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text:
Sun, 23 Oct 2016 23:49:55 GMT
16.3: A Cubic Equation of State
Chem 476: Physical Chemistry II (Levinger)
16: The Properties of Gases
Isotherms
Isotherms are plots of the pressure of a gas as a function of volume at a fixed constant temperature. The isotherms for an ideal gas are hypberbolas
\[P=\dfrac{RT}{\bar{V}}\]
where \(\bar{V}\) is the molar volume \(V/n\). We know that at sufficiently low temperatures, any real gas, when compressed, must undergo a transition from gas to liquid. The signature of such a transition is a discontinuous change in the volume, signifying the condensation of the gas into a liquid that occupies a significantly lower volume.
Figure \(\PageIndex{1}\): Ideal gas isotherms for one mole of the gas and at select temperatures. Image used with permission (public domain).
The isotherms for the van der Waals Equation of state are shown in Figure \(\PageIndex{2}\). At sufficiently high temperature, the isotherms approach those of an ideal gas. However, we also see something strange in some of the isotherms. Specifically, we see a region in which \(P\) and \(V\) increase together, and we know that this cannot actually happen in a real gas. It should be clear that many approximations and assumptions go into the derivation of the van der Waals equation so that some of the important physics is missing from the model. Hence, we should not be surprised if the van der Waals equation has some unphysical behavior buried in it.
Figure \(\PageIndex{2}\): Different isotherms (curves of constant temperature) of the van der Waals equation of state using parameters \(a\) and \(b\) computed for carbon dioxide. The dashed line from A to B is drawn in accordance with Maxwell's equal area rule. The carbon dioxide molecule (CO2) has pC = 7.37 MPa and TC = 304.1 K = 31 ˚C , which gives a = 0.366 m6 Pa and b = 42.9 10-6 m3. The critical pressure is at 73.7 bar = 7370 kPa.
For large volumes, the pressures are low and the fluid obeys approximately the ideal gas law \(pV = nRT\) for all temperatures shown. If we decrease the volume (go to the left in the figure along an isotherm), the pressure rises. Consider the (blue) isotherm of 10 0C, which is below the critical temperature. Decrease the volume until we reach the point B, where condensation (formation of liquid CO2) starts. At this point the van der Waals curve is no longer physical (excluding the possibility of the occurrence of an oversaturated, metastable gas), because in reality from B to the left (to smaller volume), the pressure stays constant—equal to the vapor pressure of the liquid. The real physical behavior is given by the dashed blue line of gas-liquid coexistence.
Unfortunately, the van der Waals equation does not correctly predict the gas-liquid coexistence behavior, and hence, it must be added in ad hoc. This is done by drawing a horizontal line through the isotherm (Figure \(\PageIndex{2}\)). The vertical position of the line is chosen so that the area above the line (between the line and the isotherm) and below the line (again between the line and the isotherm) is exactly the same. In this way, we entirely remove the artifact of the unphysical increase of \(P\) with \(V\) when we compute the compressional work on the gas from \(\int P(V) \: dV\), to be discussed in our section on thermodynamics. This horizontal line is called the tie line.
The areas, bounded by the 10 °C isotherm (blue curve), below and above the coexistence line are equal. This is the content of Maxwell's equal-area rule. Decreasing the volume further, we end at point A where all molecules are now in the liquid phase, no molecules are remaining in the gas phase. When the volume is diminished of a vessel that contains only liquid, the pressure rises steeply, because the compressibility of a liquid is considerable smaller than that of a gas.
If one follows the (green) 31 °C curve of critical temperature, one meets a horizontal point of inflection (first and second derivatives of p with respect to V are zero). Note that the figure exhibits two isotherms of temperature higher than the critical temperature, if they are followed no liquid-gas phase transition will be seen; the higher pressure fluid will resemble a liquid, while at lower pressures the fluid will be more gas-like. At temperatures higher than the critical temperature no gas-liquid interface appears any longer. Although the maxima and minima in the van der Waals curves below the critical point are not physical, the equation for these curves, derived by van der Waals in 1873, was a great scientific achievement.
Even today it is not possible to give a single equation that describes correctly the gas-liquid phase transition.
As it happens, there is exactly one isotherm along which the van der Waals equation correctly predicts the gas-to-liquid phase transition. Along this isotherm, the volume discontinuity captured by the tie line is shrunken down to a single point (so that there is no possibility of an increase of \(P\) with \(V\)!). This isotherm, in fact, corresponds to the highest possible temperature at which such a transition can occur. As we approach this isotherm from higher temperatures, this isotherm is a kind of dividing line between the system's remaining a gas at all value of \(P\) and \(V\) and the system's actually undergoing a gas-to-liquid transition. Hence, this isotherm is called the critical isotherm ( the green curve in Figure \(\PageIndex{2}\)): The temperature of this isotherm is called the critical temperature, denoted \(T_c\). The point at which the curve flattens out, signifying the phase transition, is called the critical point. If we draw a curve through the isotherms joining all points of these isotherms at which the tie lines begin, continue the curve up to the critical isotherm, and down the other side where the tie lines end, this curve reaches a maximum at the critical point. This is illustrated below:
The shape of the critical isotherm at the critical point allows us to determine the exact temperature, pressure, and volume at which the phase transition from gas to liquid will occur. At this point, the isotherm is both horizontal and flat. This means that both the first and second derivatives of \(P\) with respect to \(V\) must vanish:
\[\dfrac{\partial P}{\partial V} = 0, \: \: \: \dfrac{\partial^2 P}{\partial V^2} = 0 \label{\(\PageIndex{9}\)}\]
Substituting the van der Waals equation into these two conditions, we find the following:
\[\begin{align} -\dfrac{nRT}{\left( V - nb \right)^2} + \dfrac{2 an^2}{V^3} &= 0 \\ \dfrac{2nRT}{\left( V - nb \right)^3} - \dfrac{6an^2}{V^4} &= 0 \end{align} \label{\(\PageIndex{1}\)0}\]
Hence, we have two equations in two unknowns \(V\) and \(T\) for the critical temperature and critical volume. Once these are determined, the van der Waals equation, itself, allows us to determine the critical pressure.
To solve the equations, first divide one by the other. This gives us a simple condition for the volume:
\[\begin{align} \dfrac{V - nb}{2} &= \dfrac{V}{3} \\ 3V - 3nb &= 2V \\ V &= 3nb \equiv V_c \end{align} \label{\(\PageIndex{1}\)1}\]
This is the critical volume. Now use either of the two conditions to obtain the critical temperature \(T_c\). If we use the first one, we find
\[\begin{align} \dfrac{nRT_c}{\left( V_c - nb \right)^2} &= \dfrac{2an^2}{V_c^3} \\ \dfrac{nRT_c}{\left( 3nb - nb \right)^2} &= \dfrac{2an^2}{\left( 3nb \right)^3} \\ \dfrac{nRT_c}{4n^2b^2} &= \dfrac{2an^2}{27n^3b^3} \\ RT_c &= \dfrac{8a}{27b} \end{align} \label{\(\PageIndex{1}\)2}\]
Finally, plugging the critical temperature and volume into the van der Waals equation, we obtain the critical pressure as
\[\begin{align} P &= \dfrac{nRT_c}{V_c - nb} - \dfrac{an^2}{V_c^2} \\ &= \dfrac{8an/27b}{3nb - nb} - \dfrac{an^2}{\left( 3nb \right)^2} \\ &= \dfrac{a}{27b^2} \end{align} \label{\(\PageIndex{1}\)3}\]
It comes as no surprise that cubic equations of state like the van der Waals (and Redlich-Kwong) equations yield three different roots for volume and compressibility factor. This is simply because they are algebraic equations, and any nth order algebraic equation will always yield "n" roots. However, those "n" roots are not required to be distinct, and that is not all: they are not required be real numbers, either. A quadratic expression (n = 2) may have zero real roots (e.g., \(x^2 + 1 = 0\)); this is because those roots are complex numbers. In the case of cubic expressions (n = 3), we will either have one or three real roots; this is because complex roots always show up in pairs (i.e., once you have a complex root, its conjugate must also be a solution). In our case, and because we are dealing with physical quantities (densities, volumes, compressibility factors), only real roots are of interest. More specifically, we look for real, positive roots such that \(\bar{V} > b\) in the case of molar volume and \( Z > Pb/RT} in the case of compressibility factor.
In a cubic equation of state, the possibility of three real roots is restricted to the case of sub-critical conditions (\(T < T_c\)), because the S-shaped behavior, which represents the vapor-liquid transition, takes place only at temperatures below critical. This restriction is mathematically imposed by the criticality conditions. Anywhere else, beyond the S-shaped curve, we will only get one real root of the type \(\bar{V} > b\). Figure \(\PageIndex{3}\) illustrates this point.
Figure \(\PageIndex{3}\): Multiple Roots in Cubic EOS
Let us examine the three cases presented in Figure \(\PageIndex{3}\):
Supercritical isotherms (\(T > T_c\): At temperatures beyond critical, the cubic equation will have only one real root (the other two are imaginary complex conjugates). In this case, there is no ambiguity in the assignment of the volume root since we have single-phase conditions. The occurrence of a unique real root remains valid at any pressure: any horizontal (isobaric) line cuts the supercritical isotherm just once in Figure \(\PageIndex{3}\) .
Critical isotherm (\(T = T_c\)): At the critical point (\(P = P_c\)), vapor and liquid properties are the same. Consequently, the cubic equation predicts three real and equal roots at this special and particular point. However, for any other pressure along the critical isotherm (\(P < P_c\) or \(P > P_c\),) the cubic equation gives a unique real root with two complex conjugates.
Subcritical isotherm (\(T < T_c\)): Predictions for pressures within the pressure range for metastability (\(P_A' < P < P_B'\)) or for the saturation condition (\(P = P^{sat}\)) will always yield three real, different roots. In fact, this is the only region in Figure 10.1 where an isobar cuts the same isotherm more than once. The smallest root is taken as the specific volume of the liquid phase; the largest is the specific volume of the vapor phase; the intermediate root is not computed as it is physically meaningless. However, do not get carried away. Subcritical conditions will not always yield three real roots of the type \(\bar{nu} > b\). If the pressure is higher than the maximum of the S-shaped curve, \(P_B\), we will only have one (liquid) real root that satisfies \(\bar{nu} > b\). By the same token, pressures between \(0 < P < P_A'\) yield only one (vapor) root. In the case of \(P_A'\) being a negative number, three real roots are to be found even for very low pressures when the ideal gas law applies. This can be seen in Figure 10.1 as well. The largest root is always the correct choice for the gas phase molar volume of pure components.
Most of these considerations apply to the cubic equation of state in Z (compressibility factor). The most common graphical representation of compressibility factor is the well-known chart of Standing and Katz, where Z is plotted against pressure (Figure \(\PageIndex{4}\)). Standing and Katz presented their chart for the compressibility factor (Z) of sweet natural gases in 1942. This chart was based on experimental data. Graphical determination of properties was widespread until the advent of computers, and thus the Standing and Katz Z-chart became very popular in the natural gas industry. Typical Standing and Katz charts are given for high temperature conditions (\(T > T_c\) or \(T_r > 1\)). Figure \(\PageIndex{2}\), using a cubic equation of state for a pure gas, presents the qualitative behavior of the solution of Z versus pressure. Isotherms (T > Tc) show the typical qualitative behavior we are accustomed to seeing in the Standing and Katz chart.
Figure \(\PageIndex{4}\): Compressibility Factor versus Pressure
Michael Adewumi (The Pennsylvania State University) Vice Provost for Global Program, Professor of Petroleum and Natural Gas Engineering
Citizendium
16.2: van der Waals and Redlich-Kwong Equations
16.4: The Law of Corresponding States

redpajama_set_name: RedPajamaCommonCrawl


text:
When is "Automated Recommendations" or "Song Mix" coming to mobile?
coolguyxp
Deezer desktop and web play allow me to start a song in a "radio" style, by using the "automated recommendations" system. Similarly, Deezer for Android beta has a feature called "Song Mix", which performs a similar functionality. Unfortunately, I cannot figure out how to receive the Beta update, so I am unable to use this feature. When can we expect this in a stable release version? I expect that the "song mix" feature is perfectly stable, and it is frustrating that the desktop player has this functionality and us mobile users are left behind. It would be extremely easy to start a "song mix" in the form of "automated recommendations" once you start a song in the queue on mobile, but even having the "song mix" on the stable version will be helpful..
Jean-Baptite Vincey
Song mix is already available in Deezer labs on current Deezer Android version. Go to Settings > Deezer labs, at the bottom of the page there should be a switch to enable song mix. Then you can launch a song mix from contextual menu of a track (the 3 dots at the right of a track).
Felipe.Toral
Smash hit
Couldn't find it in Android...
Deezer Legend
Hi @Felipe.Toral
I think it's on the android beta (not the normal) which you can download and try.
I'm a "Deezerhead" (fanboy) and just love music! - Deezer Profile: - https://www.deezer.com/us/profile/832898145
Mike.Valeriano
In order to download the beta app you need to use Google plus. Which is - forgive the choice of words here - stupid.
Also there's some waiting involved. The whole thing doesn't make a lot of sense.
And the funny/sad thing is that this feature should be in the current version for a long time, it's not supposed to be an "extra". It's a trivial function that every other player out there comes with, out of the box.
This, coupled with the limit on how many songs you can favorite make this app very sub par.
Perhaps Deezer should be looking for a few developers who actually understand UX.


text:
CBH: City of Beverly Hills
What does CBH mean?
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Definition in English: City of Beverly Hills
City of Beverly Hills is a word or phrase that means CBH.
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What does CBH stand for?
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'City of Beverly Hills' can be abbreviated as CBH.
CBH: Can't Be Heard
CBH: Comic Book Heroes
CBH: Compagnie Bancaire Helvétique
CAM: Computer Address Matrix
CAM: Coronographic Apodizer Mechanism


M. Allen Cunningham founded Atelier26 Books in 2011 out of deep personal convictions as a reader and writer, and he brings a writer's sensibility to his editing and publishing practices. Cunningham released his debut novel The Green Age of Asher Witherow (Unbridled Books) at age twenty-six. Set in a coal-mining town in nineteenth-century California, The Green Age served as the inaugural title for independent publisher Unbridled Books. The novel was widely acclaimed, selected by the American Booksellers Association as a #1 Indie Next Pick, named a Finalist for the Indie Next Book of the Year Award in a shortlist with Marilynne Robinson's Gilead and Philip Roth's The Plot Against America, listed as a USA Today Novel to Watch and as a Salt Lake Tribune Best Book of the West, and dubbed a "Regional Classic" by the Mountains & Plains Booksellers Association. Foreword Reviews called The Green Age "a feat reminiscent of William Styron's Lie Down in Darkness, likewise published in the author's twenty-sixth year," adding: "not only are the stories of both novels carefully designed, but every sentence in each one is crafted with care." Pulitzer Prize winner Robert Olen Butler called The Green Age "a startling accomplishment," and Booklist said it "display[ed] a mastery that is surprising in a novelistic debut." The Green Age was published in Germany, Austria, and Switzerland by Atrium Verlag in 2005. An audio edition appeared in 2014.
Three years after the publication of The Green Age, Cunningham released Lost Son (Unbridled Books), an experimental biographical novel about Rainer Maria Rilke. The culmination of more than ten years of reading, writing, research, and travel, Lost Son is a fantasia on Rilkean themes and an exploration of the enduring conflicts between life and art. One of the most distinguished literary critics of the 20th century, Ihab Hassan, said of Lost Son that "the magic of Rilke reach[es] out from every page," and called the novel "a subtle and signal imaginative achievement, putting readers on notice: an extraordinary talent has come upon the scene." Lost Son receives in-depth consideration by scholar Zvile Gimbutas in her book-length study of artist novels, where it is the sole work by a living author discussed alongside works by James Joyce, John Updike, and Virginia Woolf. The book Truthful Fictions: Conversations with American Biographical Novelists (Bloomsbury, 2014) features an extensive interview with Cunningham about Lost Son, in the company of interviews with the likes of Russell Banks, Anita Diamant, Ron Hansen, and Joyce Carol Oates. Lost Son was listed as a Top 10 Book of 2007 in The Oregonian.
Author testimonials and more in our homemade video: "A Glimpse Inside Atelier26"
The physical elegance of all our titles is a main priority at Atelier26 Books. Since our inception, we've had the great good fortune to work with designer Nathan Shields. Nathan is an artist, mathematician, teacher, and, as the mind behind SaipanCakes.com, the famous creator of pancake portraits and motifs. His work has been featured by the Today Show, Good Morning America, Nickelodeon, PBS.org, USAToday.com, The Huffington Post, and at the White House Correspondents' Dinner. As the founder of Draw4Us, he has served clients as diverse as Nutella and the Canadian government. He lives in Port Angeles, WA with his family. Read a bit about our design process HERE and HERE.
Atelier26 publicist Diane Prokop brings more than 20 years of experience in public relations and magazine writing. She is a widely published freelance book reviewer and a well-known literary blogger and author interviewer. She also serves on the Atelier26 Advisory Board. She lives in Portland, Oregon.
Paul Martone is a writer and teacher in Portland, Oregon, and served as the executive director of Late Night Library. His short stories have been finalists for two Glimmer Train awards and the John Steinbeck Award.
Laura Stanfill is the founder and publisher of Forest Avenue Press. She serves on the PubWest Board of Directors and is a sought-after public speaker on the topic of small press publishing. Laura's professional background includes stints in public relations and freelancing for regional magazines and newspapers in Virginia, New York, and Oregon.


A popular actor and TV presenter has been arrested in a mall in Saudi Arabia after his appearance caused a huge commotion among young female fans.
Abdul Aziz al-Kassar, a Saudi national who lives in Kuwait, was on a working visit to Riyadh when he was mobbed by fans trying to take pictures and selfies with him.
Kassar had publicised his visit to the Al Nakheel shopping centre on Friday evening, asking his social media followers for recommendations of "the best mall to visit", Gulf News reported.
But in a TV interview at the weekend, he told the Gulf Rotana network he had not expected the "overwhelming" welcome he received from fans.
Video from the mall posted to YouTube and Twitter appears to show Kassar surrounded by women taking photos, before a man in white robes grabs him by the shirt and hauls him away.
Kassar told Gulf Rotana: "I did not expect to find so many people waiting for me. I want to clarify that the presence of young women at the mall was not something under my control.


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MOTOGP: Pedrosa To Retire At The End Of The Season
By Chineze Ogugua
Honda MotoGP rider, Dani Pedrosa has announced that he will retire at the end of the season after he recently lost his seat to Jorge Lorenzo.
The 32-year-old Spaniard who made his debut in 2006 has finished as championship runner-up three times this season.
Pedrosa said in a statement: "It's a hard decision because this is the sport I love. I've thought about it for a long time."
"Despite having good opportunities to keep racing, I feel like I don't live racing with the same intensity as before and I now have different priorities in my life." he added.
Pedrosa's last race will be at the Valencian GP in Spain in November.
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Co-hosted by the Poland-based Microfinance Centre (MFC) and the Belgium-based European Microfinance Network (EMN), this event's theme for 2018 is "People and the Digital Revolution: Advancing Our Social Mission through Technology." Although the agenda of conference is still in development, it will include subjects such as Capitalising on Big Data for Financial Inclusion, MFI (Microfinance Institution) Partnerships with Fintech, Innovative Risk Management Including Alternative Risk Management Tools, and Microfinance Clients' Financial Health and Ways to Measure It. The event will also include the presentation of the 11th Microfinance Research Award, offering a prize of EUR 1,000 (USD 1,157) to authors on topics such as digitalization in the microfinance sector, job creation, social entrepreneurship or social investment performance measurement.
Background on Organizer: MFC is a network of 111 MFIs operating in 36 countries that aims to promote a socially oriented and sustainable microfinance sector. Its services include knowledge management, policy advocacy, technical assistance, and research and development. As of December 2016, MFC's member MFIs serve approximately 1.5 million customers.
EMN aims to bring together microfinance practitioners and other industry stakeholders in Europe with the purpose of promoting best practices in microfinance, self-employment and microenterprise development. It also seeks to improve the regulatory framework for microfinance at the EU and member-state levels. The NGO disseminates its information via webinars, conferences, peer-to-peer visits and publications. As of 2018, EMN has 112 members and partners located in 25 European countries.


How Do You Deal With Lonliness And Boredom As A Single Sahm?
All Communities > Stay at Home Moms > How do you deal with lonliness and boredom as a single sahm?
I love spending time with my kids. I'm never bored when they're around b/c they keep me on my toes constantly. But when they're in school I get lonely and bored. I miss them so much and can't wait for them to get home. After I clean the house, plan dinner, take care of everything, lately I've been getting bored and lonely. I have a routine I follow every day and its beginning to drive me crazy. I need some excitement or a challenge in my life but I can't think of anything. Does anyone have any ideas of what I can do during the day when I'm alone and bored? Something to keep my mind occupied and me busy?
I have to agree with Jodi on this one if you are bored when your children are in school try getting a part time job. Even if it is just a couple hour a day or week it would give you something to do and give you extra money. It is great that your ex is supporting you and I commend him for that but lets be honest here, he did not get you pregnant by himself and the children are the responsibility of bth of you not just him. I am a stay at home mom and my husband has a good job that offers insurance and allows me to do so but if not I would get a job when my children enter school. When that time comes I may get a part time job any way.
I just read your other post about the child support - personally, I think you have an obligation to also be working if your children are at school. It isn't only your ex's responsibility to financially provide for the children. I could understand it if they were not school age, because childcare can get very expensive, but they are at school, you are bored, and your ex is financially supporting you all. That doesn't sound particularly fair to me.
Could you get a part time job? I imagine as a single parent, this would also help financially.


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India Gearing up To Curb Communicable Diseases
The government's 12th Plan aims to address several public health challenges to control communicable diseases
Calling communicable diseases a "major public health challenge", Union Health Minister Ghulam Nabi Azad on Wednesday said various socio-economic and environmental reasons underlie the growing burden of communicable diseases.
"Communicable diseases pose a major public health challenge for India. The country is vulnerable to emerging and re-emerging diseases because of the existing environmental, socio-economic and demographic situation," Azad said speaking at a meeting of the Health Ministry's Consultative Committee of Parliament
The minister said that while "note-worthy" success had been registered during the 11th Five Year Plan, the 12th Plan aims to address several public health challenges to control communicable diseases, reports IANS.
"The 12th Five Year Plan aims to address several public health challenges, such as ensuring primary health care to all including the urban slum population; strengthening of health care infrastructure; increasing public health workforce; strengthening disease surveillance and response systems; formulation and enforcement of appropriate public health laws and increasing public health allocation and spending," said Azad.
Several members expressed serious concerns over the increase in Japanese encephalitis cases.
According to Ministry figures, 5,149 acute encephalitis syndrome (AES) cases and 677 deaths were reported across India in 2010. Of these, there were 565 cases and 110 deaths due to Japanese encephalitis in 11 states.
The members suggested preventive programmes and a coordinated approach to tackle communicable diseases. Awareness campaigns on Doordarshan and All India Radio were also suggested along with allocation of funds for local health 'melas'.
As per Health Ministry figures, the prevalence of tuberculosis (TB) is about 266 cases per lakh people and 23 persons die because of TB.
About 1.5 million cases of malaria with 30,000 deaths annually are reported. About 40 million persons infected with filaria, one-third of global cases, live in India and about 129 million are at risk of 'kala-azar' (leishmaniasis) in 52 endemic districts mostly in Bihar, Jharkhand, West Bengal and eastern Uttar Pradesh.
Figures also show nearly 126,800 new cases of leprosy were reported in 2010 which is nearly half of global numbers, and more than 300 million episodes of acute diarrhoea occur every year in India in children below 5 years of age.
The minister said inter-sectoral coordination was important for controlling spread of communicable diseases.
iGovernment


As a new facility to offer information, Kirara café is a place where people interact each other with information. The community information and idea from all Kamakura are getting together here and people brush up the idea and improve through actions. The realization of harmonious coexistence of various people is aimed.
Small tea house. Enjoy the taste of authentic Chinese tea in home-like atmosphere.
We sell Kimono, Tenugui (Japanese face cloth), serving dishes and small articles. It is a small store close to the farmer's market with hurtful hospitality surrounded by Japanese atmosphere. Japanese sweets and tea are also available.
"Kamakura Itoko Café Wakan" is a café shop located in a place just 4 minutes on foot from Enoden Hase Station conveniently. Kannon Anmitsu is a sweet gem that you should try. There are also other menus such as an assorted fresh whitebait plate.
"Miso Shop Kamakura Inoue" is a miso shop with Café as a "place to enjoy miso with five senses" in Kamakura, the place of birth of miso soup. We will make various proposals using fermented foods such as miso for desserts and drinks as well as for lunch and dinner.
"Bergfeld Kamakura main store" is a long-established bakery founded in 1980. German bread such as wheat germ bread and rye bread made with non-additive ingredients and homemade yeast has many local fans.
Coffee specialty shop "MINIKOMU" on Komachi Street is a cafe with Showa's fragrant.
"Fiesta" is a Mexican cuisine, BURRITO (Burrito) and QUESADILLA (Kasadilla) specialty restraunt.
"Gihei" is known by it's thin skinned Manju (steamed cake filled with bean paste), which can be seen from the platform of Kitakamakura station. It is a delicious Manju with reduced sweetness.
Toshimaya famous for <Dove Sabray> has kept making Kamakura-like sweets as a narrative of Kamakura. On the first floor of the Toyoshimaya door store in front of Kamakura station, we sold the pigeon subleay and established a new baked bread corner on that side. On the second floor, we prepared a space that you can easily eat bread you bought. The third floor is a snack cafe.


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By car: From Junction 29 on the M25, continue along the A127 until the A130 junction. Turn back on yourself along the A127 and then left after the Alton Garden Centre but before the small garage (a pub is on the opposite side of the dual carriageway). Turn left into Pound Lane. Please note that Pound Lane is only accessible from the east to west lane of the A127.
By train: London (Fenchurch Street) to Pitsea/Basildon or London (Liverpool Street) to Wickford. Journey time approximately 40 minutes. Monday to Saturday trains leave every 20 minutes. Sunday trains leave every 30 minutes. Taxi ranks are situated outside the stations.
By bus: Regular bus services are run by NIBS Buses. Route 21 is the only bus that travels to the site - please see www.nibsbuses.com for timetables.
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