Re: [Samba] Joining Samba to ADS domain (win2k3)
On 4/19/06, Gerald (Jerry) Carter [EMAIL PROTECTED] wrote: This is a bug in the e2fsprogs. Is there a work-around for this bug? upgrade e2fsprogs. If you are on FC4 for example, run 'yum upgrade' Thank you, that corrected the problem. -- To unsubscribe from this list go to the following URL and read the instructions: https://lists.samba.org/mailman/listinfo/samba
Re: [Samba] Joining Samba to ADS domain (win2k3)
On 4/19/06, Gerald (Jerry) Carter [EMAIL PROTECTED] wrote: This is a bug in the e2fsprogs. Is there a work-around for this bug? Thanks, Charles -- To unsubscribe from this list go to the following URL and read the instructions: https://lists.samba.org/mailman/listinfo/samba
[Samba] Joining Samba to ADS domain (win2k3)
Hello, I am having trouble joining Samba to my ADS domain. I am using Samba 3 and krb5. I have configured and tested krb5 and know that it is functioning as it should be. I can successfully authenticate users using kinit. I've also configured winbindd. When I exicute net ads joing -U admin username and enter the proper password samba generates the following aborting the process at the end: [2006/04/18 12:02:15, 0] libads/ldap.c:ads_add_machine_acct(1414) ads_add_machine_acct: Host account for mainproxy already exists - modifying old account Using short domain name -- DOMAIN Joined 'TESTSERV' to realm 'DOMAIN' *** glibc detected *** net: free(): invalid pointer: 0x00cca7f0 *** === Backtrace: = /lib/libc.so.6[0x1da424] /lib/libc.so.6(__libc_free+0x77)[0x1da95f] /lib/libcom_err.so.2(remove_error_table+0x4b)[0x13eabb] /usr/lib/libkrb5.so.3[0xc68823] /usr/lib/libkrb5.so.3[0xc685c7] /usr/lib/libkrb5.so.3[0xcb93ba] /lib/ld-linux.so.2[0x875058] /lib/libc.so.6(exit+0xc5)[0x1a1c69] /lib/libc.so.6(__libc_start_main+0xce)[0x18bdee] net[0x59c091] === Memory map: 00111000-00123000 r-xp fd:00 3372889/lib/libnsl-2.3.5.so 00123000-00124000 r-xp 00011000 fd:00 3372889/lib/libnsl-2.3.5.so 00124000-00125000 rwxp 00012000 fd:00 3372889/lib/libnsl-2.3.5.so 00125000-00127000 rwxp 00125000 00:00 0 00127000-0013d000 r-xp fd:00 7252441 /usr/lib/libgssapi_krb5.so.2.2 0013d000-0013e000 rwxp 00016000 fd:00 7252441 /usr/lib/libgssapi_krb5.so.2.2 0013e000-0014 r-xp fd:00 3372886/lib/libcom_err.so.2.1 0014-00141000 rwxp 1000 fd:00 3372886/lib/libcom_err.so.2.1 00141000-00175000 r-xp fd:00 7252514/usr/lib/libldap- 2.2.so.7.0.16 00175000-00177000 rwxp 00033000 fd:00 7252514/usr/lib/libldap- 2.2.so.7.0.16 00177000-0029b000 r-xp fd:00 3372878/lib/libc-2.3.5.so 0029b000-0029d000 r-xp 00124000 fd:00 3372878/lib/libc-2.3.5.so 0029d000-0029f000 rwxp 00126000 fd:00 3372878/lib/libc-2.3.5.so 0029f000-002a1000 rwxp 0029f000 00:00 0 002a1000-002aa000 r-xp fd:00 3371861/lib/libnss_files-2.3.5.so 002aa000-002ab000 r-xp 8000 fd:00 3371861/lib/libnss_files-2.3.5.so 002ab000-002ac000 rwxp 9000 fd:00 3371861/lib/libnss_files-2.3.5.so 002ac000-002ae000 r-xp fd:00 7300403/usr/lib/gconv/UTF-16.so 002ae000-002b rwxp 1000 fd:00 7300403/usr/lib/gconv/UTF-16.so 002b-002b2000 r-xp fd:00 7300310/usr/lib/gconv/IBM850.so 002b2000-002b4000 rwxp 1000 fd:00 7300310/usr/lib/gconv/IBM850.so 002b4000-002b8000 r-xp fd:00 3371858/lib/libnss_dns-2.3.5.so 002b8000-002b9000 r-xp 3000 fd:00 3371858/lib/libnss_dns-2.3.5.so 002b9000-002ba000 rwxp 4000 fd:00 3371858/lib/libnss_dns-2.3.5.so 002ba000-002c3000 r-xp fd:00 3372882/lib/libgcc_s- 4.0.0-20050520.so.1 002c3000-002c4000 rwxp 9000 fd:00 3372882/lib/libgcc_s- 4.0.0-20050520.so.1 002e7000-002e9000 r-xp fd:00 7247055 /usr/lib/libkrb5support.so.0.0 002e9000-002ea000 rwxp 1000 fd:00 7247055 /usr/lib/libkrb5support.so.0.0 002ea000-003e2000 r-xp fd:00 3372887/lib/libcrypto.so.0.9.7f 003e2000-003f4000 rwxp 000f8000 fd:00 3372887/lib/libcrypto.so.0.9.7f 003f4000-003f7000 rwxp 003f4000 00:00 0 004f5000-00504000 r-xp fd:00 3372883/lib/libresolv-2.3.5.so 00504000-00505000 r-xp e000 fd:00 3372883/lib/libresolv-2.3.5.so 00505000-00506000 rwxp f000 fd:00 3372883/lib/libresolv-2.3.5.so 00506000-00508000 rwxp 00506000 00:00 0 0056b000-00778000 r-xp fd:00 7243076/usr/bin/net 00778000-00784000 rwxp 0020c000 fd:00 7243076/usr/bin/net 00784000-00794000 rwxp 00784000 00:00 0 0083-0083d000 r-xp fd:00 7243986/usr/lib/liblber- 2.2.so.7.0.16 0083d000-0083e000 rwxp c000 fd:00 7243986/usr/lib/liblber- 2.2.so.7.0.16 00867000-00881000 r-xp fd:00 3372877/lib/ld-2.3.5.so 00881000-00882000 r-xp 00019000 fd:00 3372877/lib/ld-2.3.5.so 00882000-00883000 rwxp 0001a000 fd:00 3372877/lib/ld-2.3.5.so 00a97000-00aa9000 r-xp fd:00 7243041/usr/lib/libz.so.1.2.2.2 00aa9000-00aaa000 rwxp 00011000 fd:00 7243041/usr/lib/libz.so.1.2.2.2 00b77000-00b9a000 r-xp fd:00 7252439/usr/lib/libk5crypto.so.3.0 00b9a000-00b9b000 rwxp 00023000 fd:00 7252439/usr/lib/libk5crypto.so.3.0 00c08000-00c1d000 r-xp fd:00 7246017/usr/lib/libsasl2.so.2.0.20 00c1d000-00c1e000 rwxp 00015000 fd:00 7246017/usr/lib/libsasl2.so.2.0.20 00c59000-00cc8000 r-xp fd:00 7252440/usr/liAborted I am able to retrieve a list of users (wbinfo -u) and groups (wbinfo -g) but am unable to retrieve a list of groups assigned to a particular user (wbinfo --user-groups=USERNAME). I am also unable to assign securites for my domain accounts Snippets from log files are as follows: *log.wb-DOMAIN* [2006/04/18 12:10:59, 0] lib/util_sid.c:string_to_sid(285) string_to_sid: Sid S-0-0 is
[Samba] uncertainty principle is untenable !!!
please reply to [EMAIL PROTECTED] or [EMAIL PROTECTED], thank you. UNCERTAINTY PRINCIPLE IS UNTENABLE By reanalysing the experiment of Heisenberg Gamma-Ray Microscope and one of ideal experiment from which uncertainty principle is derived , it is found that actually uncertainty principle can not be obtained from these two ideal experiments . And it is found that uncertainty principle is untenable. Key words : uncertainty principle; experiment of Heisenberg Gamma-Ray Microscope; ideal experiment Ideal Experiment 1 Experiment of Heisenberg Gamma-Ray Microscope A free electron sits directly beneath the center of the microscope's lens (see the picture below or AIP page: http://www.aip.org/history/heisenberg/p08b.htm). The circular lens forms a cone of angle 2A from the electron. The electron is then illuminated from the left by gamma rays--high energy light which has the shortest wavelength. These yield the highest resolution, for according to a principle of wave optics, the microscope can resolve (that is, see or distinguish) objects to a size of dx, which is related to and to the wavelength L of the gamma ray, by the expression: dx = L/(2sinA) (1) However, in quantum mechanics, where a light wave can act like a particle, a gamma ray striking an electron gives it a kick. At the moment the light is diffracted by the electron into the microscope lens, the electron is thrust to the right. To be observed by the microscope, the gamma ray must be scattered into any angle within the cone of angle 2A. In quantum mechanics, the gamma ray carries momentum, as if it were a particle. The total momentum p is related to the wavelength by the formula p = h / L, where h is Planck's constant. (2) In the extreme case of diffraction of the gamma ray to the right edge of the lens, the total momentum in the x direction would be the sum of the electron's momentum P'x in the x direction and the gamma ray's momentum in the x direction: P'x + (h sinA) / L', where L' is the wavelength of the deflected gamma ray. In the other extreme, the observed gamma ray recoils backward, just hitting the left edge of the lens. In this case, the total momentum in the x direction is: P''x - (h sinA) / L''. The final x momentum in each case must equal the initial x momentum, since momentum is never lost (it is conserved). Therefore, the final x momenta are equal to each other: P'x + (h sinA) / L' = P''x - (h sinA) / L'' (3) If A is small, then the wavelengths are approximately the same, L' ~ L ~ L. So we have P''x - P'x = dPx ~ 2h sinA / L (4) Since dx = L/(2 sinA), we obtain a reciprocal relationship between the minimum uncertainty in the measured position,dx, of the electron along the x axis and the uncertainty in its momentum, dPx, in the x direction: dPx ~ h / dxor dPx dx ~ h. (5) For more than minimum uncertainty, the greater than sign may added. Except for the factor of 4pi and an equal sign, this is Heisenberg's uncertainty relation for the simultaneous measurement of the position and momentum of an object . Reanalysis To be seen by the microscope, the gamma ray must be scattered into any angle within the cone of angle 2A. The microscope can resolve (that is, see or distinguish) objects to a size of dx, which is related to and to the wavelength L of the gamma ray, by the expression: dx = L/(2sinA) (1) It is the resolving limit of the microscope, and it is the uncertain quantity of the object's position. Microscope can not see the object which the size is smaller than its resolving limit dx. Therefore, to be seen by the microscope, the size of the electron must be larger than the resolving limit dx or equal to the resolving limit dx. But if the size of the electron is larger than or equal to the resolving limit dx, electron will not be in the range dx. dx can not be deemed to be the uncertain quantity of the electron's position which can be seen by microscope, dx can be deemed to be the uncertain quantity of the electron's position which can not be seen by microscope only. dx is the position's uncertain quantity of the electron which can not be seen by microscope To be seen by the microscope, the gamma ray must be scattered into any angle within the cone of angle 2A, so we can measure the momentum of the electron. dPx is the momentum's uncertain quantity of the electron which can be seen by microscope. What relates to dx is the electron which the size is smaller than the resolving limit .The electron is in the range dx, it can not be seen by the microscope, so its position is uncertain. What relates to dPx is the electron which the size is larger than or equal to the resolving limit .The electron is not in the range dx, it can be seen by the microscope, so its
[Samba] uncertainty principle is untenable !!! (new)
please reply to [EMAIL PROTECTED] or [EMAIL PROTECTED], thank you. UNCERTAINTY PRINCIPLE IS UNTENABLE By reanalysing the experiment of Heisenberg Gamma-Ray Microscope and one of ideal experiment from which uncertainty principle is derived , it is found that actually uncertainty principle can not be obtained from these two ideal experiments . And it is found that uncertainty principle is untenable. Key words : uncertainty principle; experiment of Heisenberg Gamma-Ray Microscope; ideal experiment Ideal Experiment 1 Experiment of Heisenberg Gamma-Ray Microscope A free electron sits directly beneath the center of the microscope's lens (see the picture below or AIP page: http://www.aip.org/history/heisenberg/p08b.htm). The circular lens forms a cone of angle 2A from the electron. The electron is then illuminated from the left by gamma rays--high energy light which has the shortest wavelength. These yield the highest resolution, for according to a principle of wave optics, the microscope can resolve (that is, see or distinguish) objects to a size of dx, which is related to and to the wavelength L of the gamma ray, by the expression: dx = L/(2sinA) (1) However, in quantum mechanics, where a light wave can act like a particle, a gamma ray striking an electron gives it a kick. At the moment the light is diffracted by the electron into the microscope lens, the electron is thrust to the right. To be observed by the microscope, the gamma ray must be scattered into any angle within the cone of angle 2A. In quantum mechanics, the gamma ray carries momentum, as if it were a particle. The total momentum p is related to the wavelength by the formula p = h / L, where h is Planck's constant. (2) In the extreme case of diffraction of the gamma ray to the right edge of the lens, the total momentum in the x direction would be the sum of the electron's momentum P'x in the x direction and the gamma ray's momentum in the x direction: P'x + (h sinA) / L', where L' is the wavelength of the deflected gamma ray. In the other extreme, the observed gamma ray recoils backward, just hitting the left edge of the lens. In this case, the total momentum in the x direction is: P''x - (h sinA) / L''. The final x momentum in each case must equal the initial x momentum, since momentum is never lost (it is conserved). Therefore, the final x momenta are equal to each other: P'x + (h sinA) / L' = P''x - (h sinA) / L'' (3) If A is small, then the wavelengths are approximately the same, L' ~ L ~ L. So we have P''x - P'x = dPx ~ 2h sinA / L (4) Since dx = L/(2 sinA), we obtain a reciprocal relationship between the minimum uncertainty in the measured position,dx, of the electron along the x axis and the uncertainty in its momentum, dPx, in the x direction: dPx ~ h / dxor dPx dx ~ h. (5) For more than minimum uncertainty, the greater than sign may added. Except for the factor of 4pi and an equal sign, this is Heisenberg's uncertainty relation for the simultaneous measurement of the position and momentum of an object . Reanalysis To be seen by the microscope, the gamma ray must be scattered into any angle within the cone of angle 2A. The microscope can resolve (that is, see or distinguish) objects to a size of dx, which is related to and to the wavelength L of the gamma ray, by the expression: dx = L/(2sinA) (1) It is the resolving limit of the microscope, and it is the uncertain quantity of the object's position. Microscope can not see the object which the size is smaller than its resolving limit dx. Therefore, to be seen by the microscope, the size of the electron must be larger than the resolving limit dx or equal to the resolving limit dx. But if the size of the electron is larger than or equal to the resolving limit dx, electron will not be in the range dx. dx can not be deemed to be the uncertain quantity of the electron's position which can be seen by microscope, dx can be deemed to be the uncertain quantity of the electron's position which can not be seen by microscope only. dx is the position's uncertain quantity of the electron which can not be seen by microscope To be seen by the microscope, the gamma ray must be scattered into any angle within the cone of angle 2A, so we can measure the momentum of the electron. dPx is the momentum's uncertain quantity of the electron which can be seen by microscope. What relates to dx is the electron which the size is smaller than the resolving limit .The electron is in the range dx, it can not be seen by the microscope, so its position is uncertain. What relates to dPx is the electron which the size is larger than or equal to the resolving limit .The electron is not in the range dx, it can be seen by the microscope, so its
