f0=yqaiVgFr0xfr=xfr=xb9 adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacaWH KbWdamaaBaaaleaapeGaaCyAaiaahQgaa8aabeaaaaa@469A@ ):
ln d ij B d =1{ d ij < d ¯ } β d ¯ ln( d ij )+ ∑ d ij =d ∑ f ij =f β df ln( d ij ), (6) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWHSbGaaCOBaiaahsgapaWaaSbaaSqaa8qacaWHPbGaaCOAaaWd aeqaaOWdbiaahkeapaWaaSbaaSqaa8qacaWHKbaapaqabaGcpeGaey ypa0JaaGymaiaacUhacaWGKbWdamaaBaaaleaapeGaamyAaiaadQga a8aabeaak8qacqGH8aapceWGKbGbaebacaGG9bGaeqOSdi2damaaBa aaleaapeGabmizayaaraaapaqabaGcpeGaciiBaiaac6gacaGGOaGa amiza8aadaWgaaWcbaWdbiaadMgacaWGQbaapaqabaGcpeGaaiykai abgUcaRmaaqafapaqaa8qadaaeqbWdaeaapeGaeqOSdi2damaaBaaa leaapeGaamizaiaadAgaa8aabeaaaeaapeGaamOza8aadaWgaaadba WdbiaadMgacaWGQbaapaqabaWcpeGaeyypa0JaamOzaaqab0Gaeyye IuoaaSWdaeaapeGaamiza8aadaWgaaadbaWdbiaadMgacaWGQbaapa qabaWcpeGaeyypa0Jaamizaaqab0GaeyyeIuoakiGacYgacaGGUbGa aiikaiaadsgapaWaaSbaaSqaa8qacaWGPbGaamOAaaWdaeqaaOWdbi aacMcacaGGSaGaaCzcaiaaxMaacaWLjaGaaiikaiaaiAdacaGGPaaa aa@6EE4@
where for d i j ≥ d ¯ MathType@MTEF@5@5@+= feaagKart1ev2aqaMzcvLHfij5gC1rhimfMBNvxyNvgaK91EPPwFGW 1zLbcxIfMC7rwFamXvP5wqSXMqHnxAJn0BKvguHDwzZbqefqvATv2C G4uz3bIuV1wyUbqedmvETj2BSbqefm0B1jxALjhiov2DaebbnrfifH hDYfgasaacH8YjY=vipgYlh9vqqj=hEeeu0xXdbba9frFj0=OqFfea 0dXdd9vqai=hGuQ8kuc9pgc9q8qqaq=dir=f0=yqaiVgFr0xfr=xfr =xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qa caWGKbWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaak8qacqGHLj YSceWGKbGbaebaaaa@4A01@ parameter estimates are allowed to vary across trade types f MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGMbaaaa@366D@ such that:
f ∈ { within Canada, Canada-US, within US} . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape GaamOzaiabgIGiolaacUhacaqG3bGaaeyAaiaabshacaqGObGaaeyA aiaab6gacaqGGaGaae4qaiaabggacaqGUbGaaeyyaiaabsgacaqGHb GaaeilaiaabccacaqGdbGaaeyyaiaab6gacaqGHbGaaeizaiaabgga caqGTaGaaeyvaiaabofacaqGSaGaaeiiaiaabEhacaqGPbGaaeiDai aabIgacaqGPbGaaeOBaiaabccacaqGvbGaae4uaiaab2hacaqGUaaa aa@58FE@
For regressions at the provinces and state levels, d ¯ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape Gabmizayaaraaaaa@370D@ equals150 kilometres, while for regressions on ER flows, d ¯ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape Gabmizayaaraaaaa@370D@ equals 50 kilometres — MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfKttLearuGrYvMBJHgitnMCPbhDG0evam XvP5wqSXMqHnxAJn0BKvguHDwzZbqegqvATv2CG4uz3bIuV1wyUbqe dmvETj2BSbqegm0B1jxALjhiov2DaebbnrfifHhDYfgasaacH8rrpk 0dbbf9q8WrFfeuY=Hhbbf9v8vrpy0dd9qqpae9q8qqvqFr0dXdHiVc =bYP0xH8peuj0lXxfrpe0=vqpeeaY=brpwe9Fve9Fve8meaacaGacm GadaWaaiqacaabaiaafaaakeaaryqqYLwySbacgaqcLbwaqaaaaaaa aaWdbiaa=rbiaaa@40D2@ below these distances, trade flows are exclusively intra-regional. Constraining the effect of the shortest distances to be the same across regions essentially imposes the same distance-related intra-regional trade costs across the two countries. The other spline segments are represented by distance class set d MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGKbaaaa@366B@ :
d∈{ d min , 500 - 999, 1,000 - 1,999, 2,000 or greater}, (7) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGKbGaeyicI4Saai4EaiaahsgapaWaaSbaaSqaa8qacaWHTbGa aCyAaiaah6gaa8aabeaak8qacaqGSaGaaeiiaiaabwdacaqGWaGaae imaiaabccacaqGTaGaaeiiaiaabMdacaqG5aGaaeyoaiaabYcacaqG GaGaaeymaiaabYcacaqGWaGaaeimaiaabcdacaqGGaGaaeylaiaabc cacaqGXaGaaeilaiaabMdacaqG5aGaaeyoaiaabYcacaqGGaGaaeOm aiaabYcacaqGWaGaaeimaiaabcdacaqGGaGaae4BaiaabkhacaqGGa Gaae4zaiaabkhacaqGLbGaaeyyaiaabshacaqGLbGaaeOCaiaac2ha caGGSaGaaCzcaiaaxMaacaWLjaGaaiikaiaaiEdacaGGPaaaaa@63E3@
d m i n = { 150 − 499 , for provinces and states , 50 − 149, 150 − 499 for ERs . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWHKbWdamaaBaaaleaapeGaaCyBaiaahMgacaWHUbaapaqabaGc peGaeyypa0Zaaiqaa8aabaqbaeaabiGaaaqaa8qacaaIXaGaaGynai aaicdacqGHsislcaqG0aGaaeyoaiaabMdacaGGSaaapaqaa8qacaqG MbGaae4BaiaabkhacaqGGaGaaeiCaiaabkhacaqGVbGaaeODaiaabM gacaqGUbGaae4yaiaabwgacaqGZbGaaeiiaiaabggacaqGUbGaaeiz aiaabccacaqGZbGaaeiDaiaabggacaqG0bGaaeyzaiaabohacaGGSa aapaqaa8qacaaI1aGaaGimaiabgkHiTiaabgdacaqG0aGaaeyoaiaa bYcacaqGGaGaaeymaiaabwdacaqGWaGaaeiiaiabgkHiTiaabccaca qG0aGaaeyoaiaabMdaa8aabaWdbiaabAgacaqGVbGaaeOCaiaabcca caqGfbGaaeOuaiaabohacaGGUaaaaaGaay5Eaaaaaa@6C58@
There are no international network distances of less than 150 kilometres in the data, so the effects of the shorter unconstrained distances only vary between within-country Canada and US flows.Note
Equation (4) has traditionally been estimated by taking the natural log and using ordinary least squares (OLS). However, Silva and Tenreyro (2006) show that this approach leads to biased estimates in the presence of heteroskedasticity, because the conditional mean of the log error term will generally not be independent of the covariates (a requirement of OLS estimation) unless strong assumptions are made about the distribution of ξ i j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGacaGaaiaabeqaamaabaabaaGcbaGaeqOVdG3aaS baaSqaaiaadMgacaWGQbaabeaaaaa@39C1@ .
Intuitively, as the value of trade flows approach zero, they can only vary in one direction (trade flows cannot be negative), whereas larger trade flows can vary upwards or downwards. Smaller regions that are farther apart being more likely to record flows that are near or at zero, where the log specification is undefined. The bias is thus a greater problem when considering smaller, more distant geographic aggregations. Silva and Tenreyro (2006) suggest dealing with heteroskedasticity by estimating (4) in its non-linear form using pseudo-maximum likelihood estimation. This approach has the added benefit of incorporating zero-valued flows as a matter of course. Among this class of estimators, they find that Poisson pseudo maximum likelihood (PPML) often yields the best results.Note Furthermore, PPML estimation has desirable properties that permit us to recover the multilateral resistance terms directly from the fixed effects (Fally 2015). These properties are important to accessing the model’s general equilibrium information, as discussed in Appendix A.
The results presented in Table 2 replicate specifications used in the existing literature, with trade aggregated to the province/state level and the effect of distance on trade constrained to be the same across trade types ( f MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGMbaaaa@366D@ ) and distance classes ( d MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGKbaaaa@366B@ ). Estimating the model using all trade [column (1)], including intraregional flows, produces a distance parameter of -1.182, which is somewhat stronger than the standard of -1 found in the literature (see Head and Mayer (2014)) and a Canada-United States border parameter estimate of -0.626, which is much weaker than generally found: Anderson and van Wincoop (2003) estimated a border coefficient border using 1993 data to be -1.65. Column (2) repeats the same model but with intra-province/state flows excluded. There are no qualitative differences in parameters (see Table 2) when intraregional flows are excluded. Due to differences with the literature in the underlying data, it is unclear what inferences should be drawn regarding the initial border effect estimate.
The distance estimates presented in columns (1) and (2) are constrained across trade types. Because the STF benchmarks Canada’s domestic flows to intra- and inter-provincial trade totals, it is expected that the effect of distance on Canadian domestic trade to be weaker than cross-border or United States domestic trade. Benchmarking has the effect of stretching flows by tracing the trade in goods from where they are made all the way to where they are used, rather than to a point along the logistics chain prior to a good’s final destination, as is the case with the United States data. This stretching gives the appearance that distance-related trade costs are lower in Canada. Columns (3), (4) and (5) of Table 2 show gravity regressions for Canada, United States and cross-border trade separately. The trade elasticity of distance for United States domestic trade is -1.140, while for Canadian domestic trade it is -0.773. Cross-border trade’s distance elasticity, at -0.96, is close to unity, as is often found in the international trade literature.
Since distance has a stronger estimated negative effect on United States trade than in the full model [see Column (2)], there will be a tendency for internal United States flows to be underestimated, biasing the border effect upwards (i.e., towards zero). Of course, the opposite holds true for Canadian trade, but because United States flows account for the vast majority of North America’s domestic trade, their effect will dominate border estimates. These differing distance parameter estimates suggest that the effect of distance needs to be allowed to vary across trade flow types.
Province-state regressions
This table displays the results of Province-state regressions All trade types, Cross-border (Canada-United States), Domestic United States and Domestic Canada (appearing as column headers).
Cross-border (Canada-United States)
-0.626Note ** -0.723Note ** Note ...: not applicable Note ...: not applicable Note ...: not applicable
0.061 0.055 Note ...: not applicable Note ...: not applicable Note ...: not applicable
-1.182Note ** -1.086Note ** -0.959Note ** -1.140Note ** -0.773Note **
0.013 0.020 0.049 0.020 0.049
3,364 3,306 960 2,256 90
Notes: All models utilize a Poisson-PML estimator and include fixed effects for origins and destinations. Columns (1) and (2) report parameter estimates with all trade types (cross-border and domestic) included in the estimation. Intra-regional (province or state) flows are included in the estimation for column (1) but excluded for column (2). Columns (3)–(5) report the model estimates for cross-border and United States and Canadian domestic trade, with intra-regional flows excluded.
The fully specified version of Equation (4) is presented in Table 3. Given the larger number of variables in the model, for ease of exposition we present the border and distance estimates separately. The first table presents the border coefficients from all regression models; the second presents the distance coefficients for our preferred model. The full model allows the effect of distance to vary by trade type ( f MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGMbaaaa@366D@ ) and distance ( d MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGKbaaaa@366B@ ) at the province/state level [columns (1) and (2)] and the ER level of spatial aggregation [columns (3) and (4)]. Relaxing the constraints addresses the error that results from differences in the construction of the STF and CFS portions of the data, as well as allowing for non-linearities in trade costs, which are expected to be particularly pronounced at lower levels of geographic aggregation.
In contrast to the results in Table 2, the province-state regressions with the unconstrained distances yield a stronger Canada-United States border effect. The border effect estimates with and without accounting for internal flows changes to -1.435 and -1.555, respectively. Comparing Tables 2 and 3 show that constraining the effect of distance across categories and trade types has a significant influence on the border effect.
Provincial and Economic Region border effect estimates across trade types, accounting for the non-linear effect of distance
This table displays the results of Provincial and Economic Region border effect estimates across trade types Province-State and Economic Region (appearing as column headers).
-1.435Note ** -1.555Note ** -1.568Note ** -1.434Note **
0.370 0.531 0.187 0.243
Note ...: not applicable Note ...: not applicable -0.576Note ** -0.785Note **
Note ...: not applicable Note ...: not applicable 0.126 0.127
Note ...: not applicable Note ...: not applicable -0.387Note ** -0.301Note **
Note ...: not applicable Note ...: not applicable 0.049 0.048
3,364 3,306 40,401 40,200
Notes: All models utilize a Poisson-PML estimator and include fixed effects for origins and destinations. The model also allows for the non-linear effect of distance on trade flows and for this effect above a minimum distance level d to vary by trade type: within Canada, Canada-United States, and within the United States. See Appendix Table 1 in the Appendix.
The border effects estimated using data at the ER level are, on the other hand, roughly the same in magnitude as the province/state level, but are estimated with greater precision.Note The Canada-United States border effect is -1.568 with and -1.434 and without intraregional flows. Assuming trade elasticity of ε = 7 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacqaH1oqzcqGH9a qpcaaI3aaaaa@38F0@ , the tariff equivalent for the former estimate is 30% and for the latter 27%. These estimates are, broadly speaking, in line with the various estimates in the literature.Note
The economic region regressions are also able to simultaneously measure provincial border effects of -0.576 and state borders -0.387 when internal flows are included. The provincial results are close to those found in Bemrose, Brown and Tweedle (2017) using the Canadian data from the STF alone and the same level of geographic aggregation.Note The exclusion of intra-regional trade flows [see Table 3, Column (4)], raises the provincial border effect in absolute terms. The state border estimates are negative and significant as well, but these are likely an artefact of CFS data and the level of geographic aggregation (Hillberry and Hummels, 2008). Bemrose, Brown and Tweedle (2017), using the Canadian equivalent of zip codes, find provincial border effects that are not qualitatively different than those estimated in this paper.
Our preferred estimates use ERs as the trading units and include intra-regional trade [Table 3, Column (3)]. The provincial border effect is the closest among the specifications to that estimated by Bemrose, Brown and Tweedle (2017) and the Canada-United States border effect is estimated with the most precision.
The distance coefficients for the preferred specification can be found in Table 4; the results for the other specifications can be found in Appendix B. Over the 500-3000 KM range, all flows (both domestic and international) are around one in absolute value, although the coefficients on United States domestic flows (from the CFS data) are generally higher than the Canada and Canada-United States flows (from the STF), likely reflecting differences in the source data. Second, there is clear evidence of a non-linearity of the effect of distance on the value of trade for Canadian domestic flows: the trade elasticities are high for very short distance flows (0-50 KM), reflecting fixed costs, and drop off over the 50-500 km range, before rising again beyond 500 KM and gently declining over longer distances. A similar, although more muted, pattern is evident for the United States domestic flows. There is large drop in the effect of distance on the value of trade for very long distance domestic flows (3000 km +), but not for international flows. It is unclear the degree to which these differences indicate data issues versus features of the economy.Note
Distance parameter estimates for Economic Regions, including intra-regional flows
This table displays the results of Distance parameter estimates for Economic Regions. The information is grouped by Trade type (appearing as row headers), Kilometers, 0 to
50, 50 to 150, 150 to 500, 500 to 1000, 1000 to 3000 and 3000 and more, calculated using coefficient units of measure (appearing as column headers).
-0.904Note ** -0.239 -0.393Note * -1.221Note ** -0.872Note ** -0.429Note *
-0.904Note ** -0.866Note ** -1.249Note ** -1.333Note ** -1.168Note ** 0.026
Note ...: not applicable Note ...: not applicable -0.950Note ** -1.033Note ** -1.134Note ** -1.020Note **
Notes: Reported are the distance parameters and significance levels for the model reported in column (3) in Table 3. The distance parameter estimates with standard errors for all four models presented in Table 4 are presented in Appendix Table 1 in the Appendix.
The previous section examined the average bilateral, first-order, estimates of Canada-United States border costs. But trade costs between two regions will change the opportunities for producers and consumers in their other potential trading partners, who will adjust accordingly. These general equilibrium, second order, adjustments will impact the relationships between all other trading regions. In other words, changes in, for example, costs at the Canada-United States border will also change the patterns of intra and inter-provincial/state trade. Welfare implications of any thinning or thickening of the border will depend not only on the bilateral impact on the two trading regions, but also on how patterns of trade respond across the continent.
The impact of a change in border costs can be illustrated by examining counterfactual scenarios. The most common counterfactuals explored in the literature are either frictionless borders or autarchy. These extreme scenarios can establish the total cost of the border or the benefits of liberalized trade. But the methodology can also be used to explore more plausible changes in trade costs. Two such plausible scenarios are discussed in Section 6.3 and the results are discussed in detail in Brown, Dar-Brodeur and Dixon (2019).
6.1 Fixed effects and multilateral resistances
Dekle, Eaton and Kortum (2008) show that, given data on output, expenditures and actual trade flows, the economic impact of counterfactual changes can be computed by recasting Equations (1) to (3) from levels to deviations from initial values and solving the transformed system for the anticipated adjustments in border costs. This method of calculating general equilibrium impacts is commonly referred to in the literature as exact hat algebra. Anderson, Larch and Yotov (2018) argue that another, equivalent, approach is to exploit the fixed effects π ^ i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfKttLearuGrYvMBJHgitnMCPbhDG0evam XvP5wqSXMqHnxAJn0BKvguHDwzZbqegqvATv2CG4uz3bIuV1wyUbqe dmvETj2BSbqegm0B1jxALjhiov2DaebbnrfifHhDYfgasaacH8rrpk 0dbbf9q8WrFfeuY=Hhbbf9v8vrpy0dd9qqpae9q8qqvqFr0dXdHiVc =bYP0xH8peuj0lXxfrpe0=vqpeeaY=brpwe9Fve9Fve8meaacaGacm GadaWaaiqacaabaiaafaaakeaadaWfGaqaaabaaaaaaaaapeGaeqiW dahal8aabeqaaGWaaiab=XJi+baakmaaBaaaleaadaWgaaadbaWdbi aadMgaa8aabeaaaSqabaaaaa@423B@ and χ ^ j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfKttLearuGrYvMBJHgitnMCPbhDG0evam XvP5wqSXMqHnxAJn0BKvguHDwzZbqegqvATv2CG4uz3bIuV1wyUbqe dmvETj2BSbqegm0B1jxALjhiov2DaebbnrfifHhDYfgasaacH8rrpk 0dbbf9q8WrFfeuY=Hhbbf9v8vrpy0dd9qqpae9q8qqvqFr0dXdHiVc =bYP0xH8peuj0lXxfrpe0=vqpeeaY=brpwe9Fve9Fve8meaacaGacm GadaWaaiqacaabaiaafaaakeaadaWfGaqaaabaaaaaaaaapeGaeq4X dmgal8aabeqaaGWaaiab=XJi+baakmaaBaaaleaapeGaamOAaaWdae qaaaaa@41FE@ , estimated in Section 4.5. In principle they should correspond to the MRs, but in practice they could include a variety of other importer/exporter-specific influences on bilateral trade. However, Fally (2015) observes that when Equation (4) is estimated by Poisson pseudo-maximum likelihood (PPML), estimates of the MR terms can be derived directly from the estimated fixed effects as follows:
P j −ϵ ^ = E j E 0 exp(− χ ^ j ), (8) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaqiaaWdaeaapeGaamiua8aadaqhaaWcbaWdbiaadQgaa8aabaWd biabgkHiTmrr1ngBPrwtHrhAXaqeguuDJXwAKbstHrhAG8KBLbacfa Gae8x9dipaaaGccaGLcmaacqGH9aqpdaWcaaWdaeaapeGaamyra8aa daWgaaWcbaWdbiaadQgaa8aabeaaaOqaa8qacaWGfbWdamaaBaaale aapeGaaGimaaWdaeqaaaaak8qaciGGLbGaaiiEaiaacchacaGGOaGa eyOeI0Iafq4XdmMbaKaapaWaaSbaaSqaa8qacaWGQbaapaqabaGcpe GaaiykaiaacYcaaaa@546B@
Π i −ϵ ^ = E 0 Y i exp(− π ^ i ). (9) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaqiaaWdaeaapeGaeuiOda1damaaDaaaleaapeGaamyAaaWdaeaa peGaeyOeI0Yefv3ySLgznfgDOfdaryqr1ngBPrginfgDObYtUvgaiu aacqWF1pG8aaaakiaawkWaaiabg2da9iaadweapaWaaSbaaSqaa8qa caaIWaaapaqabaGcpeGaamywa8aadaWgaaWcbaWdbiaadMgaa8aabe aak8qaciGGLbGaaiiEaiaacchacaGGOaGaeyOeI0IafqiWdaNbaKaa paWaaSbaaSqaa8qacaWGPbaapaqabaGcpeGaaiykaiaac6cacaWLja GaaCzcaiaaxMaacaGGOaGaaGyoaiaacMcaaaa@5900@
For their derivation, Equations (8) and (9) rely on the exclusion of an importer fixed effect ( χ ^ 0 = 0 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacuaHhpWygaqca8aadaWgaaWcbaWdbiaaicdaa8aabeaak8qacqGH 9aqpcaaIWaaaaa@3ACB@ ), the normalization of the corresponding IMR ( P 0 = 1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGqbWaaSbaaSqaaiaaicdaaeqaaOGaeyypa0JaaGymaaaa@399C@ ), and the fact that the sum of the outward equals the sum of the inward fixed effects. Anderson, Larch and Yotov (2018) show that using MRs recovered from the fixed effects estimated by PPML under actual and counterfactual values for trade costs produce estimates for changes in trade and welfare that are equivalent to the ‘exact hat’ results.
6.2 Trade costs, output and expenditure
The general equilibrium impact of trade costs on trade and welfare will depend on the underlying model used to derive Equation (1). To establish a lower bound for welfare estimates, this paper uses a version of the canonical Armington endowment model used in Anderson and van Wincoop (2003). In this model, each region has an endowment of its own distinct good that generates utility in a CES function that is identical across regions. Welfare changes from trade stem from producers fetching a lower or higher price for their endowment of goods, and consumers having more or less favourable access to a greater variety of goods.Note The first effect is captured by changes in producer prices, while the second is measured by the changes in the consumer price index.
With CES demand, the consumer price index is simply the inward multilateral resistance term ( P j MathType@MTEF@5@5@+= feaagKart1ev2aqaMDbvLHfij5gC1rhimfMBNvxyNvgaq9LAamXvP5 wqSXMqHnxAJn0BKvguHDwzZbqefqvATv2CG4uz3bIuV1wyUbqedmvE Tj2BSbqefm0B1jxALjhiov2DaebbnrfifHhDYfgasaacH8YjY=vipg Ylh9vqqj=hEeeu0xXdbba9frFj0=OqFfea0dXdd9vqai=hGuQ8kuc9 pgc9q8qqaq=dir=f0=yqaiVgFr0xfr=xfr=xb9adbaqaaeGaciGaai aabeqaamaabaabaaGcbaaeaaaaaaaaa8qacaWGqbWdamaaBaaaleaa peGaamOAaaWdaeqaaaaa@4045@ ). Producer prices in the Armington framework can be recovered from the aggregate CES demand for region i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGPbaaaa@3670@ ’s unique good. The demand for this good in region j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGQbaaaa@3671@ is given by
X ij = ( γ i p i t ij P j ) 1−σ E j , (10) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGybWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaak8qacqGH 9aqpdaqadaWdaeaapeWaaSaaa8aabaWdbiabeo7aN9aadaWgaaWcba WdbiaadMgaa8aabeaak8qacaWGWbWdamaaBaaaleaapeGaamyAaaWd aeqaaOWdbiaadshapaWaaSbaaSqaa8qacaWGPbGaamOAaaWdaeqaaa GcbaWdbiaadcfapaWaaSbaaSqaa8qacaWGQbaapaqabaaaaaGcpeGa ayjkaiaawMcaa8aadaahaaWcbeqaa8qacaaIXaGaeyOeI0Iaeq4Wdm haaOGaamyra8aadaWgaaWcbaWdbiaadQgaa8aabeaak8qacaGGSaGa aCzcaiaaxMaacaWLjaGaaiikaiaaigdacaaIWaGaaiykaaaa@5255@
where the parameter γ i > 0 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqaHZoWzpaWaaSbaaSqaa8qacaWGPbaapaqabaGcpeGaeyOpa4Ja aGimaaaa@3AE1@ reflects the geographic distribution of comparative advantage and p i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiCamaaBa aaleaacaWGPbaabeaaaaa@3805@ is region i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGPbaaaa@3670@ producers’ prices. The trade elasticity in this model is − ϵ = 1 − σ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqGHsisltuuDJXwAK1uy0HwmaeHbfv3ySLgzG0uy0Hgip5wzaGqb aiab=v=aYlabg2da9iaaigdacqGHsislcqaHdpWCaaa@476D@ , or the consumers’ elasticity of substitution between regional varieties. Summing over all its consumers (including in the region itself), the market clearing condition for region i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGPbaaaa@3670@ ’s output is Y i = ∑ j X i j = ( γ i p i ) 1 − σ ∑ j ( t i j P j ) 1 − σ E j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGzbWdamaaBaaaleaapeGaamyAaaWdaeqaaOWdbiabg2da9maa qafapaqaa8qacaWGybWdamaaBaaaleaapeGaamyAaiaadQgaa8aabe aaaeaapeGaamOAaaqab0GaeyyeIuoakiabg2da9iaacIcacqaHZoWz paWaaSbaaSqaa8qacaWGPbaapaqabaGcpeGaamiCa8aadaWgaaWcba WdbiaadMgaa8aabeaak8qacaGGPaWdamaaCaaaleqabaWdbiaaigda cqGHsislcqaHdpWCaaGcdaaeqbWdaeaapeGaaiikamaalaaapaqaa8 qacaWG0bWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaaaOqaa8qa caWGqbWdamaaBaaaleaapeGaamOAaaWdaeqaaaaak8qacaGGPaWdam aaCaaaleqabaWdbiaaigdacqGHsislcqaHdpWCaaaapaqaa8qacaWG QbaabeqdcqGHris5aOGaamyra8aadaWgaaWcbaWdbiaadQgaa8aabe aaaaa@5B53@ .
Using Equation (10) and solving for producer prices yields:
p i = Y i 1 σ−1 γ i Π i . (11) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGWbWdamaaBaaaleaapeGaamyAaaWdaeqaaOWdbiabg2da9maa laaapaqaa8qacaWGzbWdamaaDaaaleaapeGaamyAaaWdaeaapeWaaS aaa8aabaWdbiaaigdaa8aabaWdbiabeo8aZjabgkHiTiaaigdaaaaa aaGcpaqaa8qacqaHZoWzpaWaaSbaaSqaa8qacaWGPbaapaqabaGcpe GaeuiOda1damaaBaaaleaapeGaamyAaaWdaeqaaaaak8qacaGGUaGa aCzcaiaaxMaacaWLjaGaaiikaiaaigdacaaIXaGaaiykaaaa@4BC6@
Arriving at general equilibrium estimates for counterfactual trade costs involves calculating how producers’ prices ( p i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiCamaaBa aaleaacaWGPbaabeaaaaa@3805@ ), output ( Y i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGzbWdamaaBaaaleaapeGaamyAaaWdaeqaaaaa@383C@ ), and expenditures ( E j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGfbWdamaaBaaaleaapeGaamOAaaWdaeqaaaaa@3829@ ) change in response to shifting market opportunities (as summarized by changes in Π i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqqHGoaupaWaaSbaaSqaa8qacaWGPbaapaqabaaaaa@38DC@ ). Note that in the endowment model, region i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGPbaaaa@3670@ ’s volume of goods remain unchanged, i.e., Y i c p i c = Y i p i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaWcaaWdaeaapeGaamywa8aadaqhaaWcbaWdbiaadMgaa8aabaWd biaadogaaaaak8aabaWdbiaadchapaWaa0baaSqaa8qacaWGPbaapa qaa8qacaWGJbaaaaaakiabg2da9maalaaapaqaa8qacaWGzbWdamaa BaaaleaapeGaamyAaaWdaeqaaaGcbaWdbiaadchapaWaaSbaaSqaa8 qacaWGPbaapaqabaaaaaaa@427F@ , where the superscript c MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGJbaaaa@366A@ denotes counterfactual values. Following the literature, the model’s counterfactuals are derived assuming constant bilateral trade balances, or E j Y j = ϕ j = E j c Y j c MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaWcaaWdaeaapeGaamyra8aadaWgaaWcbaWdbiaadQgaa8aabeaa aOqaa8qacaWGzbWdamaaBaaaleaapeGaamOAaaWdaeqaaaaak8qacq GH9aqpcqaHvpGzpaWaaSbaaSqaa8qacaWGQbaapaqabaGcpeGaeyyp a0ZaaSaaa8aabaWdbiaadweapaWaa0baaSqaa8qacaWGQbaapaqaa8 qacaWGJbaaaaGcpaqaa8qacaWGzbWdamaaDaaaleaapeGaamOAaaWd aeaapeGaam4yaaaaaaaaaa@466E@ . Finally, welfare ( W ^ j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qaceWGxbGbaKaapaWaaSbaaSqaa8qacaWGQbaapaqabaaaaa@384B@ ) implications of trade policy changes in this model can be summarized by changes in the value of region j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVCI8FfYJH8YrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfea0=yr0RYxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9 Ff0dmeaabaqaciaacaGaaeqabaWaaeaaeaaakeaacaWGQbaaaa@3671@ ’s expenditures, deflated by the region’s consumer price index:
W ^ j = E j c / P j c E j / P j . (12) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qaceWGxbGbaKaapaWaaSbaaSqaa8qacaWGQbaapaqabaGcpeGaeyyp a0ZaaSaaa8aabaWdbiaadweapaWaa0baaSqaa8qacaWGQbaapaqaa8 qacaWGJbaaaOGaai4laiaadcfapaWaa0baaSqaa8qacaWGQbaapaqa a8qacaWGJbaaaaGcpaqaa8qacaWGfbWdamaaBaaaleaapeGaamOAaa WdaeqaaOWdbiaac+cacaWGqbWdamaaBaaaleaapeGaamOAaaWdaeqa aaaak8qacaGGUaGaaCzcaiaaxMaacaWLjaGaaiikaiaaigdacaaIYa Gaaiykaaaa@4B23@
Anderson, Larch and Yotov (2018) propose an algorithm for calculating counterfactual trade, prices, output and expenditures after a policy change that exploits the MRs estimated by the fixed effects. They characterize their method as ‘estibration’, combining the advantages of PPML estimation and calibration. The algorithm consists of four steps:
Estimate fixed effects with PPML and use them to construct baseline indexes, Π ^ i k MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacuqHGoaugaqca8aadaqhaaWcbaWdbiaadMgaa8aabaWdbiaadUga aaaaaa@39ED@ , P ^ j k MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qaceWGqbGbaKaapaWaa0baaSqaa8qacaWGQbaapaqaa8qacaWGRbaa aaaa@3945@ and p i k MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGWbWdamaaDaaaleaapeGaamyAaaWdaeaapeGaam4Aaaaaaaa@3954@ according to Equations (8), (9) and (11), where the iteration counter k = 0 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGRbGaeyypa0JaaGimaaaa@38C6@ .
Impose counterfactual trade costs, T i j B c ^ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWHubWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaak8qadaqi aaWdaeaapeGaaCOqa8aadaahaaWcbeqaa8qacaWGJbaaaaGccaGLcm aaaaa@3C2E@ , re-estimate Equation (5) and use the fixed effects to calculate “conditional” general equilibrium (GE) indexes, Π ^ i k + 1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacuqHGoaugaqca8aadaqhaaWcbaWdbiaadMgaa8aabaWdbiaadUga cqGHRaWkcaaIXaaaaaaa@3B8A@ , P ^ j k + 1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qaceWGqbGbaKaapaWaa0baaSqaa8qacaWGQbaapaqaa8qacaWGRbGa ey4kaSIaaGymaaaaaaa@3AE2@ and p ^ i k + 1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qaceWGWbGbaKaapaWaa0baaSqaa8qacaWGPbaapaqaa8qacaWGRbGa ey4kaSIaaGymaaaaaaa@3B01@ in the first iteration.
Use the change in producer prices ( p ^ i k + 1 p ^ i k = [ exp ( π ^ i k + 1 ) exp ( π ^ i k ) ] 1 1 − σ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaWcaaWdaeaapeGabmiCayaajaWdamaaDaaaleaapeGaamyAaaWd aeaapeGaam4AaiabgUcaRiaaigdaaaaak8aabaWdbiqadchagaqca8 aadaqhaaWcbaWdbiaadMgaa8aabaWdbiaadUgaaaaaaOGaeyypa0Ja ai4wamaalaaapaqaa8qaciGGLbGaaiiEaiaacchacaGGOaGafqiWda NbaKaapaWaa0baaSqaa8qacaWGPbaapaqaa8qacaWGRbGaey4kaSIa aGymaaaakiaacMcaa8aabaWdbiGacwgacaGG4bGaaiiCaiaacIcacu aHapaCgaqca8aadaqhaaWcbaWdbiaadMgaa8aabaWdbiaadUgaaaGc caGGPaaaaiaac2fapaWaaWbaaSqabeaapeWaaSaaa8aabaWdbiaaig daa8aabaWdbiaaigdacqGHsislcqaHdpWCaaaaaaaa@58CA@ ) and MRs to update the values of bilateral trade flows according to:
X ij ^ k+1 = ( t ij 1−σ ) ^ c t ij 1−σ ^ Y i ^ k+1 E j ^ k+1 Y ^ i k E ^ j k ( Π i 1−σ ^ ) k ( P j 1−σ ^ ) k ( Π i 1−σ ^ ) k+1 ( P j 1−σ ^ ) k+1 X ij ^ k . (13) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaqiaaWdaeaapeGaamiwa8aadaWgaaWcbaWdbiaadMgacaWGQbaa paqabaaak8qacaGLcmaapaWaaWbaaSqabeaapeGaam4AaiabgUcaRi aaigdaaaGccqGH9aqpdaWcaaWdaeaapeGaaiikamaaHaaapaqaa8qa caWG0bWdamaaDaaaleaapeGaamyAaiaadQgaa8aabaWdbiaaigdacq GHsislcqaHdpWCaaGccaGGPaaacaGLcmaapaWaaWbaaSqabeaapeGa am4yaaaaaOWdaeaapeWaaecaa8aabaWdbiaadshapaWaa0baaSqaa8 qacaWGPbGaamOAaaWdaeaapeGaaGymaiabgkHiTiabeo8aZbaaaOGa ayPadaaaamaalaaapaqaa8qadaqiaaWdaeaapeGaamywa8aadaWgaa WcbaWdbiaadMgaa8aabeaaaOWdbiaawkWaa8aadaahaaWcbeqaa8qa caWGRbGaey4kaSIaaGymaaaakmaaHaaapaqaa8qacaWGfbWdamaaBa aaleaapeGaamOAaaWdaeqaaaGcpeGaayPadaWdamaaCaaaleqabaWd biaadUgacqGHRaWkcaaIXaaaaaGcpaqaa8qaceWGzbGbaKaapaWaa0 baaSqaa8qacaWGPbaapaqaa8qacaWGRbaaaOGabmyrayaajaWdamaa DaaaleaapeGaamOAaaWdaeaapeGaam4AaaaaaaGcdaWcaaWdaeaape GaaiikamaaHaaapaqaa8qacqqHGoaupaWaa0baaSqaa8qacaWGPbaa paqaa8qacaaIXaGaeyOeI0Iaeq4WdmhaaaGccaGLcmaacaGGPaWdam aaCaaaleqabaWdbiaadUgaaaGccaGGOaWaaecaa8aabaWdbiaadcfa paWaa0baaSqaa8qacaWGQbaapaqaa8qacaaIXaGaeyOeI0Iaeq4Wdm haaaGccaGLcmaacaGGPaWdamaaCaaaleqabaWdbiaadUgaaaaak8aa baWdbiaacIcadaqiaaWdaeaapeGaeuiOda1damaaDaaaleaapeGaam yAaaWdaeaapeGaaGymaiabgkHiTiabeo8aZbaaaOGaayPadaGaaiyk a8aadaahaaWcbeqaa8qacaWGRbGaey4kaSIaaGymaaaakiaacIcada qiaaWdaeaapeGaamiua8aadaqhaaWcbaWdbiaadQgaa8aabaWdbiaa igdacqGHsislcqaHdpWCaaaakiaawkWaaiaacMcapaWaaWbaaSqabe aapeGaam4AaiabgUcaRiaaigdaaaaaaOWaaecaa8aabaWdbiaadIfa paWaaSbaaSqaa8qacaWGPbGaamOAaaWdaeqaaaGcpeGaayPadaWdam aaCaaaleqabaWdbiaadUgaaaGccaGGUaGaaCzcaiaaxMaacaWLjaGa aiikaiaaigdacaaIZaGaaiykaaaa@96F9@
Note that all the ratios to the right of the trade cost terms can be expressed in terms of changes in fixed effects.
Using X i j ^ k + 1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaqiaaWdaeaapeGaamiwa8aadaWgaaWcbaWdbiaadMgacaWGQbaa paqabaaak8qacaGLcmaapaWaaWbaaSqabeaapeGaam4AaiabgUcaRi aaigdaaaaaaa@3CFE@ , re-estimate the fixed effects. Iterate this estimation for k = 1 , … , K MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGRbGaeyypa0JaaGymaiaacYcacqGHMacVcaGGSaGaam4saaaa @3C85@ substituting the appropriate k-indexed terms into Equation (13) for each iteration until all regions’ producer prices change by less than some predetermined tolerance level, or Δ p i k + 1 < z MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqqHuoarcaWGWbWdamaaDaaaleaapeGaamyAaaWdaeaapeGaam4A aiabgUcaRiaaigdaaaGccqGH8aapcaWG6baaaa@3E64@ for all i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGPbaaaa@3704@ .
The first step, computing estimates of the multilateral resistances, is achieved in this paper by using the fixed effect estimates from Section 3 along with the predicted expenditures/output, in Equations (8) and (9). The second step involves generating counterfactual trade costs. The assumptions involved in generating our counterfactual scenarios (one in which the border is removed, and another where a revised Canada-United States trade agreement is sun-setted without replacement) are discussed in section 6.3.
6.3 Counterfactual scenarios: an illustration
To illustrate the ‘estibration’ methodology described above, we consider two scenarios for changing border costs. The first considers a world in which the cost of trading between Canada and the United States is assumed to be equivalent to trading across provincial borders. This amounts to reducing the estimated Canada-United States border effect from a 30% to a 10% tariff equivalent. The second scenario is one in which Canada and the United States withdraw altogether from a preferential trading agreement. In this case, tariffs would return to their Most-Favoured Nation (MFN) levels as the bilateral trading relationship would be governed by World Trade Organization rules, plus any additional non-tariff trade costs, such as heightened trade policy uncertainty for exporters, who face a less predictable trading environment. We use an approximation of the effect NAFTA had on reducing trade costs between the two countries beyond the explicit reduction in tariffs. This amounts to increasing trade costs by six percentage points to 36%.Note
Aggregate general equilibrium impacts are presented in Table 5. The effect of changing border costs is significant; a reduction increases trade from Canada to the United States by 82%, and from the United States to Canada by almost 72%. This comes at the expense of internal trade in Canada, both inter- or intra-provincial, falling by about half. The much larger United States economy, however, gets a boost in domestic trade. Welfare (total expenditures on domestic and imported goods) increases in both Canada (11.4%) and the United States (0.8%).
On the other hand, an increase in border costs reduces trade from Canada to the United States by almost a quarter, and from United States to Canada by 18%. There is a substitution towards internal trade in Canada, which rises by around 10%. Domestic trade in the United States rises slightly as well, by around 1%. Overall welfare declines by almost 2% in Canada and -0.2% in the United States.
General equilibrium impacts of changing Canada-United States trade costs on exports and expenditures, 2012
This table displays the results of General equilibrium impacts of changing Canada-United States trade costs on exports and expenditures Cross-border
exports, Domestic
Canadian exports, Domestic
United States exports, Total
expenditures, Canada to United States, United States to Canada, Inter-provincial, Intra-provincial, Inter-state, Intra-state, Canada and United States, calculated using percent change units of measure (appearing as column headers).
expendituresTable 5 Note 1
Reduction in border costs
82.2 71.6 -52.0 -46.1 8.9 10.3 11.4 0.8
Increase in border costs
-23.4 -18.1 11.3 9.8 1.1 0.7 -1.8 -0.2
Total expenditures are used as a proxy measure for total "welfare" gains/losses due to changes in trade costs.
Note: Trade costs are reduced from 30% to 10% in the first scenario. In the second scenario, MFN tariffs and non-tariff barriers increase trade costs from 30% to 36%.
Source: Statistics Canada, Surface Transportation File (STF) and the Bureau of Transportation Statistics, Commodity Flow Survey (CFS).
The world economy has become increasingly integrated since the Second World War. It has been knit together by flows of goods and services facilitated, in part, by falling trade costs associated with administrative borders. Some of these costs take the form of explicit tariffs and quotas levied on imports. Others consist of difficult-to-enumerate and quantify non-tariff barriers, which are a diverse set of frictions ranging from red tape and delay at the border to regulatory differences across jurisdictions.
Canada and the United States share one of the most important trading relationships in the world. Over the past thirty years, this relationship has developed under the auspices of an agreement that ultimately became NAFTA. The uncertainty generated by the 2018 renegotiation of that agreement has highlighted the need to understand the impact of a changing Canada-United States border on firms and consumers within the two countries. This paper uses the gravity model framework on data from a combination of Canada’s Surface Transportation File and the United States’ 2012 Commodity Flow Survey to quantify indirectly the cost of the border on bilateral trade. It also shows how to use these results in combination with the GEPPML methodology to generate general equilibrium estimates of cross-border and domestic trade and welfare resulting from changing border costs.
Appendix Table 1 presents the full set of estimates of Equation (4) for trade measured at province/state and ER levels of aggregation. The province-state level regressions constrain the effect of distance to be the same below 150 kilometres. As Table 1 in section 3.3 shows, most of these flows are still intra-province/state and so costs imposed by distances 0 to 150 kilometres is the minimum distance at the province/state regressions level of aggregation. On the other hand, the ER level regressions allow for a more detailed specification at shorter distances. The lowest distances, ranging from 0 to 50 kilometres correspond to the network length travelled exclusively by goods within ERs; the 50 to 150 kilometre range captures the distance covered by flows outside the regions, but still within the United States or Canada. For network distances above 150 kilometres, the effect of distance is allows to vary by distance class and trade type.
The spline captures the non-linearity of trade costs, at least for Canada and Canada-United States flows. These flows are captured in more detail by the STF portion of the data than is available for United States flows through the CFS. For the within Canada flows, the effect of distance is initially high, dropping over the 50 to 500 kilometres range, before rising above one in absolute value for distances up to 1,000 kilometres. The effect of distance for all flows is roughly comparable for all three types of flows over the middle distances. But for flows longer than 2,000 kilometres, the cost of distance drops for Canada and United States flows and is actually positive for United States flows. By contrast, the impact of distance for Canada-United States flows stays consistently high for all levels of the spline.
The drop in trade costs at longer distances is most likely due to how the Alchian-Allen effect manifests in models using iceberg transportation costs. Goods that are worth shipping very long distances are typically of much higher value than shorter distance flows, creating the impression that less “ice is melting” over these distances. It does not seem to be the case for Canada-United States flows, however. The source of the discrepancy is between long distance trade costs for intra- versus international flows. This pattern is consistent with higher transport rates over these longer distances resulting from a lack of cabotage rights for Canadian trucking firms. It is, however, beyond the scope of this paper to identify this effect.
Province-State and Economic Region Regressions with Spline Distances
This table displays the results of Province-State and Economic Region Regressions with Spline Distances Province-State and Economic Region (appearing as column headers).
-1.435Note ** -1.555Note ** -1.434Note ** -1.568Note **
0.37 0.531 0.243 0.187
Note ...: not applicable Note ...: not applicable -0.785Note ** -0.576Note **
Note ...: not applicable Note ...: not applicable 0.127 0.126
Note ...: not applicable Note ...: not applicable -0.301Note ** -0.387Note **
Note ...: not applicable Note ...: not applicable 0.048 0.049
Note ...: not applicable Note ...: not applicable 0.184 -0.904Note **
Note ...: not applicable Note ...: not applicable 0.403 0.109
Canada 50-150 km
Note ...: not applicable Note ...: not applicable -0.079 -0.239
Note ...: not applicable Note ...: not applicable 0.256 -0.179
United States 50-150 km
Note ...: not applicable Note ...: not applicable -1.009Note ** -0.866Note **
Note ...: not applicable Note ...: not applicable 0.151 0.064
-1.24Note ** -1.207Note * Note ...: not applicable Note ...: not applicable
0.072 0.509 Note ...: not applicable Note ...: not applicable
Canada 150-500 km
-0.972Note ** -1.979Note ** -0.138 -0.393Note *
0.216 0.576 0.14 0.179
United States 150-500 km
-1.202Note ** -0.986Note ** -1.205Note ** -1.249Note **
0.058 0.078 0.054 0.054
Canada-United States 150-500 km
-0.56 -0.839Note * -0.999Note ** -0.95Note **
0.371 0.393 0.201 0.192
Canada 500-1,000 km
-1.831Note ** -0.329 -1.099Note ** -1.221Note **
0.527 0.365 0.329 0.326
United States 500-1,000 km
-1.416Note ** -1.529Note ** -1.426Note ** -1.333Note **
0.076 0.069 0.054 0.06
Canada-United States 500-1,000 km
-0.885Note ** -0.765Note ** -0.94Note ** -1.033Note **
0.272 0.256 0.203 0.213
Canada 1,000-3,000 km
-0.301 -1.313Note ** -0.948Note ** -0.872Note **
0.446 0.295 0.332 0.336
United States 1000-3000 km
-1.241Note ** -1.168Note ** -1.118Note ** -1.168Note **
0.076 0.067 0.053 0.064
Canada-United States 1,000-3,000 km
-1.224Note ** -0.983Note ** -1.181Note ** -1.134Note **
0.202 0.191 0.142 0.15
Canada 3,000 km+
-0.678Note ** -0.371Appendix Table Note † -0.503Note * -0.529Note *
0.231 0.218 0.232 0.259
United States 3,000 km+
-0.062 -0.38Note ** -0.215Note ** 0.026
0.104 0.087 0.067 0.081
Canada-United States 3,000 km+
-1.057Note ** -1.156Note ** -1.031Note ** -1.02Note **
0.176 0.157 0.117 0.124
3,364 3,306 40,200 40,401
Notes: All models utilize a Poisson-PML estimator and include fixed effects for origins and destinations. The model also allows for the non-linear effect of distance on trade flows and for this effect above a minimum distance level d to vary by trade type, within Canada, Canada-United States and within the United States.
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Negotiations began in August 2017 and the Canada-United States-Mexico Agreement, or CUSMA, was signed on October 1, 2018. It has not been ratified by any of the three parties at time of writing.
Note that the Anderson, Larch and Yotov (2018) method can be used to examine regional variation in the impact of changing border costs. These results are presented in detail in Brown, Dar-Brodeur and Dixon (2019).
Head and Mayer (2014) discuss the conditions necessary for applying the “structural” moniker to empirical gravity models. See Head and Mayer (2014) and Costinot and Rodriguez-Clare (2013) for an overview of a number of these models.
The trade cost elasticity is given by ϵ ≡ − ∂ ln X i j ∂ ln t i j > 0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=xjYJH8sqFD0xXdHaVhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaamrr1ngBPrwtHr hAXaqeguuDJXwAKbstHrhAG8KBLbacfaaeaaaaaaaaa8qacqWF1pG8 cqGHHjIUcqGHsisldaWcaaWdaeaapeGaeyOaIyRaciiBaiaac6gaca WGybWdamaaBaaaleaapeGaamyAaiaadQgaa8aabeaaaOqaa8qacqGH ciITciGGSbGaaiOBaiaadshapaWaaSbaaSqaa8qacaWGPbGaamOAaa Wdaeqaaaaak8qacqGH+aGpcaaIWaaaaa@5607@ .
Note that Π i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=xjYJH8sqFD0xXdHaVhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape GaeuiOda1damaaBaaaleaapeGaamyAaaWdaeqaaaaa@3B21@ and P j MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=xjYJH8sqFD0xXdHaVhbbf9v8qqaqFr0xc9pk0xbb a9q8WqFfeaY=biLkVcLq=JHqpepeea0=as0Fb9pgeaYRXxe9vr0=vr 0=vqpWqaaeaabiGaciaacaqabeaadaqaaqaaaOqaaabaaaaaaaaape Gaamiua8aadaWgaaWcbaWdbiaadQgaa8aabeaaaaa@3A79@ can only be solved up to a scalar: if Π ^ i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacuqHGoaugaqca8aadaWgaaWcbaWdbiaadMgaa8aabeaaaaa@3AFF@ and P ^ j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qaceWGqbGbaKaapaWaaSbaaSqaa8qacaWGQbaapaqabaaaaa@3A57@ are solutions to Equations (2) and (3), then so are λ Π ^ i MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqaH7oaBcuqHGoaugaqca8aadaWgaaWcbaWdbiaadMgaa8aabeaa aaa@3CB3@ and P ^ j λ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qadaWcaaWdaeaapeGabmiuayaajaWdamaaBaaaleaapeGaamOAaaWd aeqaaaGcbaWdbiabeU7aSbaaaaa@3C54@ . A unique solution requires choosing a base region (for which i = 0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyAaiabg2 da9iaaicdaaaa@3AB8@ , j = 0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOAaiabg2 da9iaaicdaaaa@3AB9@ when i = j MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGPbGaeyypa0JaamOAaaaa@3B0C@ ) and setting either Π 0 = 1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacqqHGoaupaWaaSbaaSqaa8qacaaIWaaapaqabaGcpeGaeyypa0Ja aGymaaaa@3C96@ or P 0 = 1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8 qacaWGqbWdamaaBaaaleaapeGaaGimaaWdaeqaaOWdbiabg2da9iaa igdaaaa@3BED@ .
The supply-use tables report international exports and imports by commodity across provinces without country detail. Hence, United States trade flows need to be estimated. This is accomplished by calculating the United States share of imports/exports by commodity and province using international trade data (adjusted from a customs to a balance of payments basis for consistency with the supply-use tables). The Atlantic Provinces (Newfoundland and Labrador, Nova Scotia, Prince Edward Island and New Brunswick) are aggregated into one region, because imports are reported by province of clearance, which would inflate New Brunswick’s imports from the United States These shares are multiplied by supply-use table-based provincial international exports and imports by detailed commodity and year to generate provincial United States trade flows. In turn, shipment-level weights on the STF are set to ensure United States exports/imports add to these benchmark totals. The sub-national United States pattern of cross border trade (i.e., the United States origin/destination of cross-border shipments) is determined by the reported origins and destination from the truck and rail shipping records.
For more details regarding the construction of the STF, please see Bemrose, Brown and Tweedle (2017).
The public-use microdata file has over 4.5 million shipments from approximately 60,000 responding establishments.
Hawaii and Alaska are excluded, because their trade is dominated by the marine and air modes and so are not consistent with the truck and rail dominated continental trading system. Following Coughlin and Novy (2016), the District of Columbia is also excluded, because of data quality concerns.
The exception is resources, where shipments are more likely to be from rural parts of states.
The effect of the definition of spatial units on empirical is often referred to as the Modifiable Areal Unit Problem (MAUP).
The median area of MAs and ERs are 22,460 km and 18,769 km, respectively. The average area of ERs at 81,535 km is larger than MA/non-MAs at 60,974 km, which reflects the very large areas of some northern ERs in Canada that have no equivalent in the United States.
There are some origin/destination pairs that have zero flows in at least one direction. In these instances, network distances were imputed using flows in the reverse direction. Where there were no flows in either direction, the network distance was imputed using predicted values from a regression of network distances on the great circle distance between the population weighted centroids of each region.
With panel data, the fixed effects should be time-varying.
It will not fully capture trade policy-driven differences that induce distance-related costs on either side of the border. An important source of these trade frictions are cabotage rights that are not extended to Canadian carriers in the United States, but which may increase the transport rates on long distance round trips, because the deadheading portion of the backhaul will likely be higher than domestic shipments. In our model, these costs are absorbed by the differing distance parameters across trade types.
Hillberry and Hummels (2008), for instance, included squared distance terms in their formulations of distance and find that these terms are significant.
Gravity regressions often include contiguity variable for adjacent regions to allow for the fact that goods travelling across borders are often attributed in the data to areas around their border crossings, as opposed to their final destination. The “contiguity effect” is likely to be particularly prominent at the international border. It is accommodated in our estimation by allowing the trade cost elasticity of distance to vary across trade types, including international trade, along the spline.
See SST’s log of gravity page for details (http://personal.lse.ac.uk/tenreyro/LGW.html).
The only major difference between the regression is at the 0 − 50 kilometres level. Since this distance covers internal flows exclusively, the difference is unsurprising.
For instance, the Economic and Social Commission for Asia and the Pacific and the World Bank estimates Canada-United States border costs in 2012 to be equivalent of a 31% tariff.
These estimates are not strictly comparable, because in Bemrose, Brown and Tweedle (2017) the estimates are based on a specification where the effect of distance is constrained.
One possibility to explain the declining effect of distance on the value of trade on domestic flows are Alchian-Allen effects. Alchian and Allen (1977) observe that high value goods tend to travel longer distances, so that the increasing value offsets the effect of transport costs between very distant locations. The fact that patterns of Canada-United States trade at long distances do not mirror their domestic counterparts may reflect the fact that Canadian truckers lack cabotage rights in the United States, increasing the costs of trade.
Costinot and Rodriguez-Clare (2014) show, using exact hat algebra, models incorporating a more sophisticated production side exhibit more pronounced welfare effects than the simple endowment model.
See Brown, Dar-Brodeur and Dixon (2019) for a description of these scenarios and more detailed results.