International Journal of Finance and Accounting
p-ISSN: 2168-4812 e-ISSN: 2168-4820
2013; 2(7): 373-378
doi:10.5923/j.ijfa.20130207.05
Mohammad Z. Hasan , Selim Akhter , Fazle Rabbi
University of Notre Dame Australia, Australia
Correspondence to: Mohammad Z. Hasan , University of Notre Dame Australia, Australia.
| Email: | ![]() |
Copyright © 2012 Scientific & Academic Publishing. All Rights Reserved.
This study estimates and compares the asymmetry and persistence of volatility of crude oil, natural gas and coal- three main sources of energy. This study also evaluates the effect of recent Global Financial Crisis (GFC) on the return and volatility of these energy prices. Threshold GARCH (TGARCH) and fractionally integrated GARCH (FIGARCH) model are employed to facilitate the study. The estimated results show that coal return volatility exhibits strong mean reversion whereas crude oil and natural gas return volatility endures shocks for relatively higher period. The estimated results also confirm that volatility of crude oil and natural gas increases after positive shocks in prices.
Keywords: Energy Price, Volatility, GARCH
Cite this paper: Mohammad Z. Hasan , Selim Akhter , Fazle Rabbi , Asymmetry and Persistence of Energy Price Volatility, International Journal of Finance and Accounting , Vol. 2 No. 7, 2013, pp. 373-378. doi: 10.5923/j.ijfa.20130207.05.
![]() | (1) |
where,
is the energy price return at time t, GFC is the dummy variable for financial crisis in 2008, t-bill is the 3 month US Treasury bill rate, and
is the error term in the mean equation at time t. Since carrying cost is one of the important components of the return function of energy commodity prices, we use carrying cost in the return function of energy price returns. In this case, we use T-bill to represent the carrying cost. Reference[16] states that the risk free rate is a significant component of this carrying cost and it can be used to represent the carrying cost. Reference[16] also uses 3 month U.S. Treasury bill rate in his study of crude oil and natural gas return volatility. The mean and variance equation are augmented by dummy variable GFC3 to identify the shift in volatility in energy prices due to the recent financial crisis. In the variance equation, the ARCH and GARCH parameters must be positive, α>0, and β>0, and the sum of
quantifies the persistence of shocks to volatility. As the return series is unexpectedly large in either the upward or downward direction, the GARCH specification captures the volatility clustering effect. ![]() | (2) |
<0; =0 otherwise.For asymmetric effect, we would see
. The condition of non-negativity is
,
,
, and
. In equation (2),
measures constant volatility,
measures the effect of lagged return shocks of energy on its volatility and
measures the effect of the previous period’s conditional volatility on the volatility of current period. The term
captures the asymmetry effect of energy return volatility. If there is a symmetric effect of lagged shocks on the volatility
is zero. In contrast, if lagged negative shocks augment the volatility by more than lagged positive shocks
, there is an asymmetric effect which is typically associated with a leverage effect or a volatility feedback effect. If lagged negative shocks decrease the volatility of energy returns
the asymmetric effect typically found for equity is inverted, i.e. positive shocks of energy return increase its volatility by more than negative shocks. For energy returns, the expectation is that positive shocks have more effect on volatility than negative shocks. Therefore, we expect negative sign in
. ![]() | (3) |
,
,
,
;
is the fractional integration parameter and L is the lag operator. The parameter
characterizes the persistence property of hyperbolic decay in volatility because it allows autocorrelations to decay at a slow hyperbolic rate. The advantage of the FIGARCH process is that for
, it is sufficiently flexible to allow for intermediate ranges of persistence. The FIGARCH model allows for long memory behaviour and a slow rate of decay after volatility shocks.
|
, is statistically significant. However, it is not statistically significant for coal and natural gas. The coefficient of the constant is negligible. The coefficient of T-bill,
, is statistically significant for all energy price returns except in TGARCH model for natural gas. This result is consistent with theory, as the return of energy prices is a function of carrying cost. In our model, T-bill rate is a proxy measure of carrying cost of energy prices. The coefficient of t-bill rate has positive coefficient suggesting when t-bill rate goes up, the returns energy returns also go up. Reference[16] also has the same results for T-bill rate in the mean equation. We have important findings for the effect of recent global financial crisis. Although the coefficients of dummy variable GFC is not statistically significant in the return function of the energy prices, GFC has effect on the volatility of energy price returns suggesting GFC contributes to the energy return volatility. The results of the variance equation show that the coefficients of the dummy variable GFC,
, are significant for all energy prices and for all GARCH class of models. In most of the cases, the coefficients of GFC are significant at 1% and at 5% level.
|
, captures persistence of shocks. When the coefficient,
, is close to 1, the shocks to volatility do not die out quickly. To measure the persistence of shocks, we estimate FIGACH (1, d, 1) model using equation (3). In the model, when fraction term is
, the volatility has long memory and underlying series is stationary and when
, the volatility does not have long memory. Our estimated results from Table 2 show that the coefficients of
are statistically significant and its value ranges from 0.2954 (gas) to 0.4607 (coal). The results imply that the volatility of energy returns exhibit long memory and any shocks to the volatility do not die out quickly. The results are confirmed by the coefficient value of
. The value of
is less than unity. Wei et al. (2010) also find the evidence of long memory in two types of oil returns. Using FIGACRH model, they estimate persistence of Brent and WTI oil return volatility and their coefficients value
range from 0.310 to 0.443. For measuring volatility persistence in energy return volatility, we also discuss about half-life, another measure persistence of volatility. The ‘half-life’ is another measure of volatility persistence. Reference[8] defines half-life as the time required for the volatility to move half way back towards its unconditional mean. The unconditional mean of the FIGARCH (1, 1) model is estimated as the ratio of the constant term (ω) in variance equation to the difference between 1 and the sum of ARCH and GARCH terms. Reference[16] measures half-life using the following equation: ![]() | (4) |
and half-life volatility measure. The second column of Table 3 contains the sum of
and
from the estimation results of equation (3) and the third column contains half-life measure of volatility. The estimation identifies that the returns volatility of energy returns exhibit long memory, since the sum of
and
is always less than one6. Among the energy prices, coal has strong mean reversion. It means that the volatility of coal approaches their average or long-run volatility relatively quickly. On the other hand, other energy prices volatility has also mean reversion; however, their volatility is relatively persistent, since the sum of
and
is close to one.
|
and
and mean reversion. As coal is relatively less persistent and its volatility moves quickly to their long-run volatility level, the half-live for coal is also relatively less. This result implies that shocks to the volatility are very transient. Crude oil return volatility exhibits the highest level of persistence. The half-life of crude oil is 67 days. It implies that any shocks to this volatility take 67 days to return half-way back without any further shocks to that volatility. On the other hand, the half life volatility of natural gas is 42 days suggesting that any shock to natural gas takes 42 days to return half way back to its volatility.
. Our estimated results show that asymmetry is evident in the volatility of crude oil and gas whereas the same is not evident in case of coal.The results of the TGARCH model estimation confirm the existence of asymmetric effect on the volatility of energy returns of crude oil, natural gas. The coefficients of ARCH and GARCH terms,
, and
, are statistically significant. It ensures that the lagged residuals and lagged conditional variance are significant in describing the conditional volatility. The sign of
is negative TGARCH model suggesting the positive shocks have higher impact on next period conditional volatility of energy return than negative shocks. This result is consistent with our expectation of positive energy price shocks have higher effect on volatility than negative price shocks. The coefficient estimates vary from -0.0029 for coal to -0.0212 for crude oil. The coefficients of asymmetry are relatively higher in oil suggesting that when energy price increases, oil return volatility is affected relatively higher than other energy commodities.
|