Description Usage Arguments Details Value References See Also Examples
View source: R/Fixed_effects.R
Fixed_Effects
estimates gravity models via
OLS and fixed effects for the countries of origin and destination.
These effects catch country specific effects.
1 2 |
y |
name (type: character) of the dependent variable in the dataset
|
dist |
name (type: character) of the distance variable in the dataset
|
fe |
vector of names (type: character) of fixed effects.
The default is set to the unilateral identifiers
|
x |
vector of names (type: character) of those bilateral variables in
the dataset |
vce_robust |
robust (type: logic) determines whether a robust
variance-covariance matrix should be used. The default is set to |
data |
name of the dataset to be used (type: character).
To estimate gravity equations, a square gravity dataset including bilateral
flows defined by the argument |
... |
additional arguments to be passed to |
To account for MR terms, Feenstra (2002) and Feenstra (2004) propose to use
importer and exporter fixed effects. Due to the use of these effects, all
unilateral influences such as GDPs can no longer be estimated.
A disadvantage of the use of Fixed_Effects
is that, when applied to
panel data, the number of country-year or country-pair fixed effects can be
too high for estimation. In addition, no comparative statistics are
possible with Fixed_Effects
as the MR terms are not estimated
explicitly. Nevertheless, Head and Mayer (2014) highlight the importance of
the use of fixed effects.
To execute the function a square gravity dataset with all pairs of
countries, ISO-codes for the country of origin and destination, a measure of
distance between the bilateral partners as well as all
information that should be considered as dependent an independent
variables is needed.
Make sure the ISO-codes are of type "character".
Missing bilateral flows as well as incomplete rows should be
excluded from the dataset.
Furthermore, flows equal to zero should be excluded as the gravity equation
is estimated in its additive form.
Country specific fixed effects are considered by incorporating
"iso_o"
and "iso_d"
in fe
.
By including country specific fixed effects, all monadic effects
are captured, including Multilateral Resistance terms.
Therefore, no other unilateral variables such as GDP can be
included as independent variables in the estimation.
Fixed_Effects
estimation can be used for both, cross-sectional as well as
panel data.
Nonetheless, the function is designed to be consistent with the
Stata code for cross-sectional data provided at the website
Gravity Equations: Workhorse, Toolkit, and Cookbook
when choosing robust estimation.
The function Fixed_Effects
was therefore tested for
For the use with panel data no tests were performed.
Therefore, it is up to the user to ensure that the functions can be applied
to panel data.
Depending on the panel dataset and the variables -
specifically the type of fixed effects -
included in the model, it may easily occur that the model is not computable.
Also, note that by including bilateral fixed effects such as country-pair
effects, the coefficients of time-invariant observables such as distance
can no longer be estimated.
Depending on the specific model, the code of the
respective function may has to be changed in order to exclude the distance
variable from the estimation.
At the very least, the user should take special
care with respect to the meaning of the estimated coefficients and variances
as well as the decision about which effects to include in the estimation.
When using panel data, the parameter and variance estimation of the models
may have to be changed accordingly.
For a comprehensive overview of gravity models for panel data
see Egger and Pfaffermayr (2003), Gomez-Herrera (2013) and Head, Mayer and
Ries (2010) as well as the references therein.
The function returns the summary of the estimated gravity model as an
lm
-object.
For more information on fixed effects as well as informaton on gravity models, theoretical foundations and suitable estimation methods in general see
Anderson, J. E. (2010) <DOI:10.3386/w16576>
Head, K. and Mayer, T. (2014) <DOI:10.1016/B978-0-444-54314-1.00003-3>
as well as
Anderson, J. E. (1979) <DOI:10.12691/wjssh-2-2-5>
Anderson, J. E. and van Wincoop, E. (2003) <DOI:10.3386/w8079>
Baier, S. L. and Bergstrand, J. H. (2009) <DOI:10.1016/j.jinteco.2008.10.004>
Baier, S. L. and Bergstrand, J. H. (2010) in Van Bergeijk, P. A., & Brakman, S. (Eds.) (2010) chapter 4 <DOI:10.1111/j.1467-9396.2011.01000.x>
Head, K., Mayer, T., & Ries, J. (2010) <DOI:10.1016/j.jinteco.2010.01.002>
Santos-Silva, J. M. C. and Tenreyro, S. (2006) <DOI:10.1162/rest.88.4.641>
and the citations therein.
See Gravity Equations: Workhorse, Toolkit, and Cookbook for gravity datasets and Stata code for estimating gravity models.
For estimating gravity equations using panel data see
Egger, P., & Pfaffermayr, M. (2003) <DOI:10.1007/s001810200146>
Gomez-Herrera, E. (2013) <DOI:10.1007/s00181-012-0576-2>
and the references therein.
1 2 3 4 5 6 7 8 9 10 | ## Not run:
data(Gravity_no_zeros)
Fixed_Effects(y="flow", dist="distw", fe=c("iso_o", "iso_d"),
x=c("rta"), vce_robust=TRUE, data=Gravity_no_zeros)
Fixed_Effects(y="flow", dist="distw", fe=c("iso_o", "iso_d"),
x=c("rta", "comcur", "contig"), vce_robust=TRUE, data=Gravity_no_zeros)
## End(Not run)
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